Author name code: choudhuri ADS astronomy entries on 2022-09-14 author:"Choudhuri, Arnab Rai" ------------------------------------------------------------------------ Title: A theoretical model of the near-surface shear layer of the Sun Authors: Jha, Bibhuti Kumar; Choudhuri, Arnab Rai Bibcode: 2021MNRAS.506.2189J Altcode: 2021arXiv210514266J; 2021MNRAS.tmp.1537J; 2021MNRAS.tmp.1557J The Sun has a near-surface shear layer (NSSL), within which the angular velocity decreases rapidly with radius. We provide an explanation of this layer based on the thermal wind balance equation. Since convective motions are not affected by solar rotation in the top layer of the convection zone, we argue that the temperature falls at the same rate at all latitudes in this layer. This makes the thermal wind term very large in this layer and the centrifugal term has also to become very large to balance it, giving rise to the NSSL. From the values of differential rotation Ω(r < rc, θ) at radii less than a radius rc, we can calculate the temperature difference ΔT(r, θ) with respect to the standard solar model at different points of the convection zone by making use of the thermal wind balance equation. Then, we again use this equation in the top layer to calculate Ω(r > rc, θ) there from ΔT(r, θ). We carry on this exercise using both an analytical expression of the differential rotation and the actual data provided by helioseismology. We find that our theoretical results of the NSSL match the observational data reasonably well for rc ≍ 0.96R, giving an estimate of the radius till which the convective motions are affected by the solar rotation. Title: Professor Govind Swarup's contribution to Indian science: the recollections of a non-radio astronomer Authors: Choudhuri, Arnab Rai Bibcode: 2021JAHH...24....3C Altcode: Professor Govind Swarup FRS, the doyen of Indian astrophysics, passed away on 7 August 2020 at 9 pm. In this short tribute to 'The Father of Indian Radio Astronomy', I want to write about him from a personal perspective, primarily in a non-radio astronomical context. Title: The meridional circulation of the Sun: Observations, theory and connections with the solar dynamo Authors: Choudhuri, Arnab Rai Bibcode: 2021SCPMA..6439601C Altcode: 2020arXiv200809347C The meridional circulation of the Sun, which is observed to be poleward at the surface, should have a return flow at some depth. Since large-scale flows like the differential rotation and the meridional circulation are driven by turbulent stresses in the convection zone, these flows are expected to remain confined within this zone. Current observational (based on helioseismology) and theoretical (based on dynamo theory) evidences point towards an equatorward return flow of the meridional circulation at the bottom of the convection zone. Assuming the mean values of various quantities averaged over turbulence to be axisymmetric, we study the large-scale flows in solar-like stars on the basis of a 2D mean field theory. Turbulent stresses in a rotating star can transport angular momentum, setting up a differential rotation. The meridional circulation arises from a slight imbalance between two terms which try to drive it in opposite directions: a thermal wind term (arising out of the higher efficiency of convective heat transport in the polar regions) and a centrifugal term (arising out of the differential rotation). To make these terms comparable, the poles of the Sun should be slightly hotter than the equator. We discuss the important role played by the meridional circulation in the flux transport dynamo model. The poloidal field generated by the Babcock-Leighton process at the surface is advected poleward, whereas the toroidal field produced at the bottom of the convection zone is advected equatorward. The fluctuations in the meridional circulation (with coherence time of about 30-40 yr) help in explaining many aspects of the irregularities in the solar cycle. Finally, we discuss how the Lorentz force of the dynamo-generated magnetic field can cause periodic variations in the large-scale flows with the solar cycle. Title: A Theoretical Estimate of the Pole-Equator Temperature Difference and a Possible Origin of the Near-Surface Shear Layer Authors: Choudhuri, Arnab Rai Bibcode: 2021SoPh..296...37C Altcode: 2020arXiv200802983C Convective motions in the deep layers of the solar convection zone are affected by rotation, making the convective heat transport latitude-dependent, but this is not the case in the top layers near the surface. We use the thermal wind balance condition in the deeper layers to estimate the pole-equator temperature difference. Surface observations of this temperature difference can be used for estimating the depth of the near-surface layer within which convection is not affected by rotation. If we require that the thermal wind balance holds in this layer also, then we have to conclude that this must be a layer of strong differential rotation and its characteristics which we derive are in broad agreement with the observational data of the near-surface shear layer. Title: M.K. Das Gupta, the first Indian radio astronomer, and his connection with the 2020 Physics Nobel Prize Authors: Choudhuri, Arnab Rai; Chatterjee, Ritaban Bibcode: 2020arXiv201201001C Altcode: Half of the 2020 Nobel Prize is awarded for discovering a super-massive black hole at the centre of our Galaxy. One of the first indications of the existence of a black hole at the centre of a galaxy was found by Jennison and Das Gupta in 1953 while carrying on a radio observation of the source Cygnus A. Mrinal Das Gupta, who was doing his PhD at Manchester University at the time of this discovery, spent the major part of his professional career at Calcutta University. We give an outline of Das Gupta's life and explain the scientific significance of his discovery. Title: Bio-inspired guidance method for a soft landing on a Near-Earth Asteroid Authors: Valenzuela Najera, R.; Everett, L.; Ortega, A. G.; Choudhuri, A.; Flores-Abad, A. Bibcode: 2020AdSpR..66.2402V Altcode: Achieving a soft landing over the surface of small celestial bodies is an essential maneuver in space to advance the status of space exploration, sample collecting and in-situ resource utilization, among other on-orbit tasks. Landing on these bodies is challenging due to the reduced-gravity and airless environment. The correct planning of execution of the trajectory to land on the surface of the body is of cumbersome importance to prevent the vehicle from bouncing up and eventually reach escape velocity. In this paper, a bio-inspired trajectory planning method to land on the surface of a Near-Earth Asteroid (NEA) with zero relative velocity is proposed. The method is based on Tau theory, which has been demonstrated to explain the way that humans and some other animals' approach to different target spots to perform tasks such as perching, landing, and grasping. We have selected the NEA Apophis asteroid as our case study due to its accessibility, and small rotational velocity and orbit condition code. Two landing scenarios are studied; one considers the case where the satellite is hovering at a low altitude; the other corresponds to a landing maneuver right after a deorbiting or breaking phase, which may cause residual initial velocity in the vehicle prior to the landing maneuver. Once the descending trajectory is obtained, a closed-loop controller is in charge of achieving trajectory tracking and calculating the continuous and on/off thrust control signals. The simulation results show that the introduced approach can achieve zero final relative velocity in both cases for different initial condition, which is a requirement for a soft landing. Besides, different kinematic behaviors can be obtained by modifying the single variable named the Tau constant. The particular advantages of the method with respect to a commonly used approach are devised and analyzed as well. Title: A New Formula for Predicting Solar Cycles Authors: Hazra, Gopal; Choudhuri, Arnab Rai Bibcode: 2019ApJ...880..113H Altcode: 2018arXiv181101363H A new formula for predicting solar cycles based on the current theoretical understanding of the solar cycle from the flux transport dynamo is presented. Two important processes—fluctuations in the Babcock-Leighton (BL) mechanism and variations in the meridional circulation (MC), which are believed to be responsible for irregularities of the solar cycle—are constrained using observational data. We take the polar field near minima of the cycle as a measure of the randomness in the BL process, and the decay rate near the minima as a consequence of the change in MC. We couple these two observationally derived quantities into a single formula to predict the amplitude of the future solar cycle. Our new formula suggests that cycle 25 would be a moderate cycle. Whether this formula for predicting the future solar cycle can be justified theoretically is also discussed using simulations from the flux transport dynamo model. Title: How the Saha Ionization Equation Was Discovered Authors: Choudhuri, Arnab Rai Bibcode: 2018arXiv181010898C Altcode: Although the Saha ionization equation is a standard topic in advanced statistical physics and most professional physicists would have some knowledge of it, the exact nature of Meghnad Saha's contributions in this subject is not widely known. Based on an analysis of Saha's original papers and other relevant papers by contemporary scientists, as well as other source materials such as letters exchanged between scientists, I discuss how Saha used the theory of thermal ionization to solve some of the most important astrophysics problems of that era. Title: Flux transport dynamo: From modelling irregularities to making predictions Authors: Choudhuri, Arnab Rai Bibcode: 2018JASTP.176....5C Altcode: 2018arXiv180808550C The flux transport dynamo, in which the poloidal magnetic field is generated by the Babcock-Leighton mechanism and the meridional circulation plays a crucial role, has emerged as an attractive model for the solar cycle. Based on theoretical calculations done with this model, we argue that the fluctuations in the Babcock-Leighton mechanism and the fluctuations in the meridional circulation are the most likely causes of the irregularities of the solar cycle. With our increased theoretical understanding of how these irregularities arise, it can be possible to predict a future solar cycle by feeding the appropriate observational data in a theoretical dynamo model. Title: Predicting a Solar Cycle Before its Onset Using a Flux Transport Dynamo Model Authors: Choudhuri, Arnab Rai Bibcode: 2018IAUS..335..177C Altcode: 2018arXiv180808543C We begin with a review of the predictions for cycle 24 before its onset. After summarizing the basics of the flux transport dynamo model, we discuss how this model had been used to make a successful prediction of cycle 24, on the assumption that the irregularities of the solar cycle arise due to the fluctuations in the Babcock-Leighton mechanism. We point out that fluctuations in the meridional circulation can be another cause of irregularities in the cycle. Title: The Sun as a Laboratory for Plasma Physics Authors: Choudhuri, Arnab Rai Bibcode: 2018arXiv180810186C Altcode: Several phenomena connected with the magnetic field of the Sun (the cool sunspots, the hot corona, solar flares, the solar wind) are collectively known as solar activity. This paper discusses how one uses the MHD equations to understand how the magnetic field of the Sun is produced by the dynamo process and then gives rise to these diverse activities, making the Sun the best laboratory for plasma physics in the limit of high magnetic Reynolds number (defined at the end of the Introduction). Title: My Life and My Journey through Solar Physics Authors: Choudhuri, Arnab Rai Bibcode: 2018arXiv180909709C Altcode: This is the talk I gave at the workshop "Solar-Stellar Magnetism: Past, Present and Future" held in Jaipur on 18 February 2018 on the occasion of my 60th year. Title: The Sun's polar magnetic field: datasets, proxies and theoretical issues Authors: Choudhuri, Arnab Rai Bibcode: 2018IAUS..340..289C Altcode: 2018arXiv181005563C The polar magnetic field of the Sun is a manifestation of certain aspects of the dynamo process and is a good precursor for predicting a sunspot cycle before its onset. Although actual synoptic measurements of this field exist only from the mid-1970s, it has now been possible to determine its evolution from the beginning of the twentieth century with the help of various proxies. The recently developed 3D kinematic dynamo model can study the build-up of the Sun's polar magnetic field more realistically than the earlier surface flux transport model. Title: Explaining the variation of the meridional circulation with the solar cycle Authors: Hazra, Gopal; Choudhuri, Arnab Rai Bibcode: 2018IAUS..340..313H Altcode: 2018arXiv180906600H The meridional circulation of the Sun is observationally found to vary with the solar cycle, becoming slower during the solar maxima. We explain this by constructing a theoretical model in which the equation of the meridional circulation (the φ component of the vorticity equation) is coupled with the equations of the flux transport dynamo model. We find that the Lorentz force of the dynamo-generated magnetic fields can slow down the meridional circulation during the solar maxima in broad conformity with the observations. Title: A theoretical model of the variation of the meridional circulation with the solar cycle Authors: Hazra, Gopal; Choudhuri, Arnab Rai Bibcode: 2017MNRAS.472.2728H Altcode: 2017arXiv170805204H Observations of the meridional circulation of the Sun, which plays a key role in the operation of the solar dynamo, indicate that its speed varies with the solar cycle, becoming faster during the solar minima and slower during the solar maxima. To explain this variation of the meridional circulation with the solar cycle, we construct a theoretical model by coupling the equation of the meridional circulation (the ϕ component of the vorticity equation within the solar convection zone) with the equations of the flux transport dynamo model. We consider the back reaction due to the Lorentz force of the dynamo-generated magnetic fields and study the perturbations produced in the meridional circulation due to it. This enables us to model the variations of the meridional circulation without developing a full theory of the meridional circulation itself. We obtain results which reproduce the observational data of solar cycle variations of the meridional circulation reasonably well. We get the best results on assuming the turbulent viscosity acting on the velocity field to be comparable to the magnetic diffusivity (i.e. on assuming the magnetic Prandtl number to be close to unity). We have to assume an appropriate bottom boundary condition to ensure that the Lorentz force cannot drive a flow in the subadiabatic layers below the bottom of the tachocline. Our results are sensitive to this bottom boundary condition. We also suggest a hypothesis on how the observed inward flow towards the active regions may be produced. Title: VizieR Online Data Catalog: Polar network index for the solar cycle studies (Priyal+, 2014) Authors: Priyal, M.; Banerjee, D.; Karak, B. B.; Munoz-Jaramillo, A.; Ravindra, B.; Choudhuri, A. R.; Singh, J. Bibcode: 2017yCat..17939004P Altcode: The spatial resolution of the Ca K spectroheliograms taken at Kodaikanal (hereafter KKL) is about 2 arcsec and the exit slit of the spectroheliograph yields a spectral window of 0.5 Å centered at the Ca-K line at 3933.67 Å. Ermoli et al. (2009ApJ...698.1000E) pointed out that the Kodaikanal archive hosts the longest homogeneous record, with fewer variations in spatial resolution. The earlier version of the 8 bit data at Kodaikanal is sufficient to study those plage area with high intensity contrast, but does not provide the required photometric accuracy to properly identify the network structures because of the small intensity contrast of these features. Therefore, we have designed and developed two digitizer units, using a 1 m labsphere with an exit port of 350 mm which provides a stable and uniform source of light with less than 1% variation from the center to the edge of the light source. The CCD camera with 4kx4k format, a pixel size of 15 u square, and a 16 bit read out, operating at temperature of -100°C, was used to digitize the images. The Ca-K network can be clearly seen because of the high spatial resolution of digitization (0.86 arcsec).

