Step 1: Concept:
The problem asks for the thermodynamic efficiency of an ideal Carnot heat engine operating between two given temperature reservoirs. Extra information (work done and cycle time) is provided as distractors.
Step 2: Key Formula or Approach:
The theoretical maximum efficiency ($\eta$) of any heat engine operating between a hot reservoir at absolute temperature $T_H$ and a cold reservoir at absolute temperature $T_C$ is given by Carnot's theorem:
\[ \eta = 1 - \frac{T_C}{T_H} \]
This value can be multiplied by 100 to express it as a percentage.
Step 3: Step-by-step Explanation:
• Identify the given variables:
Hot reservoir temperature, $T_H = 850 \text{ K}$
Cold reservoir temperature, $T_C = 300 \text{ K}$
(The work $W = 1200 \text{ J}$ and time $t = 0.25 \text{ s}$ are not needed to calculate Carnot efficiency, as Carnot efficiency depends entirely and exclusively on the reservoir temperatures).
• Substitute the temperature values into the efficiency formula:
\[ \eta = 1 - \frac{300}{850} \]
• Simplify the fraction:
\[ \frac{300}{850} = \frac{30}{85} = \frac{6}{17} \]
• Calculate the final decimal value:
\[ \eta = 1 - \frac{6}{17} = \frac{11}{17} \]
\[ \eta \approx 1 - 0.3529 \approx 0.6471 \]
• Convert to a percentage:
\[ \eta \approx 64.71\% \]
• Looking at the options, $64.71\%$ is closest to $\simeq 65\%$.
Step 4: Final Answer:
The efficiency is approximately $65\%$, which matches option (B).