Step 1: Understanding the Concept:
A Carnot engine working between two temperatures has an efficiency \( \eta = 1 - \frac{Q_{out}}{Q_{in}} \). When engines are arranged in series such that the heat rejected by one is the input for the next, the overall efficiency of the chain can be expressed as a product of terms related to individual efficiencies. The total work done is the sum of the work from each engine.
Step 2: Key Formula or Approach:
For each engine \( i \): \( Q_{i, out} = Q_{i, in} (1 - \eta) \).
For \( N \) engines in series: \( Q_{N, out} = Q_{1, in} (1 - \eta)^N \).
Net efficiency \( \eta_{net} = 1 - \frac{Q_{N, out}}{Q_{1, in}} = 1 - (1 - \eta)^N \).
Step 3: Detailed Explanation:
Given \( N = 5 \) engines and \( \eta_{net} = \frac{211}{243} \).
\[ 1 - (1 - \eta)^5 = \frac{211}{243} \]
\[ (1 - \eta)^5 = 1 - \frac{211}{243} = \frac{243 - 211}{243} = \frac{32}{243} \]
We recognize that \( 32 = 2^5 \) and \( 243 = 3^5 \).
\[ (1 - \eta)^5 = \left( \frac{2}{3} \right)^5 \]
Taking the fifth root of both sides:
\[ 1 - \eta = \frac{2}{3} \]
\[ \eta = 1 - \frac{2}{3} = \frac{1}{3} \approx 0.333... \]
Step 4: Final Answer:
The value of the individual engine efficiency is \( 1/3 \). Expressed as a numerical value, this is approximately 0.33.