This paper presents the electromagnetic wave propagation characteristics in plasma and the attenuation coefficients of the microwave in terms of the parameters n_e,v,ω,L,ω_b.The φ800 mm high temperature shock tube ...This paper presents the electromagnetic wave propagation characteristics in plasma and the attenuation coefficients of the microwave in terms of the parameters n_e,v,ω,L,ω_b.The φ800 mm high temperature shock tube has been used to produce a uniform plasma.In order to get the attenuation of the electromagnetic wave through the plasma behind a shock wave,the microwave transmission has been used to measure the relative change of the wave power.The working frequency is f=(2~35)GHz(ω=2πf,wave length λ=15 cm~8 mm).The electron density in the plasma is n_e=(3×10^(10)~1×10^(14))cm^(-3).The collision frequency v=(1×10~8~6×10^(10))Hz.The thickness of the plasma layer L=(2~80)cm.The electron circular frequency ω_b=eBo/m_e,magnetic flux density B_0=(0~0.84)T.The experimental results show that when the plasma layer is thick (such as L/λ(?)10),the correlation between the attenuation coefficients of the electromagnetic waves and the parameters n_e,v,ω,L determined from the measurements are in good agreement with the theoretical predictions of electromagnetic wave propagations in the uniform infinite plasma.When the plasma layer is thin(such as when both L and λ are of the same order),the theoretical results are only in a qualitative agreement with the experimental observations in the present parameter range, but the formula of the electromagnetic wave propagation theory in an uniform infinite plasma can not be used for quantitative computations of the correlation between the attenuation coefficients and the parameters n_e,v,ω,L.In fact,if ω<ω_p,v^2(?)ω~2,the power attenuations K of the electromagnetic waves obtained from the measurements in the thin-layer plasma are much smaller than those of the theoretical predictions.On the other hand,if ω>ω_p,v^2(?)ω~2(just v≈f),the measurements are much larger than the theoretical results.Also,we have measured the electromagnetic wave power attenuation value under the magnetic field and without a magnetic field.The result indicates that the value measured under the magnetic field shows a distinct improvement.展开更多
The experimental results for the excited time of the nonequlibrium radiation andthe ionization behind strong shock waves are presented. Using an optical multichannel analyzer, InSb infrared detectors and near-free-mol...The experimental results for the excited time of the nonequlibrium radiation andthe ionization behind strong shock waves are presented. Using an optical multichannel analyzer, InSb infrared detectors and near-free-molecular Langmuir probes, the infrared radiation, the electron density of air and the nonequlibrium radiation spectra at different moments of the relaxation process in nitrogen test gas behind normal shock waves were obtained, respectively, in hydrogen oxygen combustion driven shock tubes.展开更多
基金The project supported by the National Natural Science Foundation of China (19982005 and 10032050) and the National Defense Science Foundation of China
文摘This paper presents the electromagnetic wave propagation characteristics in plasma and the attenuation coefficients of the microwave in terms of the parameters n_e,v,ω,L,ω_b.The φ800 mm high temperature shock tube has been used to produce a uniform plasma.In order to get the attenuation of the electromagnetic wave through the plasma behind a shock wave,the microwave transmission has been used to measure the relative change of the wave power.The working frequency is f=(2~35)GHz(ω=2πf,wave length λ=15 cm~8 mm).The electron density in the plasma is n_e=(3×10^(10)~1×10^(14))cm^(-3).The collision frequency v=(1×10~8~6×10^(10))Hz.The thickness of the plasma layer L=(2~80)cm.The electron circular frequency ω_b=eBo/m_e,magnetic flux density B_0=(0~0.84)T.The experimental results show that when the plasma layer is thick (such as L/λ(?)10),the correlation between the attenuation coefficients of the electromagnetic waves and the parameters n_e,v,ω,L determined from the measurements are in good agreement with the theoretical predictions of electromagnetic wave propagations in the uniform infinite plasma.When the plasma layer is thin(such as when both L and λ are of the same order),the theoretical results are only in a qualitative agreement with the experimental observations in the present parameter range, but the formula of the electromagnetic wave propagation theory in an uniform infinite plasma can not be used for quantitative computations of the correlation between the attenuation coefficients and the parameters n_e,v,ω,L.In fact,if ω<ω_p,v^2(?)ω~2,the power attenuations K of the electromagnetic waves obtained from the measurements in the thin-layer plasma are much smaller than those of the theoretical predictions.On the other hand,if ω>ω_p,v^2(?)ω~2(just v≈f),the measurements are much larger than the theoretical results.Also,we have measured the electromagnetic wave power attenuation value under the magnetic field and without a magnetic field.The result indicates that the value measured under the magnetic field shows a distinct improvement.
文摘The experimental results for the excited time of the nonequlibrium radiation andthe ionization behind strong shock waves are presented. Using an optical multichannel analyzer, InSb infrared detectors and near-free-molecular Langmuir probes, the infrared radiation, the electron density of air and the nonequlibrium radiation spectra at different moments of the relaxation process in nitrogen test gas behind normal shock waves were obtained, respectively, in hydrogen oxygen combustion driven shock tubes.