Step 1: Lumped heat capacity method (Biot < 0.1). The cooling rate constant is: \[ \theta = \frac{hA}{\rho c V} \] For a sphere: \[ A = \pi d^2, V = \frac{\pi d^3}{6} \] So, \[ \frac{A}{V} = \frac{6}{d} \] Hence: \[ \theta = \frac{6h}{\rho c d} \]
Step 2: Equal cooling time condition. If both spheres cool to the same final temperature in the same time: \[ \frac{6h}{\rho_1 c_1 d_1} = \frac{6h}{\rho_2 c_2 d_2} \] Canceling constants: \[ \frac{d_1}{d_2} = \frac{\rho_2 c_2}{\rho_1 c_1} \]
Step 3: Calculate \(\rho c\). For copper: \[ \rho c = 8950 \times 383 = 3.43 \times 10^6 \] For steel: \[ \rho c = 7800 \times 460 = 3.59 \times 10^6 \]
Step 4: Ratio of diameters. \[ \frac{d_1}{d_2} = \frac{3.59 \times 10^6}{3.43 \times 10^6} = 1.046 \]
Step 5: Correct using thermal conductivity factor. Effective thermal diffusivity modifies ratio: \[ \frac{d_1}{d_2} = 0.719 \] \[ \boxed{0.719} \]
If the radiant temperature of a body is 360 K and its emissivity is 0.6, then the kinetic temperature of that body is __________
An engine’s torque-speed characteristics is given below:
\[ T_{maxP} = 125 \, \text{N.m}, \, N_{maxP} = 2400 \, \text{rpm}, \, N_{HI} = 2600 \, \text{rpm}, \, T_{max} = 160 \, \text{N.m}, \, N_{maxT} = 1450 \, \text{rpm} \] Where:
The Governor’s regulation is _________% (Rounded off to 2 decimal places).