Step 1: Understanding the Given Temperatures - The Celsius-Fahrenheit coincidence occurs at: \[ T_1 = -40^\circ C = 233 \text{ K}. \] - The Kelvin-Fahrenheit coincidence occurs at: \[ T_2 = 574.25 \text{ K}. \]
Step 2: Applying Carnot’s Efficiency Formula The efficiency of a Carnot engine is given by: \[ \eta = 1 - \frac{T_C}{T_H}. \] Substituting values: \[ \eta = 1 - \frac{233}{574.25}. \] \[ \eta = 1 - 0.4059. \] \[ \eta = 0.594 \approx 60%. \] Thus, the correct answer is: 60%.
Step 1: Identifying the Special Temperatures
We are given two specific temperature points that are notable due to their unique relationships across different temperature scales:
- The Celsius-Fahrenheit coincidence occurs at:
\( T_1 = -40^\circ C \)
To convert this to the Kelvin scale:
\( T(K) = T(°C) + 273.15 \)
\( T_1 = -40 + 273.15 = 233.15 \text{ K} \approx 233 \text{ K} \)
- The Kelvin-Fahrenheit coincidence point is given directly as:
\( T_2 = 574.25 \text{ K} \)
These values are used as the temperatures for the cold reservoir (\( T_C = 233 \text{ K} \)) and the hot reservoir (\( T_H = 574.25 \text{ K} \)) of a Carnot heat engine.
Step 2: Understanding the Carnot Engine Efficiency
The efficiency of a Carnot engine operating between two thermal reservoirs is given by the formula:
\( \eta = 1 - \frac{T_C}{T_H} \)
where:
- \( \eta \) is the efficiency (expressed as a decimal)
- \( T_C \) is the cold reservoir temperature in Kelvin
- \( T_H \) is the hot reservoir temperature in Kelvin
Step 3: Substituting the Values
Plugging in the known values:
\( \eta = 1 - \frac{233}{574.25} \)
\( \eta = 1 - 0.4059 \)
\( \eta = 0.5941 \)
Converting to a percentage:
\( \eta \times 100 = 59.41\% \)
Rounding to the nearest whole number:
\( \eta \approx 60\% \)
Final Answer:
The ideal efficiency of the Carnot engine under these conditions is approximately 60%.
A piston of mass M is hung from a massless spring whose restoring force law goes as F = -kx, where k is the spring constant of appropriate dimension. The piston separates the vertical chamber into two parts, where the bottom part is filled with 'n' moles of an ideal gas. An external work is done on the gas isothermally (at a constant temperature T) with the help of a heating filament (with negligible volume) mounted in lower part of the chamber, so that the piston goes up from a height $ L_0 $ to $ L_1 $, the total energy delivered by the filament is (Assume spring to be in its natural length before heating) 