(4 data files). Title: Starspots, stellar cycles and stellar flares: Lessons from solar dynamo models Authors: Choudhuri, Arnab Rai Bibcode: 2017SCPMA..60a9601C Altcode: 2016arXiv161202544C; 2017SCPMA..6019601C In this review, we discuss whether the present solar dynamo models can be extrapolated to explain various aspects of stellar activity. We begin with a summary of the following kinds of data for solar-like stars: (i) data pertaining to stellar cycles from Ca H/K emission over many years; (ii) X-ray data indicating hot coronal activity; (iii) starspot data (especially about giant polar spots); and (iv) data pertaining to stellar superflares. Then we describe the current status of solar dynamo modelling—giving an introduction to the flux transport dynamo model, the currently favoured model for the solar cycle. While an extrapolation of this model to solar-like stars can explain some aspects of observational data, some other aspects of the data still remain to be theoretically explained. It is not clear right now whether we need a different kind of dynamo mechanism for stars having giant starspots or producing very strong superflares. Title: A Theoretical Study of the Build-up of the Sun’s Polar Magnetic Field by using a 3D Kinematic Dynamo Model Authors: Hazra, Gopal; Choudhuri, Arnab Rai; Miesch, Mark S. Bibcode: 2017ApJ...835...39H Altcode: 2016arXiv161002726H We develop a three-dimensional kinematic self-sustaining model of the solar dynamo in which the poloidal field generation is from tilted bipolar sunspot pairs placed on the solar surface above regions of strong toroidal field by using the SpotMaker algorithm, and then the transport of this poloidal field to the tachocline is primarily caused by turbulent diffusion. We obtain a dipolar solution within a certain range of parameters. We use this model to study the build-up of the polar magnetic field and show that some insights obtained from surface flux transport models have to be revised. We present results obtained by putting a single bipolar sunspot pair in a hemisphere and two symmetrical sunspot pairs in two hemispheres. We find that the polar fields produced by them disappear due to the upward advection of poloidal flux at low latitudes, which emerges as oppositely signed radial flux and which is then advected poleward by the meridional flow. We also study the effect that a large sunspot pair, violating Hale’s polarity law, would have on the polar field. We find that there would be some effect—especially if the anti-Hale pair appears at high latitudes in the mid-phase of the cycle—though the effect is not very dramatic. Title: The treatment of magnetic buoyancy in flux transport dynamo models Authors: Choudhuri, Arnab Rai; Hazra, Gopal Bibcode: 2016AdSpR..58.1560C Altcode: 2015arXiv151103782C One important ingredient of flux transport dynamo models is the rise of the toroidal magnetic field through the convection zone due to magnetic buoyancy to produce bipolar sunspots and then the generation of the poloidal magnetic field from these bipolar sunspots due to the Babcock-Leighton mechanism. Over the years, two methods of treating magnetic buoyancy-a local method and a non-local method-have been used widely by different groups in constructing 2D kinematic models of the flux transport dynamo. We review both these methods and conclude that neither of them is fully satisfactory-presumably because magnetic buoyancy is an inherently 3D process. We also point out so far we do not have proper understanding of why sunspot emergence is restricted to rather low latitudes. Title: Presenting the science of the Sun to the general public Authors: Choudhuri, Arnab Rai Bibcode: 2016cosp...41E1619C Altcode: Although the science behind the Sun is so fascinating, there has not been sufficient worldwide effort in presenting this science to the general public. My recently published popular science book "Nature's Third Cycle: A Story of Sunspots" (Oxford University Press, 2015) is probably the first popular science book introducing the phenomenology of the solar cycle along with a non-technical account of dynamo theory. I shall discuss my perspective of the challenges involved in presenting the science of the Sun to the public. The Amazon link of my book is: http://www.amazon.co.uk/Natures-Third-Cycle-Story-Sunspots/dp/0199674752/ Title: Correlation Between Decay Rate and Amplitude of Solar Cycles as Revealed from Observations and Dynamo Theory Authors: Hazra, Gopal; Karak, Bidya Binay; Banerjee, Dipankar; Choudhuri, Arnab Rai Bibcode: 2015SoPh..290.1851H Altcode: 2015SoPh..tmp...80H; 2014arXiv1410.8641H Using different proxies of solar activity, we have studied the following features of the solar cycle: i) The linear correlation between the amplitude of cycle and its decay rate, ii) the linear correlation between the amplitude of cycle n and the decay rate of cycle (n −1 ), and iii) the anti-correlation between the amplitude of cycle n and the period of cycle (n −1 ). Features ii) and iii) are very useful because they provide precursors for future cycles. We have reproduced these features using a flux-transport dynamo model with stochastic fluctuations in the Babcock-Leighton α effect and in the meridional circulation. Only when we introduce fluctuations in meridional circulation, are we able to reproduce different observed features of the solar cycle. We discuss the possible reasons for these correlations. Title: Book review: Nature's third cycle - a story of sunspots (Choudhuri) Authors: Meadows, P.; Choudhuri, A. R. Bibcode: 2015JBAA..125Q.123M Altcode: No abstract at ADS Title: Communicating the science of the 11-year sunspot cycle to the general public Authors: Choudhuri, A. R. Bibcode: 2015HiA....16..638C Altcode: Astrophysics is one branch of science which excites the imagination of the general public. Pioneer science popularizers like George Gamow and Fred Hoyle wrote on different aspects of astrophysics. However, of late, we see a trend which I find disturbing. While it has become extremely fashionable to write popular science books on cosmology, other areas of astrophysics are grossly neglected. Title: A Critical Assessment of the Flux Transport Dynamo Authors: Choudhuri, Arnab Rai Bibcode: 2015JApA...36....5C Altcode: 2015JApA..tmp...20C; 2014arXiv1408.3968C We first discuss how the flux transport dynamo with reasonably high diffusion can explain both the regular and the irregular features of the solar cycle quite well. Then, we critically examine the inadequacies of the model and the challenge posed by some recent observational data about meridional circulation, arriving at a conclusion that this model can still work within the bounds of observational data. Title: Flux Transport Dynamos: From Kinematics to Dynamics Authors: Karak, Bidya Binay; Jiang, Jie; Miesch, Mark S.; Charbonneau, Paul; Choudhuri, Arnab Rai Bibcode: 2015sac..book..561K Altcode: No abstract at ADS Title: Flux Transport Dynamos: From Kinematics to Dynamics Authors: Karak, Bidya Binay; Jiang, Jie; Miesch, Mark S.; Charbonneau, Paul; Choudhuri, Arnab Rai Bibcode: 2014SSRv..186..561K Altcode: 2014SSRv..tmp...55K Over the past several decades, Flux-Transport Dynamo (FTD) models have emerged as a popular paradigm for explaining the cyclic nature of solar magnetic activity. Their defining characteristic is the key role played by the mean meridional circulation in transporting magnetic flux and thereby regulating the cycle period. Most FTD models also incorporate the so-called Babcock-Leighton (BL) mechanism in which the mean poloidal field is produced by the emergence and subsequent dispersal of bipolar active regions. This feature is well grounded in solar observations and provides a means for assimilating observed surface flows and fields into the models in order to forecast future solar activity, to identify model biases, and to clarify the underlying physical processes. Furthermore, interpreting historical sunspot records within the context of FTD models can potentially provide insight into why cycle features such as amplitude and duration vary and what causes extreme events such as Grand Minima. Though they are generally robust in a modeling sense and make good contact with observed cycle features, FTD models rely on input physics that is only partially constrained by observation and that neglects the subtleties of convective transport, convective field generation, and nonlinear feedbacks. Here we review the formulation and application of FTD models and assess our current understanding of the input physics based largely on complementary 3D MHD simulations of solar convection, dynamo action, and flux emergence. Title: The irregularities of the sunspot cycle and their theoretical modelling Authors: Choudhuri, Arnab Rai Bibcode: 2014InJPh..88..877C Altcode: 2013arXiv1312.3408C The 11-year sunspot cycle has many irregularities, the most promi- nent amongst them being the grand minima when sunspots may not be seen for several cycles. After summarizing the relevant observational data about the irregularities, we introduce the flux transport dynamo model, the currently most successful theoretical model for explaining the 11-year sunspot cycle. Then we analyze the respective roles of nonlinearities and random fluctuations in creating the irregularities. We also discuss how it has recently been realized that the fluctuations in meridional circula- tion also can be a source of irregularities. We end by pointing out that fluctuations in the poloidal field generation and fluctuations in meridional circulation together can explain the occurrences of grand minima. Title: Polar Network Index as a Magnetic Proxy for the Solar Cycle Studies Authors: Priyal, Muthu; Banerjee, Dipankar; Karak, Bidya Binay; Muñoz-Jaramillo, Andrés; Ravindra, B.; Choudhuri, Arnab Rai; Singh, Jagdev Bibcode: 2014ApJ...793L...4P Altcode: 2014arXiv1407.4944P The Sun has a polar magnetic field which oscillates with the 11 yr sunspot cycle. This polar magnetic field is an important component of the dynamo process which operates in the solar convection zone and produces the sunspot cycle. We have direct systematic measurements of the Sun's polar magnetic field only from about the mid-1970s. There are, however, indirect proxies which give us information about this field at earlier times. The Ca-K spectroheliograms taken at the Kodaikanal Solar Observatory during 1904-2007 have now been digitized with 4k × 4k CCD and have higher resolution (~0.86 arcsec) than the other available historical data sets. From these Ca-K spectroheliograms, we have developed a completely new proxy (polar network index, hereafter PNI) for the Sun's polar magnetic field. We calculate PNI from the digitized images using an automated algorithm and calibrate our measured PNI against the polar field as measured by the Wilcox Solar Observatory for the period 1976-1990. This calibration allows us to estimate the polar fields for the earlier period up to 1904. The dynamo calculations performed with this proxy as input data reproduce reasonably well the Sun's magnetic behavior for the past century. Title: A Dynamo Model of Magnetic Activity in Solar-like Stars with Different Rotational Velocities Authors: Karak, Bidya Binay; Kitchatinov, Leonid L.; Choudhuri, Arnab Rai Bibcode: 2014ApJ...791...59K Altcode: 2014arXiv1402.1874K We attempt to provide a quantitative theoretical explanation for the observations that Ca II H/K emission and X-ray emission from solar-like stars increase with decreasing Rossby number (i.e., with faster rotation). Assuming that these emissions are caused by magnetic cycles similar to the sunspot cycle, we construct flux transport dynamo models of 1 M stars rotating with different rotation periods. We first compute the differential rotation and the meridional circulation inside these stars from a mean-field hydrodynamics model. Then these are substituted in our dynamo code to produce periodic solutions. We find that the dimensionless amplitude f m of the toroidal flux through the star increases with decreasing rotation period. The observational data can be matched if we assume the emissions to go as the power 3-4 of f m. Assuming that the Babcock-Leighton mechanism saturates with increasing rotation, we can provide an explanation for the observed saturation of emission at low Rossby numbers. The main failure of our model is that it predicts an increase of the magnetic cycle period with increasing rotation rate, which is the opposite of what is found observationally. Much of our calculations are based on the assumption that the magnetic buoyancy makes the magnetic flux tubes rise radially from the bottom of the convection zone. Taking into account the fact that the Coriolis force diverts the magnetic flux tubes to rise parallel to the rotation axis in rapidly rotating stars, the results do not change qualitatively. Title: Is a Deep One-cell Meridional Circulation Essential for the Flux Transport Solar Dynamo? Authors: Hazra, Gopal; Karak, Bidya Binay; Choudhuri, Arnab Rai Bibcode: 2014ApJ...782...93H Altcode: 2013arXiv1309.2838H The solar activity cycle is successfully modeled by the flux transport dynamo, in which the meridional circulation of the Sun plays an important role. Most of the kinematic dynamo simulations assume a one-cell structure of the meridional circulation within the convection zone, with the equatorward return flow at its bottom. In view of the recent claims that the return flow occurs at a much shallower depth, we explore whether a meridional circulation with such a shallow return flow can still retain the attractive features of the flux transport dynamo (such as a proper butterfly diagram, the proper phase relation between the toroidal and poloidal fields). We consider additional cells of the meridional circulation below the shallow return flow—both the case of multiple cells radially stacked above one another and the case of more complicated cell patterns. As long as there is an equatorward flow in low latitudes at the bottom of the convection zone, we find that the solar behavior is approximately reproduced. However, if there is either no flow or a poleward flow at the bottom of the convection zone, then we cannot reproduce solar behavior. On making the turbulent diffusivity low, we still find periodic behavior, although the period of the cycle becomes unrealistically large. In addition, with a low diffusivity, we do not get the observed correlation between the polar field at the sunspot minimum and the strength of the next cycle, which is reproduced when diffusivity is high. On introducing radially downward pumping, we get a more reasonable period and more solar-like behavior even with low diffusivity. Title: Studies of grand minima in sunspot cycles by using a flux transport solar dynamo model Authors: Karak, Bidya Binay; Choudhuri, Arnab Rai Bibcode: 2013RAA....13.1339K Altcode: 2013arXiv1306.5438K We propose that grand minima in solar activity are caused by simultaneous fluctuations in the meridional circulation and the Babcock—Leighton mechanism for the poloidal field generation