12 results on '"Vipin K. Yadav"'
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2. Science objectives of the magnetic field experiment onboard Aditya-L1 spacecraft
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Nandita Srivastava, Vipin K. Yadav, Santosh Ghosh, P. T. Srikar, and Krishnamoorthy Subhalakshmi
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Atmospheric Science ,010504 meteorology & atmospheric sciences ,Magnetometer ,Aerospace Engineering ,01 natural sciences ,law.invention ,law ,0103 physical sciences ,Coronal mass ejection ,Astrophysics::Solar and Stellar Astrophysics ,Interplanetary magnetic field ,010303 astronomy & astrophysics ,0105 earth and related environmental sciences ,Remote sensing ,Physics ,Spacecraft ,business.industry ,Astronomy and Astrophysics ,Fluxgate compass ,Solar wind ,Geophysics ,Space and Planetary Science ,Physics::Space Physics ,General Earth and Planetary Sciences ,Astrophysics::Earth and Planetary Astrophysics ,Interplanetary spaceflight ,business ,Halo orbit - Abstract
The Aditya-L1 is first Indian solar mission scheduled to be placed in a halo orbit around the first Lagrangian point (L1) of Sun-Earth system in the year 2018–19. The approved scientific payloads onboard Aditya-L1 spacecraft includes a Fluxgate Digital Magnetometer (FGM) to measure the local magnetic field which is necessary to supplement the outcome of other scientific experiments onboard. The in-situ vector magnetic field data at L1 is essential for better understanding of the data provided by the particle and plasma analysis experiments, onboard Aditya-L1 mission. Also, the dynamics of Coronal Mass Ejections (CMEs) can be better understood with the help of in-situ magnetic field data at the L1 point region. This data will also serve as crucial input for the short lead-time space weather forecasting models. The proposed FGM is a dual range magnetic sensor on a 6 m long boom mounted on the Sun viewing panel deck and configured to deploy along the negative roll direction of the spacecraft. Two sets of sensors (tri-axial each) are proposed to be mounted, one at the tip of boom (6 m from the spacecraft) and other, midway (3 m from the spacecraft). The main science objective of this experiment is to measure the magnitude and nature of the interplanetary magnetic field (IMF) locally and to study the disturbed magnetic conditions and extreme solar events by detecting the CME from Sun as a transient event. The proposed secondary science objectives are to study the impact of interplanetary structures and shock solar wind interaction on geo-space environment and to detect low frequency plasma waves emanating from the solar corona at L1 point. This will provide a better understanding on how the Sun affects interplanetary space. In this paper, we shall give the main scientific objectives of the magnetic field experiment and brief technical details of the FGM onboard Aditya-1 spacecraft.
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- 2018
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3. Observation of suprathermal argon in the exosphere of Mars
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Tirtha Pratim Das, P. Sreelatha, R. Satheesh Thampi, A. V. Aliyas, Neha Naik, J. K. Abhishek, Smitha V. Thampi, Amarnath Nandi, G. Padma Padmanabhan, B. Sundar, Anil Bhardwaj, Dinakar Prasad Vajja, M. B. Dhanya, P. Pradeepkumar, and Vipin K. Yadav
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Martian ,education.field_of_study ,010504 meteorology & atmospheric sciences ,Population ,Scale height ,Atmosphere of Mars ,Mars Exploration Program ,01 natural sciences ,Astrobiology ,law.invention ,Orbiter ,Geophysics ,Altitude ,law ,0103 physical sciences ,General Earth and Planetary Sciences ,education ,010303 astronomy & astrophysics ,Geology ,0105 earth and related environmental sciences ,Exosphere - Abstract
The altitude profiles of argon-40 (Ar) in the Martian exosphere are reported using Mars Exospheric Neutral Composition Analyser aboard Indian Mars Orbiter Mission (MOM) from four orbits during December 2014 (Ls = 250°–257°), when MOM's periapsis altitude was the lowest. The upper limit of Ar number density corresponding to this period is ∼5 × 105 cm−3 (∼250 km), and the typical scale height is ∼16 km, corresponding to an exospheric temperature of ∼275 K. However, on two orbits, the scale height over this altitude region is found to increase significantly making the effective temperature >400 K. Neutral Gas and Ion Mass Spectrometer observations on the Mars Atmosphere and Volatile Evolution mission also indicate that the change in slope in Ar density occurs near the upper exosphere (around 230–260 km). These observations indicate significant suprathermal CO2 and Ar populations in the Martian exosphere. Significant wave-like perturbations are observed but only on certain days when suprathermal population is seen. Pickup ion-induced heating is discussed as the other viable source.
