When an ideal diatomic gas is heated at constant pressure, the fraction of the heat energy supplied which increases the internal energy of the gas, is
IIT 1990, Medium
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(d) Fraction of supplied energy which in creases the internal energy is given by
$f = \frac{{\Delta U}}{{{{(\Delta Q)}_P}}} = \frac{{{{(\Delta Q)}_V}}}{{{{(\Delta Q)}_P}}} = \frac{{\mu {C_V}\Delta T}}{{\mu {C_P}\Delta T}} = \frac{1}{\gamma }$
For diatomic gas $\gamma = \frac{7}{5}$==> $f = \frac{5}{7}$
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