in the flux transport dynamo model. We present the following results: (a) fluctuations in the meridional circulation are more effective in producing grand minima; (b) both sudden and gradual initiations of grand minima are possible; (c) distributions of durations and waiting times between grand minima seem to be exponential; (d) the coherence time of the meridional circulation has an effect on the number and the average duration of grand minima, with a coherence time of about 30 yr being consistent with observational data. We also study the occurrence of grand maxima and find that the distributions of durations and waiting times between grand maxima are also exponential, like the grand minima. Finally we address the question of whether the Babcock—Leighton mechanism can be operative during grand minima when there are no sunspots. We show that an α-effect restricted to the upper portions of the convection zone can pull the dynamo out of the grand minima and can match various observational requirements if the amplitude of this α-effect is suitably fine-tuned. Title: Flux-transport and mean-field dynamo theories of solar cycles Authors: Choudhuri, Arnab Rai Bibcode: 2013IAUS..294...37C Altcode: 2012arXiv1211.0520C We point out the difficulties in carrying out direct numerical simulation of the solar dynamo problem and argue that kinematic mean-field models are our best theoretical tools at present for explaining various aspects of the solar cycle in detail. The most promising kinematic mean-field model is the flux transport dynamo model, in which the toroidal field is produced by differential rotation in the tachocline, the poloidal field is produced by the Babcock-Leighton mechanism at the solar surface and the meridional circulation plays a crucial role. Depending on whether the diffusivity is high or low, either the diffusivity or the meridional circulation provides the main transport mechanism for the poloidal field to reach the bottom of the convection zone from the top. We point out that the high-diffusivity flux transport dynamo model is consistent with various aspects of observational data. The irregularities of the solar cycle are primarily produced by fluctuations in the Babcock-Leighton mechanism and in the meridional circulation. We summarize recent work on the fluctuations of meridional circulation in the flux transport dynamo, leading to explanations of such things as the Waldmeier effect. Title: Modelling grand minima of solar activity using a flux transport dynamo model Authors: Karak, Bidya Binay; Choudhuri, Arnab Rai Bibcode: 2013IAUS..294..433K Altcode: 2012arXiv1211.0165K The occurrence of grand minima like the Maunder minimum is an intriguing aspect of the sunspot cycle. We use the flux transport dynamo model to explain the grand minima, showing that they arise when either the poloidal field or the meridional circulation falls to a sufficiently low value due to fluctuations. Assuming these fluctuations to be Gaussian and determining the various parameters from the data of the last 28 cycles, we carry on a dynamo simulation with both these fluctuations. The results are remarkably close to the observational data. Title: Can Superflares Occur on Our Sun? Authors: Shibata, Kazunari; Isobe, Hiroaki; Hillier, Andrew; Choudhuri, Arnab Rai; Maehara, Hiroyuki; Ishii, Takako T.; Shibayama, Takuya; Notsu, Shota; Notsu, Yuta; Nagao, Takashi; Honda, Satoshi; Nogami, Daisaku Bibcode: 2013PASJ...65...49S Altcode: 2012arXiv1212.1361S Recent observations of Sun-like stars, similar to our Sun in their surface temperature (5600-6000 K) and slow rotation (rotational period > 10 d), using the Kepler satellite by Maehara et al. (2012, Nature, 485, 478) have revealed the existence of superflares (with energy of 1033-1035 erg). From statistical analyses of these superflares, it was found that superflares with energy of 1034 erg occur once in 800 yr, and superflares with 1035 erg occur once in 5000 yr. In this paper, we examine whether superflares with energy of 1033-1035 erg could occur on the present Sun through the use of simple order-of-magnitude estimates based on current ideas related to the mechanisms of the solar dynamo. If magnetic flux is generated by differential rotation at the base of the convection zone, as assumed in typical dynamo models, it is possible that the present Sun would generate a large sunspot with a total magnetic flux of ∼2 × 1023 Mx (= G cm2) within one solar cycle period, and lead to superflares with an energy of 1034 erg. To store a total magnetic flux of ∼1024 Mx, necessary for generating 1035 erg superflares, it would take ∼40 yr. Hot Jupiters have often been argued to be a necessary ingredient for the generation of superflares, but we found that they do not play any essential role in the generation of magnetic flux in the star itself, if we consider only the magnetic interaction between the star and the hot Jupiter. This seems to be consistent with Maehara et al.'s finding of 148 superflare-generating solar-type stars that do not have a hot Jupiter-like companion. Altogether, our simple calculations, combined with Maehara et al.'s analysis of superflares on Sun-like stars, show that there is a possibility that superflares of 1034 erg would occur once in 800 yr on our present Sun. Title: Fluctuations in the alpha-effect and grand solar minima Authors: Olemskoy, S. V.; Choudhuri, A. R.; Kitchatinov, L. L. Bibcode: 2013ARep...57..458O Altcode: 2013arXiv1305.2660O The parameters of a special type of α-effect known in dynamo theory as the Babcock-Leighton mechanism are estimated using the data of sunspot catalogs. The estimates support the presence of the Babcock-Leighton α-effect on the Sun. Fluctuations of the α-effect are also estimated. The fluctuation amplitude appreciably exceeds themean value, and the characteristic time for the fluctuations is comparable to the period of the solar rotation. Fluctuations with the parameters found are included in a numericalmodel for the solar dynamo. Computations show irregular changes in the amplitudes of the magnetic cycles on time scales of centuries and millennia. The calculated statistical characteristics of the grand solar minima and maxima agree with the data on solar activity over the Holocene. Title: Origin of Grand Minima in Sunspot Cycles Authors: Choudhuri, Arnab Rai; Karak, Bidya Binay Bibcode: 2012PhRvL.109q1103C Altcode: 2012arXiv1208.3947C One of the most striking aspects of the 11-year sunspot cycle is that there have been times in the past when some cycles went missing, a most well-known example of this being the Maunder minimum during 1645-1715. Analyses of cosmogenic isotopes (C14 and Be10) indicated that there were about 27 grand minima in the last 11 000 yrs, implying that about 2.7% of the solar cycles had conditions appropriate for forcing the Sun into grand minima. We address the question of how grand minima are produced and specifically calculate the frequency of occurrence of grand minima from a theoretical dynamo model. We assume that fluctuations in the poloidal field generation mechanism and in the meridional circulation produce irregularities of sunspot cycles. Taking these fluctuations to be Gaussian and estimating the values of important parameters from the data of the last 28 solar cycles, we show from our flux transport dynamo model that about 1-4% of the sunspot cycles may have conditions suitable for inducing grand minima. Title: Is meridional circulation important in modelling irregularities of the solar cycle? Authors: Karak, Bidya Binay; Choudhuri, Arnab Rai Bibcode: 2012IAUS..286..367K Altcode: 2011arXiv1111.2144K We explore the importance of meridional circulation variations in modelling the irregularities of the solar cycle by using the flux transport dynamo model. We show that a fluctuating meridional circulation can reproduce some features of the solar cycle like the Waldmeier effect and the grand minimum. However, we get all these results only if the value of the turbulent diffusivity in the convection zone is reasonably high. Title: Theoretical modeling of grand minima Authors: Choudhuri, Arnab Rai; Karak, Bidya Binay Bibcode: 2012cosp...39..339C Altcode: 2012cosp.meet..339C We explore whether the flux transport dynamo model of solar cycles can explain the occurrence of grand minima. If fluctuations in the Babcock-Leighton process make the poloidal field at the end of a cycle fall to sufficiently low values, then that can cause a grand minimum (Choudhuri and Karak 2009, RAA 9, 953). Additionally, if the meridional circulation of the Sun falls to a sufficiently low value, then that also can push the dynamo into a grand minimum if the diffusivity is sufficiently high (Karak 2010, ApJ 724, 1021). Considering Gaussian fluctuations in both poloidal field generation and in meridional circulation, we calculate the probability of occurrence of grand minima and find our results to be consistent with the observational claim that there have been about 27 grand minima in the last 11,000 years (Choudhuri and Karak 2012, under preparation). Title: Variable meridional circulation in the dynamo model Authors: Karak, Bidya Binay; Choudhuri, Arnab Rai Bibcode: 2012cosp...39..879K Altcode: 2012cosp.meet..879K Meridional circulation is an important ingredient in the flux transport dynamo models of modeling solar cycles. It connects spatially segregated sources of poloidal field generation (near the solar surface) and the toroidal field generation (near the bottom of the convection zone). Unfortunately the origin and specifically the temporal variation of the meridional circulation is very poorly known due to the observational limitation and also due to the complex dynamics of the solar convection zone. However using the relation based on the flux transport dynamo model that the meridional circulation is inversely related to the cycle period, we infer that the meridional circulation had random variation in past with a coherence time around 30-40 yrs. We have shown that this randomly variable meridional circulation helps to model irregularities of the solar cycle including some of its features like the Waldmeier effect. Title: Dynamo models of grand minima Authors: Choudhuri, Arnab Rai Bibcode: 2012IAUS..286..350C Altcode: 2011arXiv1111.1839C Since a universally accepted dynamo model of grand minima does not exist at the present time, we concentrate on the physical processes which may be behind the grand minima. After summarizing the relevant observational data, we make the point that, while the usual sources of irregularities of solar cycles may be sufficient to cause a grand minimum, the solar dynamo has to operate somewhat differently from the normal to bring the Sun out of the grand minimum. We then consider three possible sources of irregularities in the solar dynamo: (i) nonlinear effects; (ii) fluctuations in the poloidal field generation process; (iii) fluctuations in the meridional circulation. We conclude that (i) is unlikely to be the cause behind grand minima, but a combination of (ii) and (iii) may cause them. If fluctuations make the poloidal field fall much below the average or make the meridional circulation significantly weaker, then the Sun may be pushed into a grand minimum. Title: Quenching of Meridional Circulation in Flux Transport Dynamo Models Authors: Karak, Bidya Binay; Choudhuri, Arnab Rai Bibcode: 2012SoPh..278..137K Altcode: 2011arXiv1111.1540K Guided by the recent observational result that the meridional circulation of the Sun becomes weaker at the time of the sunspot maximum, we have included a parametric quenching of the meridional circulation in solar dynamo models such that the meridional circulation becomes weaker when the magnetic field at the base of the convection zone is stronger. We find that a flux transport solar dynamo tends to become unstable on including this quenching of meridional circulation if the diffusivity in the convection zone is less than about 2×1011 cm2 s−1. The quenching of α, however, has a stabilizing effect and it is possible to stabilize a dynamo with low diffusivity with sufficiently strong α-quenching. For dynamo models with high diffusivity, the quenching of meridional circulation does not produce a large effect and the dynamo remains stable. We present a solar-like solution from a dynamo model with diffusivity 2.8×1012 cm2 s−1 in which the quenching of meridional circulation makes the meridional circulation vary periodically with solar cycle as observed and does not have any other significant effect on the dynamo. Title: Possible explanations of the Maunder minimum from a flux transport dynamo model Authors: Karak, Bidya Binay; Choudhuri, Arnab Rai Bibcode: 2011IAUS..273..430K Altcode: 2011arXiv1101.4342K We propose that at the beginning of the Maunder minimum the poloidal field or amplitude of meridional circulation or both fell abruptly to low values. With this proposition, a flux transport dynamo model is able to reproduce various important aspects of the historical records of the Maunder minimum remarkably well. Title: A theoretical model of torsional oscillations from a flux transport dynamo model Authors: Chatterjee, Piyali; Chakraborty, Sagar; Choudhuri, Arnab Rai Bibcode: 2011IAUS..273..366C Altcode: 2010arXiv1008.2161C Assuming that the torsional oscillation is driven by the Lorentz force of the magnetic field associated with the sunspot cycle, we use a flux transport dynamo to model it and explain its initiation at a high latitude before the beginning of the sunspot cycle. Title: Origin of solar magnetism Authors: Choudhuri, Arnab Rai Bibcode: 2011IAUS..273...28C Altcode: 2010arXiv1008.2432C The most promising model for explaining the origin of solar magnetism is the flux transport dynamo model, in which the toroidal field is produced by differential rotation in the tachocline, the poloidal field is produced by the Babcock-Leighton mechanism at the solar surface and the meridional circulation plays a crucial role. After discussing how this model explains the regular periodic features of the solar cycle, we come to the questions of what causes irregularities of solar cycles and whether we can predict future cycles. Only if the diffusivity within the convection zone is sufficiently high, the polar field at the sunspot minimum is correlated with strength of the next cycle. This is in conformity with the limited available observational data. Title: The origin of the solar magnetic cycle Authors: Choudhuri, Arnab Rai Bibcode: 2011Prama..77...77C Altcode: 2011arXiv1103.3385C After summarizing the relevant observational data, we discuss how a study of flux tube dynamics in the solar convection zone helps us to understand the formation of sunspots. Then we introduce the flux transport dynamo model and assess its success in modelling both the solar cycle and its departures from strictly periodic behaviour. Title: Correlation Between The Rise Rate And The Amplitude Of The Solar Magnetic Cycles Authors: Karak, Bidya Binay; Choudhuri, Arnab Rai Bibcode: 2011arXiv1102.4052K Altcode: We discuss one important aspect of Waldmeier effect which says that the stronger cycles rise rapidly than weaker cycles. We studied four different data set of solar activity indices, and find strong linear correlation between rise rates and amplitudes of solar activity. We study this effect theoretically by introducing suitable stochastic fluctuations in our regular solar dynamo model. Title: The Waldmeier effect and the flux transport solar dynamo Authors: Karak, Bidya Binay; Choudhuri, Arnab Rai Bibcode: 2011MNRAS.410.1503K Altcode: 2010MNRAS.tmp.1490K; 2010arXiv1008.0824K We confirm that the evidence for the Waldmeier effect WE1 (the anticorrelation between rise times of sunspot cycles and their strengths) and the related effect WE2 (the correlation between rise rates of cycles and their