Consider an isolated system of two concentric spherical black bodies. The inner sphere of radius \( R \) is at temperature \( T \), and the outer sphere of radius \( 4R \) is at temperature \( 2T \). The rate of absorption of radiant energy by the outer sphere is:
\( 64 \sigma \pi R^2 T^4 \)
Step 1: Understanding Black Body Radiation The power radiated by a black body follows Stefan-Boltzmann law: \[ P = \sigma A T^4 \] where: - \( P \) is the radiated power, - \( \sigma \) is the Stefan-Boltzmann constant, - \( A \) is the surface area of the radiating body, - \( T \) is the temperature in Kelvin.
Step 2: Calculating the Power Radiated by the Inner Sphere The inner sphere has radius \( R \), so its surface area is: \[ A_{\text{inner}} = 4 \pi R^2 \] The power radiated by the inner sphere: \[ P_{\text{inner}} = \sigma A_{\text{inner}} T^4 \] \[ P_{\text{inner}} = \sigma (4 \pi R^2) T^4 \] \[ P_{\text{inner}} = 4 \sigma \pi R^2 T^4 \]
Step 3: Absorption by the Outer Sphere The outer sphere completely surrounds the inner sphere and absorbs all the radiation. Thus, the rate of absorption of radiant energy by the outer sphere is equal to the power radiated by the inner sphere: \[ P_{\text{absorbed}} = P_{\text{inner}} = 4 \sigma \pi R^2 T^4 \]
Step 4: Verifying the Correct Option Comparing with the given options, the correct answer is: \[ \mathbf{4 \sigma \pi R^2 T^4} \]
Consider a water tank shown in the figure. It has one wall at \(x = L\) and can be taken to be very wide in the z direction. When filled with a liquid of surface tension \(S\) and density \( \rho \), the liquid surface makes angle \( \theta_0 \) (\( \theta_0 < < 1 \)) with the x-axis at \(x = L\). If \(y(x)\) is the height of the surface then the equation for \(y(x)\) is: (take \(g\) as the acceleration due to gravity)
Match the following: