The problem requires determining the temperature variation of a gas subjected to an adiabatic compression, transitioning from an initial volume and temperature to a final volume. The presence of thermally non-conducting walls in the container confirms the adiabatic nature of the process.
For a reversible adiabatic process, the relationship governing the absolute temperature (T) and volume (V) of a gas is described by the equation:
\[ TV^{\gamma-1} = \text{constant} \]Here, \( \gamma \) represents the ratio of specific heats (\( C_p/C_v \)). For two distinct states, initial (1) and final (2), this relationship can be expressed as:
\[ T_1 V_1^{\gamma-1} = T_2 V_2^{\gamma-1} \]Step 1: Enumerate the provided initial and final state variables and convert the temperature to Kelvin.
The given values are:
In thermodynamic calculations, it is imperative to utilize the absolute temperature scale (Kelvin). The conversion formula is \( T(\text{K}) = T(^\circ\text{C}) + 273 \).
\[T_1 = 27 + 273 = 300 \, \text{K}\]Step 2: Formulate the adiabatic relation to derive the final temperature \( T_2 \).
By rearranging the relation \( T_1 V_1^{\gamma-1} = T_2 V_2^{\gamma-1} \), we can solve for \( T_2 \):
\[T_2 = T_1 \left( \frac{V_1}{V_2} \right)^{\gamma-1}\]Step 3: Substitute the given values into the derived equation and compute \( T_2 \).
Initially, calculate the exponent \( \gamma - 1 \):
\[\gamma - 1 = 1.5 - 1 = 0.5 = \frac{1}{2}\]Subsequently, compute the ratio of the volumes:
\[\frac{V_1}{V_2} = \frac{800 \, \text{cm}^3}{200 \, \text{cm}^3} = 4\]Now, substitute these computed values into the equation for \( T_2 \):
\[T_2 = 300 \, \text{K} \times (4)^{0.5} = 300 \, \text{K} \times \sqrt{4}\]\[T_2 = 300 \, \text{K} \times 2 = 600 \, \text{K}\]The problem specifically asks for the change in temperature, calculated as \( \Delta T = T_2 - T_1 \).
\[\Delta T = 600 \, \text{K} - 300 \, \text{K} = 300 \, \text{K}\]The resulting change in temperature is 300 K. This aligns with option (4).