strengths) is found in different kinds of sunspot data. We explore whether these effects can be explained theoretically on the basis of the flux transport dynamo models of sunspot cycles. Two sources of irregularities of sunspot cycles are included in our model: fluctuations in the poloidal field generation process and fluctuations in the meridional circulation. We find WE2 to be a robust result which is produced in different kinds of theoretical models for different sources of irregularities. The Waldmeier effect WE1, on the other hand, arises from fluctuations in the meridional circulation and is found only in the theoretical models with reasonably high turbulent diffusivity which ensures that the diffusion time is not more than a few years. Title: Back-reactions of dynamo-generated magnetic fields: torsional oscillations and variations in meridional circulation Authors: Choudhuri, Arnab Rai Bibcode: 2011ASInC...2..131C Altcode: 2011arXiv1111.2443C The periodically varying Lorentz force of the periodic solar magnetic field generated by the solar dynamo can induce two kinds of motions: torsional oscillations and periodic variations in the mc. Observational evidence now exists for both these kinds of motions. We discuss our ongoing effort in theoretically studying the variations of the mc. Then we present our theoretical model of torsional oscillations, which addresses the question why these oscillations start before sunspot cycles at latitudes higher than where sunspots are seen. Title: Solar physics in India: developments from the nineteenth century to the present era Authors: Hasan, S. S.; Choudhuri, Arnab Rai; Rajaguru, S. P. Bibcode: 2011ASInC...2..367H Altcode: Modern solar astronomy took root in India with the discovery of helium during the total solar eclipse of 1868 and followed by the setting up of the Kodaikanal Observatory in 1899. We provide a brief overview of the growth of this field, describe the various Indian solar observing facilities and summarize the highlights of solar research in India during the last few decades. Title: Astrophysics for Physicists Authors: Choudhuri, Arnab Rai; Smoot, George Bibcode: 2011PhT....64a..57C Altcode: No abstract at ADS Title: Modeling solar cycles using a variable meridional circulation in a flux transport dynamo model Authors: Karak, Bidya Binay; Choudhuri, Arnab Rai Bibcode: 2011ASInC...3...99K Altcode: The sunspot number - a proxy of solar activity - varies roughly periodically with time. However the individual cycle durations and amplitudes are found to vary in an irregular way. An important feature of the solar cycle is the Maunder minimum during 1645-1715 when there were very few sunspots. We explore whether this irregular solar cycle can be modeled with the help of a flux transport dynamo model of the solar cycle. We model the periods of the last 23 sunspot cycles by varying the meridional circulation speed. We find that most of the cycle amplitudes also get modeled up to some extent when we model the periods. Moreover, under certain situations we are able to reproduce Maunder like grand minimum. However, we fail to reproduce these results if the value of turbulent diffusivity is reasonably low. Title: Astrophysics for Physicists Authors: Choudhuri, Arnab Rai Bibcode: 2010asph.book.....C Altcode: 1. Introduction; 2. Interaction of radiation with matter; 3. Stellar astrophysics I: basic theoretical ideas and observational data; 4. Stellar astrophysics II: nucleosynthesis and other advanced topics; 5. End states of stellar collapse; 6. Our galaxy and its interstellar matter; 7. Elements of stellar dynamics; 8. Elements of plasma astrophysics; 9. Extragalactic astronomy; 10. The spacetime dynamics of the Universe; 11. The thermal history of the Universe; 12. Elements of tensors and general relativity; 13. Some applications of general relativity; 14. Relativistic cosmology; Appendixes; References; Index. Title: UTEP Center for Space Exploration Technology Research: Integrated Science and Engineering Approach to Propulsion, In-Situ Resource Utilization, and Planetary Science and Aerospace Education Authors: Choudhuri, A.; Borrok, D. M.; Hurtado, J. M.; Shafirovich, E. Bibcode: 2010LPI....41.2682C Altcode: The purpose of this presentation is to disseminate information on the Center for Space Exploration Technology Research (cSETR), established at the University of Texas at El Paso (UTEP), effective October 1, 2009. Title: The Waldmeier Effect in Sunspot Cycles Authors: Karak, B. B.; Choudhuri, A. R. Bibcode: 2010ASSP...19..402K Altcode: 2010arXiv1008.2931K; 2010mcia.conf..402K We discuss two aspects of the Waldmeier Effect, namely (1) the rise times of sunspot cycles are anti-correlated to their strengths (WE1) and (2) the rates of rise of the cycles are correlated to their strengths (WE2). To avoid overlapping effect and the lack of single peaks in some cycles, we carefully define rise times to study WE1. From analysis of four different data sets, we conclude that WE1 exists in all, although the significance levels are poor in some cases due to insufficient data. We also find strong evidence for WE2 in all the data sets. We study this effect theoretically by introducing suitable stochastic fluctuations in our regular solar dynamo model. Some preliminary results are presented. Title: Cycle Prediction from Dynamo Theory Authors: Choudhuri, A. R. Bibcode: 2010ASSP...19..498C Altcode: 2010mcia.conf..498C Many previous efforts in sunspot cycle prediction were based on various empirical correlations, most of which have limited statistical significance because they were inferred from observations of very few cycles. Perhaps the most successful of the empirical methods is to use the strength of the polar field in the previous sunspot minimum as a precursor for the next cycle. As the polar field at the present time is weak, Schatten [2005, Geophys. Res. Lett., 32, L21106] and Svalsgaard et al. [2005, Geophys. Res. Lett., 32, L01104] have predicted that cycle 24 will be a weak cycle. Title: Why Does the Torsional Oscillation Precede the Sunspot Cycle? Authors: Chatterjee, P.; Chakraborty, S.; Choudhuri, A. R. Bibcode: 2010ASSP...19..500C Altcode: 2010mcia.conf..500C The Sun's rotation shows a periodic variation with the sunspot cycle, called torsional oscillations, the nature of which inside the solar convection zone has been determined from helioseismology. Several authors developed theoretical models of torsional oscillations by assuming that they are driven by the Lorentz force of the Sun's cyclically varying magnetic field. If this is true, then one would expect the torsional oscillations to follow the sunspot cycles. However, the torsional oscillations of a cycle begin a couple of years before the sunspots of that cycle appear and at a latitude higher than where the first sunspots are subsequently seen. Our aim in this paper is to provide an explanation for this seemingly causality defying phenomenon. Title: A possible explanation of the Maunder minimum from a flux transport dynamo model Authors: Choudhuri, Arnab Rai; Karak, Bidya Binay Bibcode: 2009RAA.....9..953C Altcode: 2009arXiv0907.3106C We propose that the poloidal field at the end of the last sunspot cycle before the Maunder minimum fell to a very low value due to fluctuations in the Babcock-Leighton process. With this assumption, a flux transport dynamo model is able to explain various aspects of the historical records of the Maunder minimum remarkably well by suitably choosing the parameters of the model to give the correct growth time. Title: Erratum: Why Does the Sun's Torsional Oscillation Begin before the Sunspot Cycle? [Phys. Rev. Lett. 102, 041102 (2009)] Authors: Chakraborty, Sagar; Choudhuri, Arnab Rai; Chatterjee, Piyali Bibcode: 2009PhRvL.103i9902C Altcode: No abstract at ADS Title: The hemispheric asymmetry of solar activity during the last century and the solar dynamo Authors: Goel, Ashish; Choudhuri, Arnab Rai Bibcode: 2009RAA.....9..115G Altcode: 2007arXiv0712.3988G We believe the Babcock-Leighton process of poloidal field generation to be the main source of irregularity in the solar cycle. The random nature of this process may make the poloidal field in one hemisphere stronger than that in the other hemisphere at the end of a cycle. We expect this to induce an asymmetry in the next sunspot cycle. We look for evidence of this in the observational data and then model it theoretically with our dynamo code. Since actual polar field measurements exist only from the 1970s, we use the polar faculae number data recorded by Sheeley (1991, 2008) as a proxy of the polar field and estimate the hemispheric asymmetry of the polar field in different solar minima during the major part of the twentieth century. This asymmetry is found to have a reasonable correlation with the asymmetry of the next cycle. We then run our dynamo code by feeding information about this asymmetry at the successive minima and compare the results with observational data. We find that the theoretically computed asymmetries of different cycles compare favorably with the observational data, with the correlation coefficient being 0.73. Due to the coupling between the two hemispheres, any hemispheric asymmetry tends to get attenuated with time. The hemispheric asymmetry of a cycle either from observational data or from theoretical calculations statistically tends to be less than the asymmetry in the polar field (as inferred from the faculae data) in the preceding minimum. This reduction factor turns out to be 0.43 and 0.51 respectively in observational data and theoretical simulations. Title: Why Does the Sun's Torsional Oscillation Begin before the Sunspot Cycle? Authors: Chakraborty, Sagar; Choudhuri, Arnab Rai; Chatterjee, Piyali Bibcode: 2009PhRvL.102d1102C Altcode: 2009arXiv0907.4842C Although the Sun’s torsional oscillation is believed to be driven by the Lorentz force associated with the sunspot cycle, this oscillation begins 2 3 yr before the sunspot cycle. We provide a theoretical explanation of this with the help of a solar dynamo model having a meridional circulation penetrating slightly below the bottom of the convection zone, because only in such dynamo models does the strong toroidal field form a few years before the sunspot cycle and at a higher latitude. Title: Prospects for predicting cycle 24 Authors: Choudhuri, Arnab Rai Bibcode: 2008JApA...29...41C Altcode: No abstract at ADS Title: A theoretical model for the magnetic helicity of solar active regions Authors: Chatterjee, Piyali; Choudhuri, Arnab Rai; Petrovay, Kristof; Nandy, Dibyendu Bibcode: 2008AdSpR..41..893C Altcode: Active regions on the solar surface are known to possess magnetic helicity, which is predominantly negative in the northern hemisphere and positive in the southern hemisphere. Choudhuri et al. [Choudhuri, A.R. On the connection between mean field dynamo theory and flux tubes. Solar Phys. 215, 31 55, 2003] proposed that the magnetic helicity arises due to the wrapping up of the poloidal field of the convection zone around rising flux tubes which form active regions. Choudhuri [Choudhuri, A.R., Chatterjee, P., Nandy, D. Helicity of solar active regions from a dynamo model. ApJ 615, L57 L60, 2004] used this idea to calculate magnetic helicity from their solar dynamo model. Apart from getting broad agreements with observational data, they also predict that the hemispheric helicity rule may be violated at the beginning of a solar cycle. Chatterjee et al. [Chatterjee, P., Choudhuri, A.R., Petrovay, K. Development of twist in an emerging magnetic flux tube by poloidal field accretion. A&A 449, 781 789, 2006] study the penetration of the wrapped poloidal field into the rising flux tube due to turbulent diffusion using a simple 1-d model. They find that the extent of penetration of the wrapped field will depend on how weak the magnetic field inside the rising flux tube becomes before its emergence. They conclude that more detailed observational data will throw light on the physical conditions of flux tubes just before their emergence to the photosphere. Title: How far are we from a ‘Standard Model’ of the solar dynamo? Authors: Choudhuri, Arnab Rai Bibcode: 2008AdSpR..41..868C Altcode: Over the last few years, dynamo theorists seem to be converging on a basic scenario as to how the solar dynamo operates. The strong toroidal component of the magnetic field is produced in the tachocline, from where it rises due to magnetic buoyancy to produce active regions at the solar surface. The decay of tilted bipolar active regions at the surface gives rise to the poloidal component, which is first advected poleward by the meridional circulation and then taken below the surface to the tachocline where it can be stretched to produce the toroidal component. The mathematical formulation of this basic model, however, involves the specification of some parameters which are still uncertain. We review these remaining uncertainties which have resulted in disagreements amongst various research groups and have made it impossible to still arrive at something that can be called a standard model of the solar dynamo. Title: Solar activity forecast with a dynamo model Authors: Jiang, Jie; Chatterjee, Piyali; Choudhuri, Arnab Rai Bibcode: 2007MNRAS.381.1527J Altcode: 2007arXiv0707.2258J; 2007MNRAS.tmp..899J Although systematic measurements of the Sun's polar magnetic field exist only from mid-1970s, other proxies can be used to infer the polar field at earlier times. The observational data indicate a strong correlation between the polar field at a sunspot minimum and the strength of the next cycle, although the strength of the cycle is not correlated well with the polar field produced at its end. This suggests that the Babcock-Leighton mechanism of poloidal field generation from decaying sunspots involves randomness, whereas the other aspects of the dynamo process must be reasonably ordered and deterministic. Only if the magnetic diffusivity within the convection zone is assumed to be high (of order 1012cm2s-1), we can explain the correlation between the polar field at a minimum and the next cycle. We give several independent arguments that the diffusivity must be of this order. In a dynamo model with diffusivity like this, the poloidal field generated at the mid-latitudes is advected toward the poles by the meridional circulation and simultaneously diffuses towards the tachocline, where the toroidal field for the next cycle is produced. To model actual solar cycles with a dynamo model having such high diffusivity, we have to feed the observational data of the poloidal field at the minimum into the theoretical model. We develop a method of doing this in a systematic way. Our model predicts that cycle 24 will be a very weak cycle. Hemispheric asymmetry of solar activity is also calculated with our model and compared with observational data. Title: A New Explanation for the Origin of Trans-equatorial Loops based on a Dynamo Model Authors: Jiang, Jie; Choudhuri, Arnab Rai; Wang, Jingxiu Bibcode: 2007SoPh..245...19J Altcode: Trans-equatorial loops (TLs) are one of the distinct magnetic structures in the solar corona and have a close relationship to solar activity. We present a systematic study of the origin of TLs linking with the Babcock - Leighton dynamo process based on the model of Chatterjee, Nandy, and Choudhuri (Astron. Astrophys.427, 1019, 2004). We propose that TLs are visible signatures of poloidal field lines across the equator. The cycle variation of TL lengths obtained by the connectivities of poloidal field lines happens to be roughly in agreement with what one gets by considering the positions of sunspots. This explains why this cycle variation of TL lengths was found to be in conformity with Spörer's law. The active regions always make the poloidal field configuration favorable to