What is the derivation of the Rankine Hugoniot relations in fluid dynamics?

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The discussion focuses on the derivation of the Rankine Hugoniot relations in fluid dynamics, specifically addressing the conservation equations across normal discontinuities. The equations presented involve the density, pressure, and velocity components of the fluid, represented as \rho_1, p_1, and \vec{v_1} for the first state, and \rho_2, p_2, and \vec{v_2} for the second state. The unit vector \vec{n} is defined as normal to the discontinuity, and the discussion highlights the importance of understanding vector algebra in this context.

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steem84
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Hello,

See picture, I do not understand one step w.r.t. to the derivation of the Rankine Hugoniot relations (fluid dynamics): how does one get the second function from the first function? I think I am missing some vector algebra here..
 

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is ud the component of u in the direction of nd or in the tangential direction to the discontinuity? (I suppose nd is normal to the discontinuity?)

Usually the conservation equations across normal discontinuities are what are known as the Rankine Hugoniot equations. For an oblique discontinuity the conservation of energy (assuming Re>>1) would be:

\rho_1 (e+v_1^2/2)\vec{v_1} \cdot \vec{n} + p_1\vec{v_1} \cdot \vec{n} = \rho_2 (e+v_2^2/2)\vec{v_2} \cdot \vec{n} + p_2\vec{v_2} \cdot \vec{n}

where \vec{n} is the unit vector normal to the discontinuity.
 

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