Step 1: Understanding the Question:
An ideal gas sample has an initial temperature of $T_1 = 27^\circ\text{C}$. It undergoes a rapid adiabatic compression such that its final volume shrinks to a fraction of its original value ($V_2 = \frac{8}{27}V_1$). Given the adiabatic index $\gamma = \frac{5}{3}$, we need to calculate the total temperature increase ($\Delta T = T_2 - T_1$).
Step 2: Key Formula or Approach:
For any ideal gas system undergoing an adiabatic process, the relationship connecting temperature and volume variables is:
$$T_1 V_1^{\gamma-1} = T_2 V_2^{\gamma-1} \implies \frac{T_2}{T_1} = \left( \frac{V_1}{V_2} \right)^{\gamma-1}$$
We must convert the initial temperature from Celsius to Kelvin ($T(\text{K}) = T(^\circ\text{C}) + 273.15$) before applying this proportional law.
Step 3: Detailed Explanation:
First, convert the initial temperature $T_1$ into Kelvin:
$$T_1 = 27^\circ\text{C} + 273 = 300\text{ K}$$
The problem states that the volume ratio is $\frac{V_2}{V_1} = \frac{8}{27}$, which means its inverse is $\frac{V_1}{V_2} = \frac{27}{8}$.
Now, compute the exponential power term $\gamma - 1$:
$$\gamma - 1 = \frac{5}{3} - 1 = \frac{2}{3}$$
Substitute these values into our adiabatic ratio equation to solve for $T_2$:
$$\frac{T_2}{300} = \left( \frac{27}{8} \right)^{\frac{2}{3}}$$
Simplify the fractional term inside the parentheses by breaking it down into cubics: $\frac{27}{8} = \left(\frac{3}{2}\right)^3$.
$$\frac{T_2}{300} = \left[ \left(\frac{3}{2}\right)^3 \right]^{\frac{2}{3}} = \left(\frac{3}{2}\right)^2 = \frac{9}{4}$$
Isolate $T_2$:
$$T_2 = 300 \times \frac{9}{4} = 75 \times 9 = 675\text{ K}$$
The question asks for the
rise in temperature ($\Delta T$), not the final absolute temperature:
$$\Delta T = T_2 - T_1 = 675\text{ K} - 300\text{ K} = 375\text{ K}$$
This matches option (D).
Step 4: Final Answer:
The net rise in the temperature of the gas is $375\text{ K}$, which corresponds to option (D).