form TLs, which causes the conformity. The formation of TLs is a three-dimensional problem, which will require three-dimensional dynamo models for full investigation. Title: An Elementary Introduction to Solar Dynamo Theory Authors: Choudhuri, Arnab Rai Bibcode: 2007AIPC..919...49C Altcode: The cyclically varying magnetic field of the Sun is believed to be produced by the hydromagnetic dynamo process. We first summarize the relevant observational data pertaining to sunspots and solar cycle. Then we review the basic principles of MHD needed to develop the dynamo theory. This is followed by a discussion how bipolar sunspots form due to magnetic buoyancy of flux tubes formed at the base of the solar convection zone. Following this, we come to the heart of dynamo theory. After summarizing the basic ideas of a turbulent dynamo and the basic principles of its mean field formulation, we present the famous dynamo wave solution, which was supposed to provide a model for the solar cycle. Finally we point out how a flux transport dynamo can circumvent some of the difficulties associated with the older dynamo models. Title: Predicting Solar Cycle 24 With a Solar Dynamo Model Authors: Choudhuri, Arnab Rai; Chatterjee, Piyali; Jiang, Jie Bibcode: 2007PhRvL..98m1103C Altcode: 2007astro.ph..1527C Whether or not the upcoming cycle 24 of solar activity will be strong is being hotly debated. The solar cycle is produced by a complex dynamo mechanism. We model the last few solar cycles by “feeding” observational data of the Sun’s polar magnetic field into our solar dynamo model. Our results fit the observed sunspot numbers of cycles 21 23 reasonably well and predict that cycle 24 will be about 35% weaker than cycle 23. Title: Helical Magnetic Fields in Solar Active Regions: Theory vs. Observations Authors: Petrovay, K.; Chaterjee, P.; Choudhuri, A. Bibcode: 2007astro.ph..2073P Altcode: The mean value of the normalized current helicity in solar active regions is on the order of 1e-8 1/m, negative in the northern hemisphere, positive in the southern hemisphere. Observations indicate that this helicity has a subsurface origin. Possible mechanisms leading to a twist of this amplitude in magnetic flux tubes include the solar dynamo, convective buffeting of rising flux tubes, and the accretion of weak external poloidal flux by a rising toroidal flux tube. After briefly reviewing the observational and theoretical constraints on the origin of helicity, we present a recently developed detailed model for poloidal flux accretion. Title: On Magnetic Coupling Between the Two Hemispheres in Solar Dynamo Models Authors: Chatterjee, Piyali; Choudhuri, Arnab Rai Bibcode: 2006SoPh..239...29C Altcode: 2006SoPh..tmp...77C By introducing an asymmetry between the two hemispheres, we study whether the solar dynamo solutions in the two hemispheres remain coupled with each other. Our calculations are based on the solar dynamo code SURYA, which incorporates the helioseismically-determined solar-rotation profile, a Babcock-Leighton α effect concentrated near the surface, and a meridional circulation. When the magnetic coupling between the hemispheres is enhanced by either increasing the diffusion or introducing an α effect distributed throughout the convection zone, we find that the solutions in the two hemispheres evolve together with a single period even when we make the meridional circulation or the α effect different in the two hemispheres. On the other hand, when the hemispheric coupling is weaker for other values of parameters, an asymmetry between the hemispheres can make solutions in the two hemispheres evolve independently with different periods. Title: Forecasting Cycle 24 with a Solar Dynamo Model Authors: Jiang, Jie; Chatterjee, P.; Choudhuri, A. R. Bibcode: 2006ihy..workE..28J Altcode: A challenge before solar physicists right now is to forecast the strength of the next solar cycle (Cycle 24). Several contrary forecasts have already been made. Most of the forecasts are based on various precursor methods. Only one forecast is based on a dynamo model (Dikpati and Gilman 2006). Since we find some aspects of this work questionable, it is desirable to have another independent forecast based on a dynamo model. We are carrying out an analysis based on our dynamo model, using a methodology different from what was used by Dikpati and Gilman (2006). We shall present the methodology of our approach and, most probably, we shall also have some results by the time of the IHY meeting. Title: Some Recent Developments in Solar Dynamo Theory Authors: Choudhuri, Arnab Rai Bibcode: 2006JApA...27...79C Altcode: We discuss the current status of solar dynamo theory and describe the dynamo model developed by our group. The toroidal magnetic field is generated in the tachocline by the strong differential rotation and rises to the solar surface due to magnetic buoyancy to create active regions. The decay of these active regions at the surface gives rise to the poloidal magnetic field by the Babcock-Leighton mechanism. This poloidal field is advected by the meridional circulation first to high latitudes and then down below to the tachocline. Dynamo models based on these ideas match different aspects of observational data reasonably well. Title: Helical Magnetic Fields in Solar Active Regions: Theory vs. Observations Authors: Petrovay, K.; Chaterjee, P.; Choudhuri, A. Bibcode: 2006PADEU..17....5P Altcode: The mean value of the normalized current helicity α_p=čB\cdot(nabla×čB)/B^2 in solar active regions is on the order of 10^{-8} m^{-1}, negative in the northern hemisphere, positive in the southern hemisphere. Observations indicate that this helicity has a subsurface origin. Possible mechanisms leading to a twist of this amplitude in magnetic flux tubes include the solar dynamo, convective buffeting of rising flux tubes, and the accretion of weak external poloidal flux by a rising toroidal flux tube. After briefly reviewing the observational and theoretical constraints on the origin of helicity, we present a recently developed detailed model for poloidal flux accretion. Title: On the Origin of Current Helicity in Active Regions Authors: Petrovay, K.; Chatterjee, P.; Choudhuri, A. Bibcode: 2006ESASP.617E..67P Altcode: 2006soho...17E..67P No abstract at ADS Title: Development of twist in an emerging magnetic flux tube by poloidal field accretion Authors: Chatterjee, P.; Choudhuri, A. R.; Petrovay, K. Bibcode: 2006A&A...449..781C Altcode: 2005astro.ph.12472C Aims.Following an earlier proposal for the origin of twist in the magnetic fields of solar active regions, we model the penetration of a wrapped up background poloidal field into a toroidal magnetic flux tube rising through the solar convective zone. Methods.The rise of the straight, cylindrical flux tube is followed by numerically solving the induction equation in a comoving Lagrangian frame, while an external poloidal magnetic field is assumed to be radially advected onto the tube with a speed corresponding to the rise velocity. Results.One prediction of our model is the existence of a ring of reverse current helicity on the periphery of active regions. On the other hand, the amplitude of the resulting twist depends sensitively on the assumed structure (diffuse vs. concentrated/intermittent) of the active region magnetic field right before its emergence, and on the assumed vertical profile of the poloidal field. Nevertheless, in the model with the most plausible choice of assumptions a mean twist comparable to the observations results. Conclusions.Our results indicate that the contribution of this mechanism to the twist can be quite significant, and under favourable circumstances it can potentially account for most of the current helicity observed in active regions. Title: How far are we from a 'Standard Model' of the solar dynamo? Authors: Choudhuri, A. R. Bibcode: 2006cosp...36..595C Altcode: 2006cosp.meet..595C Many aspects of the solar cycle can be explained with kinematic solar dynamo models In a kinematic dynamo model it is necessary to specify various parameters such as the differential rotation the alpha-coefficient the turbulent diffusion and the meridional circulation in addition to prescribing some way to treat the magnetic buoyancy Within the last few years new developments in helioseismology and flux tube simulations have put important constraints on many of these parameters Different solar dynamo groups around the world now agree on some basics although there still exist major sources of disagreement I shall describe the current status of solar dynamo models which take into account the various constraints I shall also list the major remaining uncertainties and discuss how they may possibly be resolved in future Title: Why do millisecond pulsars have weaker magnetic fields compared to ordinary pulsars? Authors: Choudhuri, A. R.; Konar, S. Bibcode: 2006cosp...36..719C Altcode: 2006cosp.meet..719C Millisecond pulsars with magnetic fields weaker by three to four orders compared to those of ordinary pulsars are presumed to be neutron stars spun up by binary accretion We expect the magnetic field to get screened by the accreted material Our simulation of this screening mechanism shows that the field decreases by a purely geometric factor sin^(-7/2) theta_(P,i) before freezing to an asymptotic value where theta_(P_i) is the initial angular width of the polar cap If theta_(P_i) lies in the range 5 - 10 ° then the magnetic field diminution factor turns out to be approx 10^3 - 10^4 in conformity with observational data The detailed results of the simulation are presented in two publications (Choudhuri & Konar 2002, MNRAS 332, 933; Konar & Choudhuri 2004, MNRAS 348, 661) Title: A theoretical model for the magnetic helicity of solar active regions Authors: Choudhuri, A. R.; Chatterjee, P.; Petrovay, K.; Nandy, D. Bibcode: 2006cosp...36..714C Altcode: 2006cosp.meet..714C Active regions on the solar surface are known to possess magnetic helicity which is predominantly negative in the northern hemisphere and positive in the southern hemisphere Choudhuri 2003 Sol Phys 123 217 proposed that the magnetic helicity arises due to the wrapping up of the poloidal field of the convection zone around rising flux tubes which form active regions Choudhuri Chatterjee and Nandy 2004 ApJ 615 L57 used this idea to calculate magnetic helicity from their solar dynamo model and found broad agreements with observational data Chatterjee Choudhuri and Petrovay 2006 A A in press have studied the penetration of the wrapped poloidal field into the rising flux tube and concluded that more detailed observational data will throw light on the physical conditions of flux tubes just before their emergence to the photosphere Title: Reply to the Comments of Dikpati et al. Authors: Choudhuri, A. R.; Nandy, D.; Chatterjee, P. Bibcode: 2005A&A...437..703C Altcode: 2005astro.ph..5232C We respond to Dikpati et al.'s criticism of our recent solar dynamo model. A different treatment of the magnetic buoyancy is the most probable reason for their different results. Title: Full-sphere simulations of a circulation-dominated solar dynamo: Exploring the parity issue Authors: Chatterjee, P.; Nandy, D.; Choudhuri, A. R. Bibcode: 2004A&A...427.1019C Altcode: 2004astro.ph..5027C We explore a two-dimensional kinematic solar dynamo model in a full sphere, based on the helioseismically determined solar rotation profile and with an α effect concentrated near the solar surface, which captures the Babcock-Leighton idea that the poloidal field is created from the decay of tilted bipolar active regions. The meridional circulation, assumed to penetrate slightly below the tachocline, plays an important role. Some doubts have recently been raised regarding the ability of such a model to reproduce solar-like dipolar parity. We specifically address the parity issue and show that the dipolar mode is preferred when certain reasonable conditions are satisfied, the most important condition being the requirement that the poloidal field should diffuse efficiently to get coupled across the equator. Our model is shown to reproduce various aspects of observational data, including the phase relation between sunspots and the weak, diffuse field. Title: Helicity of Solar Active Regions from a Dynamo Model Authors: Choudhuri, Arnab Rai; Chatterjee, Piyali; Nandy, Dibyendu Bibcode: 2004ApJ...615L..57C Altcode: We calculate helicities of solar active regions based on the idea that poloidal flux lines get wrapped around a toroidal flux tube rising through the convection zone, thereby giving rise to the helicity. Rough estimates based on this idea compare favorably with the observed magnitude of helicity. We use our solar dynamo model based on the Babcock-Leighton α-effect to study how helicity varies with latitude and time. At the time of solar maximum, our theoretical model gives negative helicity in the northern hemisphere and positive helicity in the south, in accordance with observed hemispheric trends. However, we find that during a short interval at the beginning of a cycle, helicities tend to be opposite of the preferred hemispheric trends. Title: Impact Features from Vargeão Dome, Southern Brazil Authors: Kazzuo-Vieira, C.; Crósta, A. P.; Choudhuri, A. Bibcode: 2004M&PSA..39.5050K Altcode: No abstract at ADS Title: Diamagnetic screening of the magnetic field in accreting neutron stars - II. The effect of polar cap widening Authors: Konar, Sushan; Choudhuri, Arnab Rai Bibcode: 2004MNRAS.348..661K Altcode: 2003astro.ph..4490K Recently, we have proposed a model for the screening of the magnetic field of an accreting neutron star by the accreted material flowing from the polar regions towards the equator and sinking there underneath the surface. In this earlier model, it was assumed that the flow pattern remained stationary over time. However, as the surface magnetic field weakens, the accretion takes place over a wider region around the pole, making the flow more radial and isotropic. In the present work, we extend this two-dimensional model to include the time dependence of the flow of the accreted material. The final radial flow is found to be less efficient in screening the magnetic field compared with the initial tangential flow. After an initial phase of rapid decay, the magnetic field slowly reaches an asymptotic value when the accretion becomes nearly isotropic and radial. Assuming the initial extent of the polar cap to be ~5°-10°, a simple geometric argument suggests that the magnetic field should decay by 3-4 orders of magnitude before stabilizing to an asymptotic value, consistent with the magnetic fields observed in millisecond pulsars. Title: Why do millisecond pulsars have weaker magnetic fields compared to ordinary pulsars? Authors: Choudhuri, Arnab Rai; Konar, Sushan Bibcode: 2004CSci...86..444C Altcode: 2003astro.ph.11031C Millisecond pulsars, with magnetic fields weaker by three to four orders compared to those of ordinary pulsars, are presumed to be neutron stars spun up by binary accretion. We expect the magnetic field to get screened by the accreted material. Our simulation of this screening mechanism shows that the field decreases by a purely geometric factor sin-7/2 qP,i before freezing to an asymptotic value, where qP,i is the initial angular width of the polar cap. If qP,i lies in the range 5-10 °, then the magnetic field diminution factor turns out to be ~ 103-104, in conformity with observational data. Title: Full Sphere Axisymmetric Simulations of the Solar Dynamo Authors: Nandy, Dibyendu; Chatterjee, Piyali; Choudhuri, Arnab Rai Bibcode: 2004IAUS..223..133N Altcode: 2005IAUS..223..133N We explore a full sphere (2D axisymmetric) kinematic solar dynamo model based on the Babcock-Leighton idea that the poloidal field is generated in the surface layers from the decay of tilted bipolar