One mole of an ideal gas expands adiabatically at constant pressure such that its temperature $T \propto \frac{1}{\sqrt{V}}$. The value of $\gamma$ for the gas is $\left( \gamma = \frac{C_p}{C_v}, V = \text{Volume of the gas} \right)$
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Whenever a process relation is given in the form $T V^x = \text{constant}$, simply set $x = \gamma - 1$ to find gamma directly! Here, $x = 0.5$, so $\gamma = 0.5 + 1 = 1.5$. A clean and simple shortcut!
Step 1: Understanding the Question:
An ideal gas undergoes an adiabatic process where its thermodynamic temperature changes in inverse proportion to the square root of its volume. We need to determine the ratio of specific heats ($\gamma$) for this gas.
Step 2: Key Formula or Approach:
The standard state relation governing temperature and volume during any reversible adiabatic process is:
$$ T V^{\gamma - 1} = \text{constant} $$
Step 3: Detailed Explanation:
The question statement provides the temperature-volume proportionality rule:
$$ T \propto \frac{1}{\sqrt{V}} \implies T \propto V^{-1/2} $$
We can convert this proportionality into an equation by introducing a constant $k$:
$$ T = k \cdot V^{-1/2} $$
Multiplying both sides by $V^{1/2}$ to group the variables on the left:
$$ T V^{1/2} = \text{constant} \quad \text{--- (Equation 1)} $$
Now, let's compare our experimental state equation with the standard theoretical adiabatic equation:
$$ T V^{\gamma - 1} = \text{constant} \quad \text{--- (Equation 2)} $$
Equating the exponents of the volume parameter $V$ from Equation 1 and Equation 2:
$$ \gamma - 1 = \frac{1}{2} $$
$$ \gamma = 1 + \frac{1}{2} = \frac{3}{2} = 1.5 $$
Step 4: Final Answer:
The value of $\gamma$ for the gas is 1.5, which corresponds to option (B).