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- 2017
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4. On the evening time exosphere of Mars: Result from MENCA aboard Mars Orbiter Mission
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P. Sreelatha, Amarnath Nandi, B. Sundar, J. K. Abhishek, Smitha V. Thampi, Neha Naik, Anil Bhardwaj, M. B. Dhanya, A. V. Aliyas, Gogulapati Supriya, G. Padma Padmanabhan, P. Pradeepkumar, R. Satheesh Thampi, Dinakar Prasad Vajja, Tirtha Pratim Das, S. V. Mohankumar, and Vipin K. Yadav
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Martian ,010504 meteorology & atmospheric sciences ,Atmospheric escape ,Mars Exploration Program ,Sunset ,01 natural sciences ,Astrobiology ,law.invention ,Atmosphere ,Orbiter ,Geophysics ,Altitude ,law ,0103 physical sciences ,General Earth and Planetary Sciences ,Environmental science ,010303 astronomy & astrophysics ,0105 earth and related environmental sciences ,Exosphere - Abstract
The Mars Exospheric Neutral Composition Analyser (MENCA) aboard the Indian Mars Orbiter Mission (MOM) is a quadrupole mass spectrometer which provides in situ measurement of the composition of the low-latitude Martian neutral exosphere. The altitude profiles of the three major constituents, i.e., amu 44 (CO2), amu 28 (N2 + CO), and amu 16 (O) in the Martian exosphere during evening (close to sunset terminator) hours are reported using MENCA observations from four orbits of MOM during late December 2014, when MOM's periapsis altitude was the lowest. The altitude range of the observation encompasses the diffusively separated region much above the well-mixed atmosphere. The transition from CO2 to O-dominated region is observed near 270 km. The mean exospheric temperature derived using these three mass numbers is 271 ± 5 K. These first observations corresponding to the Martian evening hours would help to provide constraints to the thermal escape models.
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- 2016
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5. Solar plasma wave studies at L1 point with magnetic field measurements from magnetometers
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Shefin Shoukath, A. Rasul Muthu, and Vipin K. Yadav
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Physics ,010504 meteorology & atmospheric sciences ,Magnetometer ,Waves in plasmas ,Magnetosphere ,Dipole model of the Earth's magnetic field ,Geodesy ,01 natural sciences ,law.invention ,Computational physics ,Magnetic field ,Physics::Plasma Physics ,law ,Physics::Space Physics ,0103 physical sciences ,Interplanetary magnetic field ,Mercury's magnetic field ,010303 astronomy & astrophysics ,Magnetosphere particle motion ,0105 earth and related environmental sciences - Abstract
Fluxgate Magnetometers (FGM) are regularly sent onboard space missions to measure the local magnetic field magnitude. These magnetic field measurements are one of the methods used to study the plasma wave parameters. The plasma waves emanating from a plasma environment carries the history of their generation mechanism with them. Plasma waves can also provide information about various physical phenomena which take place locally in and around the Sun where the in-situ measurements are not possible due to extreme and hostile conditions. For solar plasma waves study, the first Lagrangian point (L1) is an excellent location as it is far off from the solar plasma environment as well as from Earth's magnetosphere. There are many spacecrafts sent at L1 point to study the scientific aspects of Sun. However only WIND and ACE were two missions which carried the magnetic field measurement instruments such as the FGM to measure the steady state magnetic field environment at L1 point. The FGMs onboard these two spacecrafts collects magnetic field data at very finite intervals to extract scientific information. Magnetic field data from FGM can be used to detect the solar plasma waves (primarily Alfven) at L1 point to estimate their wave properties.