solar active regions. This model incorporates the helioseismically deduced solar rotation profile and an algorithm for buoyancy motivated from simulations of flux tube dynamics. A prescribed deep meridional circulation plays an important role in the advection of magnetic flux. We specifically address the parity issue and show that - contrary to some recent claims - the Babcock-Leighton dynamo can reproduce solar-like dipolar parity if certain reasonable conditions are satisfied in the solar interior, the most important requirement being that the poloidal field of the two hemispheres be efficiently coupled across the equator. Title: The Origin of Helicity in Solar Active Regions Authors: Choudhuri, Arnab Rai; Chatterjee, Piyali; Nandy, Dibyendu Bibcode: 2004IAUS..223...45C Altcode: 2005IAUS..223...45C; 2004astro.ph..6598C We present calculations of helicity based on our solar dynamo model and show that the results are consistent with observational data. Title: On Solar Radius Variation with Magnetic Field Authors: Choudhuri, Arnab Rai; Chatterjee, Piyali Bibcode: 2003astro.ph.11028C Altcode: In response to the claim by Dziembowski et al. (2001) that the solar radius decreases with magnetic activity at the rate of 1.5 km/yr, we consider the theoretical question whether a radius variation is expected with the solar cycle. If the radius variation is caused by the magnetic pressure of toroidal flux tubes at the bottom of the convection zone, then the dynamo model of Nandy and Choudhuri (2002) would suggest a radius decrease with magnetic activity, in contrast to other dynamo models which would suggest a radius increase. However, the radius decrease is estimated to be only of the order of hundreds of metres. Title: On the Connection Between Mean Field Dynamo Theory and Flux Tubes Authors: Choudhuri, Arnab Rai Bibcode: 2003SoPh..215...31C Altcode: 2002astro.ph.11591C Mean field dynamo theory deals with various mean quantities and does not directly throw any light on the question of existence of flux tubes. We can, however, draw important conclusions about flux tubes in the interior of the Sun by combining additional arguments with the insights gained from solar dynamo solutions. The polar magnetic field of the Sun is of order 10 G, whereas the toroidal magnetic field at the bottom of the convection zone has been estimated to be 100 000 G. Simple order-of-magnitude estimates show that the shear in the tachocline is not sufficient to stretch a 10 G mean radial field into a 100 000 G mean toroidal field. We argue that the polar field of the Sun must get concentrated into intermittent flux tubes before it is advected to the tachocline. We estimate the strengths and filling factors of these flux tubes. Stretching by shear in the tachocline is then expected to produce a highly intermittent magnetic configuration at the bottom of the convection zone. The meridional flow at the bottom of the convection zone should be able to carry this intermittent magnetic field equatorward, as suggested recently by Nandy and Choudhuri (2002). When a flux tube from the bottom of the convection zone rises to a region of pre-existing poloidal field at the surface, we point out that it picks up a twist in accordance with the observations of current helicities at the solar surface. Title: Insights on Turbulent Flows Authors: Nandy, D.; Choudhuri, A. R. Bibcode: 2003PADEU..13...21N Altcode: Turbulent flows in the interior of the Sun, both at small and large scales, are believed to feed and sustain the solar hydromagnetic dynamo that generates the solar cycle. The solar cycle itself strikingly manifests in a 11-year periodic variation in the number of sunspots seen on the solar surface. Sunspots are regions of concentrated magnetic fields, occurring at low latitudes on the solar surface and are believed to be tracers of the underlying dynamo mechanism. An important ingredient in recent models of the dynamo mechanism is the meridional flow of material, which is believed to originate from turbulent stresses in the solar convection zone. This meridional circulation is observed to be poleward in the outer 15% of the Sun and must be balanced by an equatorward counterflow in the interior. The nature and exact location of this counterflow, however, is unknown. We discuss here results from a dynamo model that reproduces the correct latitudinal distribution of sunspots and show that this requires a meridional counterflow of material that penetrates much deeper than hitherto believed -- into the radiative layers below the convection zone. We comment on the viability of such a deep counterflow of material and discuss its implications for turbulent convection and elemental abundance in the Sun and related stellar atmospheres. Title: The solar dynamo as a model of the solar cycle Authors: Choudhuri, A. R. Bibcode: 2003dysu.book..103C Altcode: It is believed that the Sun's magnetic field is produced by the dynamo process, which involves nonlinear interactions between the solar plasma and the magnetic field. Summarising the main charateristics of solar magnetic field, the basic ideas of dynamo theory are presented and its current status is discussed. Title: Diamagnetic screening of the magnetic field in accreting neutron stars Authors: Konar, Sushan; Choudhuri, Arnab Rai Bibcode: 2002BASI...30..697K Altcode: 2002astro.ph..2248K A possible mechanism for screening of the surface magnetic field of an accreting neutron star, by the accreted material, is investigated. In particular, we investigate the nature of the evolution of the internal field configuration in the case of a) a polar cap accretion and b) a spherical accretion. Title: Solar dynamo models with realistic internal rotation Authors: Choudhuri, Arnab Rai; Nandy, Dibyendu Bibcode: 2002ESASP.505...91C Altcode: 2002IAUCo.188...91C; 2002solm.conf...91C Solar dynamo models based on differetial rotation inferred from helioseismology tend to produce rather strong magnetic activity at high solar latitudes, in contrast to the observed fact that sunspots appear at low latitudes. We show that a meridional circulation penetrating below the tachocline can solve this problem. Title: Diamagnetic screening of the magnetic field in accreting neutron stars Authors: Choudhuri, Arnab Rai; Konar, Sushan Bibcode: 2002MNRAS.332..933C Altcode: 2001astro.ph..8229C A possible mechanism for screening of the surface magnetic field of an accreting neutron star, by the accreted material, is investigated. We model the material flow in the surface layers of the star by an assumed two-dimensional velocity field satisfying all the physical requirements. Using this model velocity we find that, in the absence of magnetic buoyancy, the surface field is screened (i.e. there is submergence of the field by advection) within the time-scale of material flow of the top layers. On the other hand, if magnetic buoyancy is present, the screening happens over a time-scale that is characteristic of the slower flow of the deeper (and hence, denser) layers. For accreting neutron stars, this longer time-scale turns out to be about 105yr, which is of a similar order of magnitude to the accretion time-scale of most massive X-ray binaries. Title: Explaining the Latitudinal Distribution of Sunspots with Deep Meridional Flow Authors: Nandy, Dibyendu; Choudhuri, Arnab Rai Bibcode: 2002Sci...296.1671N Altcode: Sunspots, dark magnetic regions occurring at low latitudes on the Sun's surface, are tracers of the magnetic field generated by the dynamo mechanism. Recent solar dynamo models, which use the helioseismically determined solar rotation, indicate that sunspots should form at high latitudes, contrary to observations. We present a dynamo model with the correct latitudinal distribution of sunspots and demonstrate that this requires a meridional flow of material that penetrates deeper than hitherto believed, into the stable layers below the convection zone. Such a deep material flow may have important implications for turbulent convection and elemental abundance in the Sun and similar stars. Title: On the absence of sunspots at high solar latitudes and associated constraints on the meridional flow in the solar interior Authors: Nandy, D.; Choudhuri, A. R. Bibcode: 2002AAS...200.8901N Altcode: 2002BAAS...34..791N Sunspots -- dark magnetic regions -- occur at low latitudes on the Sun's surface and are believed to be tracers of the magnetic field generated in the interior by the dynamo mechanism. An important ingredient in recent models of this dynamo mechanism is the meridional flow of material, which is observed to be poleward on the Sun's surface and must be balanced by an equatorward counterflow in the interior. The nature and exact location of this counterflow, however, is unknown. Recent solar dynamo models, which use the helioseismically determined internal rotation of the Sun and confine the counterflow within the convection zone (as classical theories of solar convection would suggest), indicate that sunspots should form at higher latitudes, contrary to observations. Here we present a solar dynamo model with the correct latitudinal distribution of sunspots and show that this requires a counterflow that penetrates much deeper than hitherto believed - into the stable layers below the convection zone. The existence of such a deep counterflow of material may have important implications for turbulent convection and elemental abundance in the Sun and related stellar atmospheres. Title: Diamagnetic Screening of the Magnetic Field of an Accreting Neutron Star Authors: Konar, S.; Choudhuri, A. Bibcode: 2002cosp...34E.721K Altcode: 2002cosp.meetE.721K A possible mechanism for screening of the surface magnetic field of an accreting neutron star, by the accreted material, is investigated. In particular, we investigate the nature of the evolution of the internal field configuration in the case of a) a polar cap accretion and b) a spherical accretion. Title: The Orientational Relaxation of Bipolar Active Regions Authors: Longcope, Dana; Choudhuri, Arnab Rai Bibcode: 2002SoPh..205...63L Altcode: In the mean, bipolar active regions are oriented nearly toroidally, according to Hale's polarity law, with a latitude-dependent tilt known as Joy's Law. The tilt angles of individual active regions deviate from this mean behavior and change over time. It has been found that on average the change is toward the mean angle at a rate characteristic of 4.37 days (Howard, 1996). We show that this orientational relaxation is consistent with the standard model of flux tube emergence from a deep dynamo layer. Under this scenario Joy's law results from the Coriolis effect on the rising flux tube (D'Silva and Choudhuri, 1993), and departures from it result from turbulent buffeting of the tubes (Longcope and Fisher, 1996). We show that relaxation toward Joy's angle occurs because the turbulent perturbations relax on shorter time scales than the perturbations from the Coriolis force. The turbulent perturbations relax more rapidly because they are localized to the topmost portion of the convection zone while the Coriolis perturbations are more widely distributed. If a fully-developed active region remains connected to the strong toroidal magnetic field at the base of the convection zone, its tilt will eventually disappear, leaving it aligned perfectly toroidally. On the other hand, if the flux becomes disconnected from the toroidal field the bipole will assume a tilt indicative of the location of disconnection. We compare models which are connected and disconnected from the toroidal field. Only those disconnected at points very deep in the convection zone are consistent with observed time scale of orientational relaxation. Title: Toward a Mean Field Formulation of the Babcock-Leighton Type Solar Dynamo. I. α-Coefficient versus Durney's Double-Ring Approach Authors: Nandy, Dibyendu; Choudhuri, Arnab Rai Bibcode: 2001ApJ...551..576N Altcode: 2001astro.ph..7466N We develop a model of the solar dynamo in which, on the one hand, we follow the Babcock-Leighton approach to include surface processes, such as the production of poloidal field from the decay of active regions, and, on the other hand, we attempt to develop a mean field theory that can be studied in quantitative detail. One of the main challenges in developing such models is to treat the buoyant rise of the toroidal field and the production of poloidal field from it near the surface. A previous paper by Choudhuri, Schüssler, & Dikpati in 1995 did not incorporate buoyancy. We extend this model by two contrasting methods. In one method, we incorporate the generation of the poloidal field near the solar surface by Durney's procedure of double-ring eruption. In the second method, the poloidal field generation is treated by a positive α-effect concentrated near the solar surface coupled with an algorithm for handling buoyancy. The two methods are found to give qualitatively similar results. Title: The Current Status of Kinematic Solar Dynamo Models Authors: Choudhuri, A. R. Bibcode: 2000JApA...21..373C Altcode: No abstract at ADS Title: The Role of Magnetic Buoyancy in a Babcock-Leighton Type Solar Dynamo Authors: Nandy, D.; Choudhuri, A. R. Bibcode: 2000JApA...21..381N Altcode: No abstract at ADS Title: Incorporating magnetic buoyancy in solar dynamo models: New results, problems -- and their possible solutions. Authors: Nandy, D.; Choudhuri, A. R. Bibcode: 2000SPD....31.0134N Altcode: There have been traditionally two kinds of approaches to understand the origin of the solar magnetic cycle: the Parker--Steenbeck--Krause--Rädler approach and the Babcock--Leighton approach. It seems at present that the most promising models of the solar dynamo are those which incorporate the best features of both these traditional approaches. One of the uncertainties in these hybrid models (Choudhuri et. al. 1995) lies in the treatment of magnetic buoyancy within a mean field framework, a subject which has rarely been explored in the past (Durney 1997). We study this problem by exploring possible ways of incorporating magnetic buoyancy in a dynamo code -- to simulate the formation and subsequent decay of sunspots and the recycling of fields, with magnetic buoyancy as an important player in the flux-transport process. The results as well as some problems faced by such new generation of dynamo models, will be discussed. References: Durney B. R., 1997, ApJ 486, 1065 Choudhuri A. R., Schussler M., Dikpati M., 1995, A&A 303, L29 Nandi D., Choudhuri A. R., 2000, submitted to ApJ Title: Incorporating magnetic buoyancy in solar dynamo models: new results, problems - and their possible solutions. Authors: Nandi, D.; Choudhuri, A. R. Bibcode: 2000BAAS...32..807N Altcode: No abstract at ADS Title: The solar dynamo Authors: Choudhuri, Arnab Rai Bibcode: 1999CSci...77.1475C Altcode: No abstract at ADS Title: On the large-scale diffuse magnetic field of the Sun - II. The Contribution of Active Regions Authors: Choudhuri, Arnab Rai; Dikpati, Mausumi Bibcode: 1999SoPh..184...61C Altcode: Dikpati and Choudhuri (1994, 1995) developed a model for the poleward migration of the weak diffuse magnetic field on the Sun's surface. This field was identified with the poloidal component produced by the solar dynamo operating at the base of the convection zone, and its evolution was studied by considering the effects of meridional circulation and turbulent diffusion. The earlier model is extended in this paper by incorporating the flux from, the decay of tilted active regions near the solar surface as an additional source of the poloidal field. This extended model can now explain various low-latitude features in the time-latitude diagram of the weak diffuse fields. These low-latitude features could not be accounted for in the earlier model, which was very successful in modeling the behavior at high latitudes. The time-latitude diagrams show that regions of a particular polarity often have `tongues' of opposite polarity. Such tongues can be produced in the theoretical model by incorporating fluctuations in the source term arising out of the decaying active regions. Title: The physics of fluids and plasmas : an introduction for astrophysicists / Authors: Choudhuri, Arnab Rai Bibcode: 1998pfp..book.....C Altcode: Introduction; Part I. Neutral Fluids: 2. Boltzmann equation; 3. March towards hydrodynamics; 4. Properties of ideal fluids; 5. Viscous flows; 6. Gas dynamics; 7. Linear theory of waves and instabilities; 8. Turbulence; 9. Rotation and hydrodynamics; Part II. Plasmas: 10. Plasma orbit theory; 11. Dynamics of many charged particles; 12. Collisionless processes in plasmas; 13. Collisional processes and the one-fluid model; 14. Basic magnetohydrodynamics; 15. Theory of magnetic topologies; 16. Dynamo theory; Appendices: A. Useful vector relations; B. Integrals in kinetic theory; C. Formulae and equations in cylindrical and spherical coordinates; D. Values of various quantities; E. Basic parameters pertaining to plasmas; Suggestions for further reading; References. Title: Coronal heating by magnetic kink waves Authors: Banerjee, D.; Dikpati, M.; Choudhuri, A. R. Bibcode: 1998ASPC..138...15B Altcode: 1998stas.conf...15B No abstract at ADS Title: (Erratum) The solar dynamo with meridional circulation. Authors: Choudhuri, A. R.; Schuessler, M.; Dikpati, M. Bibcode: 1997A&A...319..362C Altcode: Erratum to Astron. Astrophys. 