The amount of heat energy required to raise the temperature of $1\,g$ of helium from $T_1\,K$ to $T_2\,K$ is

  • A
    $\frac{3}{2}\,{N_a}{k_B}\,\left( {{T_2} - {T_1}} \right)$
  • B
    $\frac{3}{4}\,{N_a}{k_B}\,\left( {{T_2} - {T_1}} \right)$
  • C
    $\frac{3}{4}\,{N_a}{k_B}\,\left( {\frac{{{T_2}}}{{{T_1}}}} \right)$
  • D
    $\frac{3}{8}\,{N_a}{k_B}\,\left( {{T_2} - {T_1}} \right)$

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Similar Questions

The specific heat at constant pressure $(C_P)$ is greater than the specific heat at constant volume $(C_V)$ for the same gas because:

Statement $A: C_P - C_V = R$
Statement $B: \frac{C_P}{C_V} = 1.67$

The specific heat at constant volume for the monoatomic argon is $0.075 \, kcal/kg-K$,whereas its gram molecular specific heat $C_V = 2.98 \, cal/mole/K$. The mass of the argon atom is (Avogadro's number $= 6.02 \times 10^{23} \, molecules/mole$)

Derive the ratio of $\frac{C_{P}}{C_{V}}$ for a diatomic gas.

The ratio of the specific heats $\frac{C_p}{C_v} = \gamma$ in terms of degrees of freedom $(n)$ is given by

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