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- 2016
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6. Fresnel zone plate telescopes for X-ray imaging II: numerical simulations with parallel and diverging beams
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Sourav Palit, Vipin K. Yadav, Sandip K. Chakrabarti, V. Girish, A. Nandi, Dipak Debnath, and A. R. Rao
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Physics ,Basis (linear algebra) ,business.industry ,Galactic Center ,Resolution (electron density) ,Solid angle ,FOS: Physical sciences ,Astronomy and Astrophysics ,Zone plate ,law.invention ,Telescope ,Optics ,Space and Planetary Science ,law ,Satellite ,Astrophysics - Instrumentation and Methods for Astrophysics ,business ,Instrumentation and Methods for Astrophysics (astro-ph.IM) ,Beam (structure) - Abstract
We present the results of simulations of shadows cast by a zone plate telescope which may have one to four pairs of zone plates. From the shadows we reconstruct the images under various circumstances. We discuss physical basis of the resolution of the telescope and demonstrate this by our simulations. We allow the source to be at a finite distance (diverging beam) as well as at an infinite distance (parallel beam) and show that the resolution is worsened when the source is nearby. By reconstructing the zone plates in a way that both the zone plates subtend the same solid angles at the source, we obtain back high resolution even for sources at a finite distance. We present simulated results for the observation of the galactic center and show that the sources of varying intensities may be reconstructed with accuracy. Results of these simulations would be of immense use in interpreting the X-ray images from recently launched CORONAS-PHOTON satellite., Comment: 17 pages, 36 figures, Published in Experimental Astronomy
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- 2009
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7. Fresnel zone plate telescopes for X-ray imaging I: experiments with a quasi-parallel beam
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Dipak Debnath, Ritabrata Sarkar, Sourav Palit, Sandip K. Chakrabarti, Vipin K. Yadav, and A. Nandi
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Parallel beam ,Materials science ,Fresnel zone ,business.industry ,Astrophysics::High Energy Astrophysical Phenomena ,Astrophysics::Instrumentation and Methods for Astrophysics ,X-ray ,FOS: Physical sciences ,chemistry.chemical_element ,Astronomy and Astrophysics ,Zone plate ,Tungsten ,law.invention ,Telescope ,Optics ,chemistry ,Space and Planetary Science ,law ,Deconvolution ,Astrophysics - Instrumentation and Methods for Astrophysics ,business ,Instrumentation and Methods for Astrophysics (astro-ph.IM) ,Beam (structure) - Abstract
Combination of Fresnel Zone Plates (FZP) can make an excellent telescope for imaging in X-rays. We present here the results of our experiments with several pairs of tungsten made Fresnel Zone plates in presence of an X-ray source kept at a distance of about 45 feet. The quasi-parallel beam allowed us to study sources placed on the axis as well as off the axis of the telescope. We present theoretical study of the fringe patterns produced by the zone plates in presence of a quasi-parallel source. We compare the patterns obtained from experiments with those obtained by our Monte-Carlo simulations. The images are also reconstructed by deconvolution from both the patterns. We compare the performance of such a telescope with other X-ray imaging devices used in space-astronomy., 16 pages, 24 figures, published in Experimental Astronomy
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- 2009
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8. Test and Commissioning of 82.6 GHz ECRH system on SST-1