303, L29 (1995). Title: Magnetic fields in the sun's interior: What do we know about them? Authors: Choudhuri, Arnab Rai Bibcode: 1996BASI...24..219C Altcode: No abstract at ADS Title: On the Out of Phase Appearance of Large-Scale Diffuse Magnetic Field of the Sun with Respect to Sunspots Authors: Dikpati, Mausumi; Choudhuri, Arnab Rai Bibcode: 1996Ap&SS.243..169D Altcode: 1996IAUCo.154..169D We assume the large-scale diffuse magnetic field of the Sun to originate from the poloidal component of a dynamo operating at the base of the convection zone, whereas the sunspots are due to the toroidal component. The evolution of the poloidal component is studied to model the poleward migration of the diffuse field seen on the solar surface and the polar reversal at the time of sunspots maxima (Dikpati and Choudhuri 1994, 1995). Title: The Evolutton Of The Magnetic Structure of the Solar Corona With The Solar Cycle Authors: Dikpati, Mausumi; Choudhuri, Arnab Rai; Venkatakrishnan, P. Bibcode: 1996ASPC...95..309D Altcode: 1996sdit.conf..309D No abstract at ADS Title: Energy Transport to the Solar Corona by Magnetic Kink Waves Authors: Choudhuri, A. R.; Dikpati, M.; Banerjee, D. Bibcode: 1995JApAS..16..390C Altcode: No abstract at ADS Title: The Evolution of Weak Magnetic Fields of the Sun in Relation to Dynamo Theory Authors: Dikpati, M.; Choudhuri, A. R. Bibcode: 1995JApAS..16..391D Altcode: No abstract at ADS Title: The solar dynamo with meridional circulation. Authors: Choudhuri, A. R.; Schussler, M.; Dikpati, M. Bibcode: 1995A&A...303L..29C Altcode: We show that meridional circulation can have a profound influence on dynamo models for the solar cycle. Motivated by the observed tilt angles of sunspot groups we assume that the generation of the poloidal field takes place near the surface, while a shear layer of radial differential rotation produces the toroidal field at the bottom of the convection zone. Both layers are coupled by a circulation with a poleward directed flow in the upper part and an equatorward flow in the deep layers of the convection zone. The circulation forces the toroidal field belts (which are responsible for the surface activity) to move equatorward. This leads to butterfly diagrams in qualitative agreement with the observations, even if the dynamo wave would propagate poleward in the absence of circulation. This result opens the possibility to construct models for the solar cycle which are based on observational data (tilt angles, differential rotation, and meridional circulation). Title: On the Large-Scale Diffuse Magnetic Field of the Sun Authors: Dikpati, Mausumi; Choudhuri, Arnab Rai Bibcode: 1995SoPh..161....9D Altcode: Although the sunspots migrate towards the equator, the large-scale weak diffuse magnetic fields of the Sun migrate poleward with the solar cycle, the polar field reversing at the time of the sunspot maxima. We apply the vector model of Dikpati and Choudhuri (1994, Paper I) to fit these observations. The dynamo layer at the base of the convection zone is taken to be the source of the diffuse field, which is then evolved in the convection zone subject to meridional circulation and turbulent diffusion. We find that the longitudinally averaged observational data can be fitted reasonably well both for positive and negative values of theα-effect by adjusting the subsurface meridional flow suitably. The model will be extended in a future paper to include the decay of active regions as an extra source of the diffuse field, which may be necessary to explain the probable phase lag betweenBr andBφ at lower latitudes. Title: The evolution of the Sun's poloidal field. Authors: Dikpati, M.; Choudhuri, A. R. Bibcode: 1994A&A...291..975D Altcode: We present here a model to explain how the weak large-scale diffuse magnetic fields of the Sun migrate poleward in contrast to the sunspots which migrate equatorward with the progress of the solar cycle. We study the evolution of the Sun's poloidal field in the convection zone by assuming that it is produced by an equatorward-propagating dynamo wave at the base of the convection zone and is then subject to turbulent diffusion and a meridional circulation with a poleward surface flow. The magnetic fieldlines in the lower part of the convection zone first move towards the equator where they are pushed upward by the upwelling meridional flow there to form magnetic bubbles by joining with their opposite hemisphere counterparts. After reaching the surface, these bubbles drift to higher latitudes with the poleward meridional flow. Our model incorporates the three-dimensional vector character of the magnetic field, whereas the previous flux transport models treated the magnetic field as a scalar on the two-dimensional solar surface. Title: Energy Transport to the Solar Corona by Magnetic Kink Waves Authors: Choudhuri, Arnab R.; Dikpati, Mausumi; Banerjee, Dipankar Bibcode: 1993ApJ...413..811C Altcode: We show that the magnetic kink waves generated by the motions of photospheric footpoints of the coronal flux tubes can supply adequate energy for heating the quiet corona, provided there are occasional rapid motions of these footpoints as found in recent observations. Choudhuri et al. (1992) modeled the solar corona as isothermal atmosphere and showed that these rapid motions are much more efficient for transporting energy compared to the slow footpoint motions taking place most of the time. We extend these calculations for a two-layer atmosphere, with the lower layer having chromospheric thickness and temperature, and the upper layer having coronal temperature. Even in the presence of such a temperature jump we find that the rapid footpoint motions are still much more efficient for transporting energy to the corona and the estimated energy flux is sufficient for quiet coronal heating. We discuss the general problem of the propagation of kink pulses in a two-layer atmosphere for different possible values of the basic parameters. We find a fairly complicated behavior which could not be anticipated from the analysis of a pure Fourier mode. Title: A theoretical model for tilts of bipolar magnetic regions Authors: D'Silva, S.; Choudhuri, A. R. Bibcode: 1993A&A...272..621D Altcode: Joy's law (Hale et al. 1919) states that bipolar magnetic regions (BMRs) are inclined to the latitudinal line, with the p-spot (preceding spot) of the BMR closer to the equator and the tilt angle increasing with latitude. It is believed that the solar dynamo operates in the overshoot region just below the convection zone and the BMRs are produced by the flux loops rising from there due to magnetic buoyancy. These rising loops are expected to be twisted by the Coriolis force so that they eventually emerge on the solar surface with a tilt. We extend the numerical calculations of Choudhuri (1989) to study the tilts produced on the rising flux loops by the Coriolis force. We find that the theoretically calculated tilts match the observations only if the magnetic field of the flux loops lies in the range between 60 and 160 kG. For such flux loops, the tilt has the correct magnitude and also varies correctly with the latitude. If the magnetic fields were stronger than 160 kG, then Coriolis force is much weaker than magnetic buoyancy and is only able to produce tilts which are very small in overall magnitude, though they still vary correctly with latitude. On the other hand, if the fields were smaller than 60 kG, then the Coriolis force would have been so overpowering that the flux loops would move parallel to the rotation axis as found earlier (Choudhuri 1989). Such flux loops appear only in high latitudes and do not obey Joy's law. On changing the drag on the flux tube, these conclusions are not changed. If we change the footpoint separation of the flux loop, then we find that magnetic tension may halt the rise of the flux loop if the footpoint separation is below a critical value. However, for flux tubes which are able to reach the surface, the range from 60 to 160 kG for the magnetic field still approximately holds. Thus our calculations seem to rule out either equipartition fields (about 10 kG) or very strong megagauss fields. Title: Implications of Rapid Footpoint Motions of Photospheric Flux Tubes for Coronal Heating Authors: Choudhuri, Arnab R.; Auffret, Herve; Priest, Eric R. Bibcode: 1993SoPh..143...49C Altcode: Some recent observations at Pic-du-Midi (Mulleret al., 1992a) suggest that the photospheric footpoints of coronal magnetic field lines occasionally move rapidly with typical velocities of the order 3 km s−1 for about 3 or 4 min. We argue that such occasional rapid footpoint motions could have a profound impact on the heating of the quiet corona. Qualitative estimates indicate that these occasional rapid motions can account for the entire energy flux needed to heat the quiet corona. We therefore carry out a mathematical analysis to study in detail the response of a vertical thin flux tube to photospheric footpoint motions in terms of a superposition of linear kink modes for an isothermal atmosphere. We find the resulting total energy that is asymptotically injected into an isothermal atmosphere (i.e., an atmosphere without any back reflection). By using typical parameter values for fast and slow footpoint motions, we show that, even if the footpoints spend only 2.5% of the time undergoing rapid motions, still these rapid motions could be more efficient in transporting energy to the corona than the slow motions that take place most of the time. Title: The Cluster Model of Sunspots Authors: Choudhuri, Arnab R. Bibcode: 1992ASIC..375..243C Altcode: 1992sto..work..243C The cluster model of sunspots proposed by Parker (1979) is examined in the light of recent theoretical and observational developments. In particular, attention is given to the original arguments for the cluster model, fine structure of sunspots, growth and decay of sunspots, and waves and oscillations in sunspots. The importance of defining the regime of validity of the cluster model is emphasized. Title: Stochastic fluctuations of the solar dynamo Authors: Choudhuri, A. R. Bibcode: 1992A&A...253..277C Altcode: The solar dynamo equations are presently solved in a slab with a single mode, taking the alpha-coefficient to be constant in space, but fluctuating stochastically in time with given amplitude and correlation time. Choudhuri's (1990) contention that the solar dynamo is of the alpha-squared(omega) type is reinforced by the solar behavior's qualitative agreement with such a dynamo's level of irregularities, which increase with rising amplitude or correlation time of stochastic fluctuations. Title: The Effect of Kelvin-Helmholtz Instability on Rising Flux Tubes in the Convection Zone Authors: D'Silva, Sydney Z.; Choudhuri, Arnab R. Bibcode: 1991SoPh..136..201D Altcode: If the solar dynamo operates at the bottom of the convection zone, then the magnetic flux created there has to rise to the surface. When the convection zone is regarded as passive, the rising flux is deflected by the Coriolis force to emerge at rather high latitudes, poleward of typical sunspot zones (Choudhuri and Gilman, 1987; Choudhuri, 1989). Choudhuri and D'Silva (1990) included the effects of convective turbulence on the rising flux through (a) giant cell drag and (b) momentum exchange by small-scale turbulence. The momentum exchange mechanism could enable flux tubes of radii not more than a few hundred km to emerge radially at low latitudes, but the giant cell drag mechanism required unrealistically small flux tube radii (a few meters for a reasonable giant cell upflow) to counteract the Coriolis force. We now include the additional effect of Kelvin-Helmholtz instability in a symmetrical flux ring caused by the azimuthal flow induced during its rise. The azimuthal flow crosses the threshold for the instability only if there is a giant cell upflow to drag the flux tubes appreciably. In the absence of such a drag, as in the case of a passive convection zone or in the case of momentum exchange by small-scale turbulence, the azimuthal velocity never becomes large enough to cause the instability, leaving the results of the previous calculations unaltered. The giant cell drag, aided by Kelvin-Helmholtz instability, however, becomes now a viable mechanism for curbing the Coriolis force - 104 G flux tubes with radii of a few hundred km being dragged radially by upflows of 70 m s-1. Title: Influence of turbulence on rising flux tubes in the solar convection zone Authors: Choudhuri, A. R.; D'Silva, S. Bibcode: 1990A&A...239..326C Altcode: The role of turbulence in facilitating the flux tubes generated at low solar latitudes at the bottom of the convection zone to emerge at the typical sunspot latitudes is investigated. It is found that large scale turbulence on the scale of the giant cells cannot dominate the Coriolis force, since such domination would require either an unreasonably large updraft velocity in the giant cells or an unreasonably small flux tube radii. On the other hand, small-scale turbulence can suppress the Coriolis force by exchanging angular momentum between the flux tube and the surroundings, provided the flux tubes have radii smaller than a few hundred km. Title: A correction to Spruit's equation for the dynamics of thin flux tubes Authors: Choudhuri, A. R. Bibcode: 1990A&A...239..335C Altcode: It is pointed out that a term was overlooked in the derivation of the equation of motion for a thin flux tube by Spruit (1981). The correction to be applied in an inertial frame and in a rotating frame are discussed. This correction makes the formulation self-consistent, though it does not invalidate the qualitative results obtained by various investigators who have used Spruit's equation. Title: On the Possibility of an alpha 2 omega --Type Dynamo in a Thin Layer inside the Sun Authors: Choudhuri, Arnab Rai Bibcode: 1990ApJ...355..733C Altcode: If the solar dynamo operates in a thin layer of 10,000-km thickness at the interface between the convection zone and the radiative core, using the facts that the dynamo should have a period of 22 years and a half-wavelength of 40 deg in the theta-direction, it is possible to impose restrictions on the values which various dynamo parameters are allowed to have. It is pointed out that the