Gaurav Singhal
Defence Research and Development Organisation
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Publication
Featured researches published by Gaurav Singhal.
Infrared Physics & Technology | 2003
R.K. Tyagi; R. Rajesh; Gaurav Singhal; Mainuddin; A.L. Dawar; Masamori Endo
Chemical oxygen-iodine laser (COIL) having a wavelength of 1.315 μm has been developed using a singlet oxygen generator (SOG) with a novel approach. Generated singlet oxygen is taken out of the SOG at an angle of 40° to avoid the problem of carry over of droplets, which is one of the major drawbacks of horizontal systems. The system has been operated using uncooled nitrogen as a buffer gas. The paper reports the results on the studies carried out on this COIL system. Under optimum conditions, we have been able to achieve stable and reproducible output power of 350 W for a chlorine flow rate of 22 mmol/s thus yielding a chemical efficiency of 17.5%.
Optics and Laser Technology | 2003
R.K. Tyagi; R. Rajesh; Gaurav Singhal; Mainuddin; A.L. Dawar; Masamori Endo
Abstract Supersonic Chemical Oxy-iodine Laser has been developed using a Singlet Oxygen Generator (SOG) with a novel approach. Generated singlet oxygen is taken out of the SOG at an angle of 40° to avoid the problem of carry over of droplets, which is one of the major drawbacks of horizontal system. The system has been operated up to 22 mmol/s chlorine flow rates. Chlorine utilization and singlet oxygen observed have been more than 90% and 60%, respectively. The observed maximum output power was 350 W , thus yielding a chemical efficiency of 17.5%.
High-power lasers and applications | 2003
R.K. Tyagi; R. Rajesh; Gaurav Singhal; Mainuddin; A.L. Dawar; Masamori Endo
Singlet Oxygen Generator ( SOG ) with a novel approach has been designed and fabricated. Singlet oxygen is taken out of the SOG at an angle of 40° thus avoiding the carry over of droplets, which is one of the major drawbacks of horizontal system. The paper discusses various design parameters for such type of SOG. For flow rates of chlorine up to 22 mmol/sec, the chlorine utilization and singlet oxygen yield have been observed to be ~ 90% and ~64% respectively.
International Journal of Infrared and Millimeter Waves | 2004
R. Rajesh; M. Hussain; Z. H. Zaidi; R.K. Tyagi; Gaurav Singhal; Mainuddin; A.L. Dawar; Masamori Endo
Chemical oxygen-iodine Laser (COIL) is one of the fast emerging high power laser source for near Infrared (λ=1.315μm) laser generation. The heart of the system is the singlet oxygen generator (SOG) which is a pumping source for this laser. A Jet type SOG with a novel approach was designed and fabricated. Singlet oxygen was taken out of the SOG at an angle of 40° thus avoiding the carry over of droplets, which is one of the major drawbacks of horizontal system. The preliminary results have been reported in our earlier publication. The present paper discusses the performance of this generator for various operational conditions viz. diluents gas nitrogen / helium, basic hydrogen peroxide composition, generator pressure and gas velocity. Further, conditions for the stable operation from generator as well as chlorine injection point of view have been identified.
Thermophysics and Aeromechanics | 2017
Gaurav Singhal; P.M.V. Subbarao; Mainuddin; R.K. Tyagi; A.L. Dawar
A class of flowing medium gas lasers with low generator pressures employ supersonic flows with low cavity pressure and are primarily categorized as high throughput systems capable of being scaled up to MW class. These include; Chemical Oxygen Iodine Laser (COIL) and Hydrogen (Deuterium) Fluoride (HF/DF). The practicability of such laser systems for various applications is enhanced by exhausting the effluents directly to ambient atmosphere. Consequently, ejector based pressure recovery forms a potent configuration for open cycle operation. Conventionally these gas laser systems require at least two ejector stages with low pressure stage being more critical, since it directly entrains the laser media, and the ensuing perturbation of cavity flow, if any, may affect laser operation. Hence, the choice of plausible motive gas injection schemes viz., peripheral or central is a fluid dynamic issue of interest, and a parametric experimental performance comparison would be beneficial. Thus, the focus is to experimentally characterize the effect of variation in motive gas supply pressure, entrainment ratio, back pressure conditions, nozzle injection position operated together with a COIL device and discern the reasons for the behavior.
