Numerical Analysis of Performance of DF Chemical Laser With a Radial-Expansion Nozzle Array According to D2 Injection Angles

Volume 1 ◽  
2004 ◽  
Author(s):  
Jun Sung Park ◽  
Seung Wook Baek

It is chemical laser system that can be used for not only new strategic weapon system for the military purpose, but also a manufacturing tool in industrial areas due to the characteristic of high power laser beam in megawatt range. In order to increase laser beam power in the chemical laser system, mixing efficiency of fuel and oxidant should be higher and more excited molecules be produced by mean of chemical reaction. Basically, the production of a lot of excited molecules in the laser cavity results from the high mass flow rates of fuel and oxidant as well as high mixing and reaction efficiencies, however, it is difficult for the planar nozzle array which has been widely used until now to supply high mass flow to the chemical laser cavity. A radial expansion nozzle array as an innovated alternative of the planar nozzle system is designed. The laser beam generation in this system is achieved by mixing F atom from supersonic nozzle and D2 molecule from the holes of round-bended supply line which are distributed with zigzag configuration, hence the reaction surface will be stretched. Consequently, it is expected that more excited molecules will be produced and population inversion also be higher. Based on that the fuel injection angle with mainstream has a big influence of performance of supersonic combustor, the effects of D2 injection angles with the main F flow on mixing enhancement and laser beam power are numerically investigated. The results are discussed by comparison with three cases of D2 injection angles; 10°, 20° and 40° with the main flow direction. Major results reveal that the area where the DF(1) excited molecules as a representative product in the DF chemical laser system are produced becomes larger when the D2 injection angle increases. The reason is that the surface of chemical reaction is larger and the field temperature is higher with increase of the D2 injection angle. And in all the vibrational transitions, the distributions of the highest maximum small signal gains are observed near the inlet when the D2 injection angle is 40°. As the D2 injection angle increases, the values of the maximum SSG are higher and the area including the high gains is also wider for the most part of domain. Based on these maximum SSG distributions, the highest power of laser beam is expected to be generated when the D2 injection angle is 40°, namely higher. However, the range of population inversion becomes narrower as the D2 injection angle increases, because the collision of molecules or atoms happens more often so that the relaxation time will be reduced as the cavity pressure caused by the high D2 injection angle with the main flow direction increases.

2012 ◽  
Vol 36 (3) ◽  
pp. 241-258 ◽  
Author(s):  
Purushothaman Dinesh Babu ◽  
Gengusamynaidu Buvanashekaran ◽  
Karupuudaiyar R. Balasubramanian

An experimental investigation with Nd:YAG laser system was carried out to study the effects of laser hardening process parameters on the microstructure and hardness during laser hardening of EN25 steel. The laser beam is allowed to scan on the surface of the work piece by varying the laser beam power (750–1250 W) and travel speed (500–1000 mm/min) of the work table. The microstructural features of the laser hardened EN25 steel were analysed using optical microscope. The microstructure of the surface layer was found to consist of plate martensite. A substantial increase in surface hardness was achieved, by a factor of 2 times the base material hardness.


2013 ◽  
Vol 740-742 ◽  
pp. 773-776 ◽  
Author(s):  
A. Hürner ◽  
T. Schlegl ◽  
B. Adelmann ◽  
H. Mitlehner ◽  
R. Hellmann ◽  
...  

In this study, we present the results of alloying nickel as ohmic contact material to n-type 4H-SiC via a continuous wave fiber laser with different laser beam powers and processing times. The laser system exhibits an emitting wavelength of 1070 nm and a beam propagation factor M2 smaller than 1.1. Contact resistance was determined by current-voltage measurement using the two-terminal contact resistance method. The results indicate that a laser beam power of at least 100 W is mandatory to initialize contact silicidation. Although the contact resistance is improvable by longer processing times, our experiments outline the much higher impact of laser beam power to contact silicidation compared with processing time. For laser beam powers of 300 W and processing times of 0.5 s a contact resistance of 6.5 , comparable to contacts alloyed in a lamp heated furnace at 910 °C for 2 min with a contact resistance of 10.3 , was achieved.


2015 ◽  
Vol 828-829 ◽  
pp. 298-304
Author(s):  
Stefan Riekehr ◽  
Riccardo Ravasi ◽  
Josephin Enz ◽  
Volker Ventzke ◽  
Nikolai Kashaev

In the present work the mechanical behaviour of laser beam welded AZ31B alloy was studied, by changing systematically the spot size of the used fibre laser system between 200 µm and 1000 µm at different power levels between 2 kW and 8 kW. Maximum welding velocities with respect to imperfections were determined. The characterization of the obtained welds - in terms of Vickers hardness, UTS, Af and weld width, resp. weld area - was correlated with the micro-texture in dependence of the different Focus Spot Diameters and Laser Beam Power levels as well as the resulting cooling rates. Highest UTS of 94% of the base material was achieved with 200 µm Focus Spot Diameter and Laser Beam Power of 4 kW at welding velocity of 100 mm/s. By increasing the Focus Spot Diameter to 600 µm, the tensile strength was reduced to 86 % of the actual strength of the base material.


Author(s):  
V. Laguzzi ◽  
F. Molinaro ◽  
B. Natan

The scope of the study is to evaluate the combustion efficiency of a ducted rocket combustor operating at different conditions, using a connected-pipe testing setup. An experimental parametric investigation was conducted to evaluate the effect of the inlet air-injection angles and the effect of the combustion pressure for different fuel-to-air ratios. The experimental results indicate that best energetic performance was obtained for an injection angle of 120°, i. e., against the main flow direction. The reason is that this way better mixing was obtained and the residence time increased. Characteristic velocity was found to decrease with decreasing the combustion pressure.


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