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B.R. Kadia, P.L. Khilar, D. Bora, P. Dharmesh, Manoj Kumar Singh, Mikhail Shmelev, A.R. Makwana, P. Biswas, V. I. Belousov, Chetan, K. G. Parmar, Kumar Rajnish, Y.S.S. Srinivas, P. Kirit, Rajan Babu, E. M. Tai, P. Jatin, B. K. Shukla, R. Sugandhi, V. Kurbatov, Yu. Belov, Jignesh Soni, Vipin K. Yadav, Mahesh Kushwah, K. Sathyanarayana, M. Harsha, G. Agrajit, Prabal K. Chattopadhyay, Harshida Patel, and D. Pragnesh
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Dummy load ,History ,Engineering ,Tokamak ,business.industry ,Electrical engineering ,Fault (power engineering) ,Computer Science Applications ,Education ,law.invention ,law ,Duty cycle ,Transmission line ,SST-1 ,Gyrotron ,business ,Interlock - Abstract
Electron Cyclotron Resonance Heating (ECRH) system will play an important role in plasma formation, heating and current drive in the Superconducting Steady state Tokamak (SST-1). Commissioning activity of the machine has been initiated. Many of the sub-systems have been prepared for the first plasma discharge. A radial and a top port have been allotted for low field side (LFS) and high field side (HFS) launch of O and X- modes in the plasma. The system is based on a gyrotron source operating at a frequency of 82.6±0.1GHz (GLGD-82.6/0.2) and capable of delivering 0.2 MW / 1000s with 17% duty cycle. The transmission line consisting of ~15 meters length 63.5mm corrugated wave guide, DC break, wave guide switch, mitre bend, polariser, bellows that terminates with a vacuum barrier CVD window. A beam launching system used to steer the microwave beam in the plasma volume is connected between the end of the transmission line and the tokamak radial and top ports. A VME based real time data acquisition and control (DAC) system is used for monitoring, acquisition and control. Hard-wired interlock operates a rail-gap based crowbar system in less than 10µs under any fault condition. Burn patterns are recorded at various stages in the transmission line. The gyrotron is tested for ~200 kW / 1000s operation on a water dummy load. Transmission line is tested at various power levels for long pulse operation. The paper highlights the experimental results of successful commissioning of the system.
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- 2005
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9. Ultrasoft x-ray emission from a linear ECR plasma source
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Vipin K Yadav and D. Bora
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Waveguide (electromagnetism) ,Range (particle radiation) ,Hydrogen ,Astrophysics::High Energy Astrophysical Phenomena ,chemistry.chemical_element ,Plasma ,Condensed Matter Physics ,Electron cyclotron resonance ,Photodiode ,law.invention ,Magnetic field ,chemistry ,Physics::Plasma Physics ,law ,Cavity magnetron ,Atomic physics - Abstract
Ultrasoft x-ray emission in the energy range 10–100 eV is observed from a linear electron cyclotron resonance (ECR) plasma system. ECR plasma is produced in a short cylindrical stainless steel (SS) chamber with a central axial magnetic field of 875 G, generated by two coils placed axially to have the first two ECR surfaces inside the experimental chamber. Plasma is produced in a pressure range of 2 × 10−5 mbar with hydrogen. Also, plasma is produced with net microwave power varying from 160 to 800 W at 2.45 GHz frequency from a magnetron. The waveguide from the magnetron to the vacuum vessel supports rectangular TE10 mode and the electromagnetic wave propagation in plasma is in extraordinary (X) mode. The ultrasoft x-ray emission is observed with a vacuum photodiode. The results clearly indicate a decrease in x-ray emission on increasing the working pressure and an increase in emission with an increase in the input microwave power. The experiments also ensure that the presence of a metal target enhances the intensity of soft x-rays generated in the ECR plasma system.