Archive | 2017
A. K. Varshney; Avinash C. Verma; Gaurav Singhal; Mainuddin; R.K. Tyagi
The present paper discusses laser kinetic modeling of diode pumped flowing medium aprotic liquid laser containing Nd3+ ions in POCl3 solvent host. Transverse pumping has been examined, which is ideal from point of view of laser scalability to higher power levels. In the computations, spectroscopic parameters of aprotic solution having an Nd3+ ion concentration of 0.3 M have been considered and numerical calculations were performed for analyzing the effect of various parameters including; active ion concentration, gain medium length, absorption depth, output coupler transmission and input pump power on laser output and efficiency. The results indicate that nearly 1.5 kW laser output may be obtained for an input pump power of 5.0 kW with a slope efficiency of nearly 31% having a threshold pump power requirement of 300 W for a given cell length of 15 cm. Hence, a set of optimized parameters have been obtained for designing an efficient transversely diode pumped kW level flowing liquid laser.
IEEE Sensors Journal | 2015
Gaurav Singhal; Mainuddin; Raghvan Rajesh; Mirza Tariq Beg; R.K. Tyagi; Avinashi Lal Dawar
High-power lasers typically form a multidisciplinary technological area laced with innumerable challenges in its realization as a practical system. The prime amongst them are infrared gas laser sources, such as carbon dioxide gas dynamic laser, hydrogen fluoride, deuterium fluoride laser, and chemical oxygen iodine laser. Each of these laser systems is associated with a unique as well as complex active medium environment involving intense interaction between lasing and pumping species under specific gas dynamic conditions. The parameters viz., specie concentration of the lasing, pumping mediums and other by-products, medium homogeneity, individual constituent gas flow rate, pressure and temperature at critical locations, and cavity Mach number are very crucial in determining the output of the gas laser system. It is essential to determine these parameters nonintrusively, with necessary precision so as to optimize these lasers especially in case of large-scale systems. Thus, the focus of this paper is to review and discuss the existing applicable optical detection methodologies ranging from the more established methods, such as optical absorption/emission spectroscopy, to very contemporary, such as Raman spectroscopy, cavity ring down spectroscopy, laser-induced fluorescence/planer laser-induced fluorescence, and so on, which are relevant for the diagnostic needs of gas lasers.
Proceedings of SPIE, the International Society for Optical Engineering | 2005
Gaurav Singhal; R. Rajesh; Mainuddin; R.K. Tyagi; A.L. Dawar; P.M.V. Subbarao; Masamori Endo
An advanced nozzle, also known as ejector nozzle, suitable for a 500 W class COIL employing an active medium flow of nearly 12 gm/s has been developed and used instead of conventional slit nozzle. The nozzle has been tested in both cold as well as hot run conditions of COIL achieving a typical cavity pressure of nearly 10 torr, pitot pressure of ~ 85 torr and a cavity Mach number of ~2.5. The present study details the gas dynamic aspects and detailed numerical studies of this ejector nozzle and highlights its potential as a COIL pressure recovery device. This nozzle in conjunction with a diffuser is capable of achieving pressure recovery of ~ 60 torr, equivalent to the much cumbersome first stage of the pressure recovery system used in case of conventional slit nozzle based system. . Thus use of this nozzle in place of conventional slit nozzle can achieve the atmospheric discharge using single stage ejector system thereby making the pressure recovery system quite compact.
Optics and Laser Technology | 2010
Gaurav Singhal; Mainuddin; R.K. Tyagi; A.L. Dawar; P.M.V. Subbarao
Experimental Thermal and Fluid Science | 2006
Gaurav Singhal; R. Rajesh; Mainuddin; R.K. Tyagi; A.L. Dawar; P.M.V. Subbarao; Masamori Endo