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Molecular Physics and Hypersonic Flows

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where, as previously, Tv is a phenomenological vibrational relaxation time. Thus, at the first order we obtain a "weak” nonequilibrium given by Eq. (26).

Conservation Equations and Physical Models for Hypersonic ...

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Thus , T Tv hs = ( Cp , t + Co , r ) dT ' + CodT ' Tref Tref Те + Cp , edT ' + h8,0 ( 32 ) Tref C. ( Tv ) = C ) ( TV ) - C.-C. ( 29 ) V V " Ugr where T ' is ...

Super- and Hypersonic Aerodynamics and Heat Transfer

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Karasev, A. B. and Kondranin, T. V., 1973. Some aspects of heat transfer in a hypersonic shock layer with ablation effects, ANMZ, No. 3, pp. 135-143.

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where, as previously, Tv is a phenomenological vibrational relaxation time. Thus, at the first order we obtain a "weak” nonequilibrium given by Eq. (26).

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where, as previously, Tv is a phenomenological vibrational relaxation time. Thus, at the first order we obtain a "weak” nonequilibrium given by Eq. (26).

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where, as previously, Tv is a phenomenological vibrational relaxation time. Thus, at the first order we obtain a "weak” nonequilibrium given by Eq. (26).

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where, as previously, Tv is a phenomenological vibrational relaxation time. Thus, at the first order we obtain a "weak” nonequilibrium given by Eq. (26).

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where, as previously, Tv is a phenomenological vibrational relaxation time. Thus, at the first order we obtain a "weak” nonequilibrium given by Eq. (26).

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where, as previously, Tv is a phenomenological vibrational relaxation time. Thus, at the first order we obtain a "weak” nonequilibrium given by Eq. (26).

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where, as previously, Tv is a phenomenological vibrational relaxation time. Thus, at the first order we obtain a "weak” nonequilibrium given by Eq. (26).

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where, as previously, Tv is a phenomenological vibrational relaxation time. Thus, at the first order we obtain a "weak” nonequilibrium given by Eq. (26).

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where, as previously, Tv is a phenomenological vibrational relaxation time. Thus, at the first order we obtain a "weak” nonequilibrium given by Eq. (26).

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where, as previously, Tv is a phenomenological vibrational relaxation time. Thus, at the first order we obtain a "weak” nonequilibrium given by Eq. (26).

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where, as previously, Tv is a phenomenological vibrational relaxation time. Thus, at the first order we obtain a "weak” nonequilibrium given by Eq. (26).

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where, as previously, Tv is a phenomenological vibrational relaxation time. Thus, at the first order we obtain a "weak” nonequilibrium given by Eq. (26).

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where, as previously, Tv is a phenomenological vibrational relaxation time. Thus, at the first order we obtain a "weak” nonequilibrium given by Eq. (26).

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where, as previously, Tv is a phenomenological vibrational relaxation time. Thus, at the first order we obtain a "weak” nonequilibrium given by Eq. (26).

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where, as previously, Tv is a phenomenological vibrational relaxation time. Thus, at the first order we obtain a "weak” nonequilibrium given by Eq. (26).

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where, as previously, Tv is a phenomenological vibrational relaxation time. Thus, at the first order we obtain a "weak” nonequilibrium given by Eq. (26).

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where, as previously, Tv is a phenomenological vibrational relaxation time. Thus, at the first order we obtain a "weak” nonequilibrium given by Eq. (26).

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where, as previously, Tv is a phenomenological vibrational relaxation time. Thus, at the first order we obtain a "weak” nonequilibrium given by Eq. (26).

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where, as previously, Tv is a phenomenological vibrational relaxation time. Thus, at the first order we obtain a "weak” nonequilibrium given by Eq. (26).

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where, as previously, Tv is a phenomenological vibrational relaxation time. Thus, at the first order we obtain a "weak” nonequilibrium given by Eq. (26).

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where, as previously, Tv is a phenomenological vibrational relaxation time. Thus, at the first order we obtain a "weak” nonequilibrium given by Eq. (26).

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where, as previously, Tv is a phenomenological vibrational relaxation time. Thus, at the first order we obtain a "weak” nonequilibrium given by Eq. (26).

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where, as previously, Tv is a phenomenological vibrational relaxation time. Thus, at the first order we obtain a "weak” nonequilibrium given by Eq. (26).

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where, as previously, Tv is a phenomenological vibrational relaxation time. Thus, at the first order we obtain a "weak” nonequilibrium given by Eq. (26).

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where, as previously, Tv is a phenomenological vibrational relaxation time. Thus, at the first order we obtain a "weak” nonequilibrium given by Eq. (26).

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