For an ideal gas, applying the First Law of Thermodynamics tells us that heat is also equal to:
"Q = \u0394E_{int} + W"
"W=0" at constant volume.
For a monatomic ideal gas we showed that
"\u0394E_{int} = (3\/2)nR\u0394T"
Comparing our two equations;
"Q = nC_V\u0394T" and "Q = (3\/2)nR\u0394T"
we see that, for a monatomic ideal gas:
"C_V = (3\/2)R"
For diatomic and polyatomic ideal gases we get:
"diatomic: C_V = (5\/2)R"
"polyatomic: C_V = 3R"
So, "C_V=\\frac{f}{2}R"
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