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- 2004
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10. Instruments of RT-2 Experiment onboard CORONAS-PHOTON and their test and evaluation III: Coded Aperture Mask and Fresnel Zone Plates in RT-2/CZT Payload
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Roni Sarkar, Vipin K. Yadav, Dipak Debnath, Anuj Nandi, Sandip K. Chakrabarti, Sourav Palit, V. Girish, A. R. Rao, T. B. Kotoch, and Dipankar Bhattacharya
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Physics ,Photon ,Fresnel zone ,business.industry ,Physics::Instrumentation and Detectors ,Detector ,Payload (computing) ,Astrophysics::Instrumentation and Methods for Astrophysics ,FOS: Physical sciences ,Astronomy and Astrophysics ,Zone plate ,law.invention ,Optics ,CMOS ,Space and Planetary Science ,law ,Angular resolution ,Coded aperture ,business ,Astrophysics - Instrumentation and Methods for Astrophysics ,Instrumentation and Methods for Astrophysics (astro-ph.IM) - Abstract
Imaging in hard X-rays of any astrophysical source with high angular resolution is a challenging job. Shadow-casting technique is one of the most viable options for imaging in hard X-rays. We have used two different types of shadow-casters, namely, Coded Aperture Mask (CAM) and Fresnel Zone Plate (FZP) pair and two types of pixellated solid-state detectors, namely, CZT and CMOS in RT-2/CZT payload, the hard X-ray imaging instrument onboard the CORONAS-PHOTON satellite. In this paper, we present the results of simulations with different combinations of coders (CAM & FZP) and detectors that are employed in the RT-2/CZT payload. We discuss the possibility of detecting transient Solar flares with good angular resolution for various combinations. Simulated results are compared with laboratory experiments to verify the consistency of the designed configuration., 27 pages, 16 figures, Accepted for publication in Experimental Astronomy (in press)
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- 2010
11. A tetrode based fast pulsed microwave source for electron cyclotron resonance breakdown experiments
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D. Bora, D. Purohit, K. Sathyanarayana, and Vipin K. Yadav
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Materials science ,business.industry ,Vacuum tube ,Astrophysics::Cosmology and Extragalactic Astrophysics ,Plasma ,Electron cyclotron resonance ,law.invention ,symbols.namesake ,Nuclear magnetic resonance ,Fall time ,Physics::Plasma Physics ,law ,Rise time ,Cavity magnetron ,symbols ,Optoelectronics ,Langmuir probe ,business ,Instrumentation ,Microwave - Abstract
To study electron cylotron resonance (ECR) breakdown and afterglow plasma in an experimental linear plasma system, a pulsed microwave source with rapid rise and fall of microwave power is desired. A pulsed microwave source with fast rise and fall capability for ECR breakdown experiments has been designed and tested for performance in the system. A tetrode, controlled by a modulator card, is used as a fast switch to initiate microwave power from a conventional magnetron operating at 2.45 GHz. The typical rise time of microwave power is approximately 3 micros and a fall time of approximately 10 micros. Using this scheme in a realistic pulsed microwave source at 800 W power, ECR breakdown of neutral gas is achieved and the plasma delay and fall time are observed from the plasma density measurements using a Langmuir probe. The design details of the fast rise pulsed microwave source are presented in this article with initial experimental results.
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- 2007
12. MENCA experiment aboard India’s Mars Orbiter Mission
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M. B. Dhanya, Anil Bhardwaj, P. Pradeepkumar, S. V. Mohankumar, A. V. Aliyas, P. Sreelatha, Gogulapati Supriya, Neha Naik, B. Sundar, Tirtha Pratim Das, Amarnath Nandi, Dinakar Prasad Vajja, R. Satheesh Thampi, G. Padma Padmanabhan, and Vipin K. Yadav
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Martian ,Orbiter ,Multidisciplinary ,law ,Analyser ,Calibration ,Orbit (dynamics) ,Environmental science ,Mars Exploration Program ,Quadrupole mass analyzer ,Astrobiology ,law.invention ,Exosphere - Abstract
The Mars Exospheric Neutral Composition Analyser (MENCA) aboard the Indian Mars Orbiter Mission (MOM) is a quadrupole mass spectrometer-based experiment. Making use of the highly elliptical and low inclination (~150°) orbit of MOM, MENCA will conduct in situ measurements of the composition and radial distribution of the Martian neutral exosphere in the 1–300 amu mass range in the equatorial and low latitudes of Mars. The functionality of MENCA has been tested during the Earth-bound and heliocentric phases of MOM before its operation in the Martian orbit. This article describes the scientific objectives, instrument details, design and development, test and evaluation, and calibration of the MENCA instrument.
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- 2015
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