dynamo should be of alpha-sq omega nature, and kinematical calculations are presented for free dynamo waves and for dynamos in thin rectangular slabs with appropriate boundary conditions. An alpha-sq omega dynamo is expected to produce a significant poloidal field which does not leak to the solar surface. It is found that the turbulent diffusity eta and alpha-coefficient are restricted to values within about a factor of 10, the median values being eta of about 10 to the 10th sq cm/sec and alpha of about 10 cm/sec. On the basis of mixing length theory, it is pointed out that such values imply a reasonable turbulent velocity of the order 30 m/s, but rather small turbulent length scales like 300 km. Title: Locating the Seat of the Solar Dynamo Authors: Choudhuri, Arnab R. Bibcode: 1990IAUS..142...51C Altcode: The hypothesis that the solar dynamo operates in a thin layer at the bottom of the convection zone is addressed. Recent work on the question whether the magnetic flux can be made to emerge at sunspot latitudes is reviewed. It is concluded that this hypothesis can fit the observational facts only if there is turbulence with a length scale of a few hundred kilometers in and around the dynamo region. Title: Effect of Turbulence on Emerging Magnetic Flux Tubes in the Convection Zone Authors: D'Silva, S.; Choudhuri, A. R. Bibcode: 1990IAUS..142...60D Altcode: No abstract at ADS Title: The Evolution of Loop Structures in Flux Rings Within the Solar Convection Zone Authors: Choudhuri, Arnab Rai Bibcode: 1989SoPh..123..217C Altcode: Choudhuri and Gilman (1987) considered certain implications of the hypothesis that the magnetic flux within the Sun is generated at the bottom of the convection zone and then rises through it. Taking flux rings symmetric around the rotation axis and using reasonable values of different parameters, they found that the Coriolis force deflects these flux rings into trajectories parallel to the rotation axis so that they emerge at rather high latitudes. This paper looks into the question of whether the action of the Coriolis force is subdued when the initial configuration of the flux ring has non-axisymmetries in the form of loop structures. The results depend dramatically on whether the flux ring with the loops lies completely within the convection zone or whether the lower parts of it are embedded in the stable layers underneath the convection zone. In the first case, the Coriolis force supresses the non-axisymmetric perturbations so that the flux ring tends to remain symmetric and the trajectories are very similar to those of Choudhuri and Gilman (1987). In the second case, however, the lower parts of the flux ring may remain anchored underneath the bottom of the convection zone, but the upper parts of the loops still tend to move parallel to the rotation axis and emerge at high latitudes. Thus the problem of the magnetic flux not being able to come out at the sunspot latitudes still persists after the non-axisymmetries in the flux rings are taken into account. Title: The Possible Role of Meridional Flows in Suppressing Magnetic Buoyancy Authors: van Ballegooijen, A. A.; Choudhuri, A. R. Bibcode: 1988ApJ...333..965V Altcode: The equation of motion for a toroidal flux ring in a stellar convective envelope is derived, and the equilibrium of such a ring is considered. Necessary conditions for the stability of toroidal flux rings are derived, and results of stability calculations for a particular model of the meridional flow are presented. The motions of the flux rings when the rings are far from their equilibrium position or when equilibrium does not exist are considered. The results confirm the linear stability analysis, and show that in the absence of stable equilibrium, the rings move toward the solar surface along a trajectory which is parallel to the rotation axis. It is expected that viscosity will tend to reduce the rotational velocity difference between the flux ring and its surroundings, thus reducing the Coriolis force and altering the equilibrium. The storage time of toroidal flux rings is estimated, and some implications for the sun are discussed. Title: On the coalescence of twisted flux tubes Authors: Choudhuri, Arnab Rai Bibcode: 1988GApFD..40..261C Altcode: We study the problem of the coalescence of twisted flux tubes by assuming that the azimuthal field lines reconnect at a current sheet during the coalescence process and everywhere else the magnetic field is frozen in the fluid. We derive relations connecting the topology of the coalesced flux tube with the topologies of the initial flux tubes, and then obtain a structure equation for calculating the field configuration of the coalesced flux tube from the given topology. Some solutions for the two extreme cases of low- plasma and high- plasma are discussed. The coalesced flux tube has less twist than the initial flux tube. Magnetic helicity is found to be exactly conserved during the coalescence, but the assumptions in the model put a constraint on the energy dissipation so that we do not get a relaxation to the minimum-energy Taylor state in the low- case. It is pointed out that the structure equation connecting the topology and the equilibrium configuration is quite general and can be of use in many two-dimensional flux tube problems. Title: Theoretical modelling of the fine structures in sunspots. Authors: Choudhuri, Arnab Rai Bibcode: 1987NASCP2483..105C Altcode: 1987tphr.conf..105C Until a decade ago most solar physicists thought of a sunspot as the upper end of a giant flux tube floating vertically. The existence of umbral dots and penumbral grains has been known for several decades. On the basis of available observations, they seem to be regions of photospheric intensity with upflowing gas motion and magnetic fields much weaker than in the surrounding sunspot surface. It has also been suggested that the differences in the appearances of umbral dots and granular cells are caused by the highly nonlinear nature of the convection problem in the presense of strong magnetic fields. The main ideas are presented here without any equations. It can be shown that a pocket of field free gas surrounded by a vertical magnetic field in the presence of gravity takes up the shape of a tapering column ending at a vertex at the top. Some convection is expected to take place in the trapped field free gas, whereas the magnetic field around it makes those regions stable against convection. Eventually the apex of the tapering column reaches the photospheric surface where the bulging of the magnetic field makes the field no longer able to close on the field free gas and trap it underneath. Title: The Coalescence of Twisted Magnetic Flux Tubes Authors: Choudhuri, A. R. Bibcode: 1987BAAS...19R.939C Altcode: No abstract at ADS Title: The Influence of the Coriolis Force on Flux Tubes Rising through the Solar Convection Zone Authors: Choudhuri, Arnab Rai; Gilman, Peter A. Bibcode: 1987ApJ...316..788C Altcode: In order to study the effect of the Coriolis force due to solar rotation on rising magnetic flux, the authors consider a flux ring, azimuthally symmetric around the rotation axis, starting from rest at the bottom of the convection zone, and then follow the trajectory of the flux ring as it rises. If it is assumed that the flux ring remains azimuthally symmetric during its ascent, then the problem can be described essentially in terms of two parameters: the value of the initial magnetic field in the ring when it starts, and the effective drag experienced by it. For field strengths at the bottom of the convection zone of order 10,000 G or less, it is found that the Coriolis force plays a dominant role and flux rings starting from low latitudes at the bottom are deflected and emerge at latitudes significantly poleward of sunspot zones. Title: Magnetic helicity as a constraint on coronal dissipation. Authors: Choudhuri, Arnab Rai Bibcode: 1986NASCP2442..451C Altcode: 1986copp.nasa..451C The Taylor hypothesis has provided a model for the relaxed magnetic configurations of not only laboratory plasmas, but also of astrophysical plasmas. However, energy dissipation is possible only for systems which depart from a strict Taylor state, and hence a parameter describing that departure must be introduced, when the Taylor hypothesis is used to estimate the dissipation. An application of the Taylor hypothesis to the problem of coronal heating provides an insight into this difficult problem. When particular sorts of footpoint motions put energy and helicity in the corona, the conservation of helicity puts a constraint on how much of the energy can be dissipated. However, on considering a random distribution of footpoint motions, this constraint gets washed away, and the Taylor hypothesis is probably not going to play any significant role in the actual calculation of relevant physical quantities in the coronal heating problem. Title: Magnetic Energy Dissipation in Force-free Jets Authors: Choudhuri, Arnab Rai; Konigl, Arieh Bibcode: 1986ApJ...310...96C Altcode: It is shown that a magnetic-pressure-dominated, supersonic jet which expands (or contracts) in response to variations in the confining external pressure can dissipate magnetic energy through field-line reconnection as it relaxes to a minimum-energy configuration. In order for a continuous dissipation to take place, the effective reconnection time must be a fraction ɛ ⪉ 1 of the expansion time. The amount of energy dissipation is calculated, and it is concluded that magnetic energy dissipation could, in principle, power the observed synchrotron emission in extragalactic radio jets such as NGC 6251. However, this mechanism is only viable if the reconnection time is substantially shorter than the nominal resistive tearing time in the jet. Title: Force-free Equilibria of Magnetized Jets: Erratum Authors: Koenigl, Arieh; Choudhuri, Arnab Rai Bibcode: 1986ApJ...305..954K Altcode: No abstract at ADS Title: The Dynamics of Magnetically Trapped Fluids. I. Implications for Umbral Dots and Penumbral Grains Authors: Choudhuri, A. R. Bibcode: 1986ApJ...302..809C Altcode: A study of the magnetohydrodynamic system in which a nonmagnetized fluid in a gravitational field is surrounded by a fluid carrying a vertical magnetic field is presented. It is pointed out that this study can throw some light on the fine-structural features of a sunspot. The equilibrium configuration of the field-free fluid is a tapering column ending at an apex. The regions away form the apex can be studied by the slender flux tube approximation. A scheme developed to treat the apex indicates that, just below the apex, the radius of the tapering column opens up with a 3/2 power dependence on the depth below the apex. If the internal pressure of the field-free fluid is increased, the apex rises, and a static equilibrium may not be possible beyond a limit if the magnetic pressure drops quickly above a certain height. The nature of steady-flow solutions beyond this limit is investigated. Under conditions inside a sunspot, a column of field-free gas is found to rise with a velocity of about 100 km/hr. If umbral dots and penumbral grains are interpreted as regions where the field-free gas ultimately emerges, a very natural explanation of most of their observed properties is obtained. Title: The Influence of the Coriolis Force on Flux Tubes Rising through Solar Convection Zone Authors: Choudhuri, A. R.; Gilman, P. A. Bibcode: 1986BAAS...18..703C Altcode: No abstract at ADS Title: Force-free Equilibria of Magnetized Jets Authors: Koenigl, A.; Choudhuri, A. R. Bibcode: 1985ApJ...289..173K Altcode: Force-free equilibrium configurations of magnetic-pressure-dominated magnetized supersonic jets confined by slowly varying external pressure are investigated analytically. For the case where internal dissipation mechanisms are active, the lowest-energy field configuration is found to be the superposition of an axisymmetric mode and a helical mode with a wavelength equal to 5 times the jet radius, and the pressure below which the nonaxisymmetric mode becomes energetically favorable is given as 2700 times the product of the 4th power of the magnetic helicity per unit length and the -6th power of the magnetic flux. A model of the total and polarized emission of such a configuration is developed and applied to the extended well-collimated astronomically resolved jet NGC 6251. The model is shown to reproduce significant features such as transverse oscillations of the ridge line, width oscillations and emission knots, the projected magnetic-field configuration, oscillations of the degree of polarization, and the distribution of the Faraday rotation measure. Title: A model of the polarization position-angle swings in BL Lacertae objects. Authors: Konigl, A.; Choudhuri, A. R. Bibcode: 1985ApJ...289..188K Altcode: The polarization position-angle swings that have been measured in a number of BL Lacertae objects and highly variable quasars are interpreted in terms of shock waves which illuminate (by enhanced synchrotron radiation) successive transverse cross sections of a magnetized, relativistic jet. The jet is assumed to have a nonaxisymmetric magnetic field configuration of the type discussed in the companion paper on the equilibria of force-free jets. For a jet that is viewed at a small angle to the axis, the passage of a shock will give rise to an apparent rotation of the polarization position angle whose amplitude can be substantially larger than 180 deg. The effects of freely propagating shocks are compared with those of bow shocks which form in front of dense obstacles in the jet, and specific applications to 0727 - 115 and BL Lacertae are considered. In the case of 0727 - 115, it is pointed out that the nonuniformity of the swing rate and the apparent oscillations of the degree of polarization could be a consequence of relativistic aberration. Title: The dynamics of magnetically-trapped fluids: 1. Implications for umbral dots and penumbral grains Authors: Choudhuri, Arnab Rai Bibcode: 1985PhDT.......173C Altcode: No abstract at ADS Title: The effect of closed boundary conditions on a stationary dynamo Authors: Choudhuri, A. R. Bibcode: 1984ApJ...281..846C Altcode: One of two boundary conditions generally assumed in solutions of the dynamo equation is related to the disappearance of the azimuthal field at the boundary. Parker (1984) points out that for the realization of this condition the field must escape freely through the surface. Escape requires that the field be detached from the gas in which it is embedded. In the case of the sun, this can be accomplished only through reconnection in the tenuous gas above the visible surface. Parker concludes that the observed magnetic activity on the solar surface permits at most three percent of the emerging flux to escape. He arrives at the conclusion that, instead of B(phi) = 0, the partial derivative of B(phi) to r is equal to zero. The present investigation is concerned with the effect of changing the boundary condition according to Parker's conclusion. Implications for the solar convection zone are discussed. Title: The Effect of Closed Boundary Conditions on the Solar Dynamo Authors: Choudhuri, A. R. Bibcode: 1983BAAS...15..994C Altcode: No abstract at ADS Title: Nonaxisymmetric equilibria of magnetized jets. Authors: Königl, A.; Choudhuri, A. R. Bibcode: 1983BAAS...15..944K Altcode: No abstract at ADS Title: Monaxisymmetric Equilibria of Magnetized Jets Authors: Königl, A.; Choudhuri, A. R. Bibcode: 1983BAAS...15Q.944K Altcode: No abstract at ADS Title: Basic Magmatism in Guiana and Continental Drift Authors: Choudhuri, A.; Milner, M. W. Bibcode: 1971NPhS..232..154C Altcode: 1971Natur.232..154C IN this article we discuss some features of basic magmatism on the Guiana Shield that are relevant to the recent article by Le Bas1.