Step 1: Understanding Carnot Efficiency Formula The efficiency \( \eta \) of a Carnot engine is given by: \[ \eta = 1 - \frac{T_C}{T_H} \] where \( T_C \) is the sink (low-temperature reservoir) temperature, and \( T_H \) is the source (high-temperature reservoir) temperature.
Step 2: Setting Up Equations for Given Conditions We are given that initially: \[ \frac{1}{6} = 1 - \frac{T_C}{T_H} \] Rearranging, \[ \frac{T_C}{T_H} = 1 - \frac{1}{6} = \frac{5}{6} \] Thus, \[ T_C = \frac{5}{6} T_H \] After lowering the sink temperature by 65 K, the efficiency increases to \( \frac{1}{3} \), so: \[ \frac{1}{3} = 1 - \frac{T_C - 65}{T_H} \] \[ \frac{T_C - 65}{T_H} = 1 - \frac{1}{3} = \frac{2}{3} \] Thus, \[ T_C - 65 = \frac{2}{3} T_H \]
Step 3: Solving for \( T_H \) and \( T_C \) From the two equations: 1. \( T_C = \frac{5}{6} T_H \) 2. \( T_C - 65 = \frac{2}{3} T_H \) Substituting the first equation into the second: \[ \frac{5}{6} T_H - 65 = \frac{2}{3} T_H \] Multiplying everything by 6 to clear fractions: \[ 5 T_H - 390 = 4 T_H \] \[ T_H = 390 \text{ K} \] Now, substituting into \( T_C = \frac{5}{6} T_H \): \[ T_C = \frac{5}{6} \times 390 = 325 \text{ K} \] After decreasing by 65 K: \[ T_C' = 325 - 65 = 260 \text{ K} \] Thus, the initial and final sink temperatures are 325 K and 260 K, respectively.
An amount of ice of mass \( 10^{-3} \) kg and temperature \( -10^\circ C \) is transformed to vapor of temperature \( 110^\circ C \) by applying heat. The total amount of work required for this conversion is,
(Take, specific heat of ice = 2100 J kg\(^{-1}\) K\(^{-1}\),
specific heat of water = 4180 J kg\(^{-1}\) K\(^{-1}\),
specific heat of steam = 1920 J kg\(^{-1}\) K\(^{-1}\),
Latent heat of ice = \( 3.35 \times 10^5 \) J kg\(^{-1}\),
Latent heat of steam = \( 2.25 \times 10^6 \) J kg\(^{-1}\))
Match List-I with List-II.