The thermally insulated vessel contains an ideal gas of molecular mass M and ratio of specific heat . It is moving with speed v and is suddenly brought to rest. Assuming no heat is lost to the surroundings, its temperature increases by :
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\(\frac{1}{2}M{\nu ^2} = {C_v}.\Delta T\)
\(\frac{1}{2}M{\nu ^2} = \frac{R}{{\gamma - 1}}.\Delta T\)
\(\Delta T = \frac{{M{\nu ^2}(\gamma - 1)}}{{2R}} = \frac{{(\gamma - 1)M{\nu ^2}}}{{2R}}\)