Measurement of hydrazine gas generator performance by gas chromatography.

Abstract

561g Q '(t, oo) = (l/u e ) dwjdt ; 0 2 '({, (») = 0 0 0 K.°o)=l; 02(£oo) = 0 3 « f oo) = 0 and at the wall, /o'«. 0) =/ 2 '«, 0) =/,'«, 0) = 0 0o'«.0) = 0; 0 2 '(£,0)=1 0&.0) = TJT e ; 0 2 (£,0) = 0 3 (£,0) = 0 ExampleAs a numerical example Eqs. (4) and (6) were solved for a spinning 11-cm-diam tangent-ogive cylinder at a Mach number of 3.0 and at 4.0° incidence 5 by the techniques described in Ref. 6. Typical results for one axial body station are summarized in Figs. 1 and 2. The results indicate that there is very little modification of the tangential velocity profiles and the temperature profiles for spin parameters within the range of validity of perturbation analysis. This is in general agreement with the experimental results of Ref. 5.