Using the Stefan-Boltzmann Law: \[ P = \sigma A T^4 \] where \( P = 30 \, \text{kW} = 30 \times 10^3 \, \text{W} \), \( A \) is the surface area of the sphere, and \( T \) is the temperature. The surface area of a sphere is given by: \[ A = 4 \pi r^2 \] Substitute \( r = 0.03 \, \text{m} \): \[ A = 4 \pi (0.03)^2 \approx 0.0113 \, \text{m}^2 \] Now use the Stefan-Boltzmann equation to solve for \( T \): \[ 30 \times 10^3 = (5.67 \times 10^{-8}) \times 0.0113 \times T^4 \] Solving for \( T \): \[ T^4 \approx \frac{30 \times 10^3}{(5.67 \times 10^{-8}) \times 0.0113} \approx 4.6 \times 10^3 \] Thus, \( T \approx 4600 \, \text{K} \).
The left and right compartments of a thermally isolated container of length $L$ are separated by a thermally conducting, movable piston of area $A$. The left and right compartments are filled with $\frac{3}{2}$ and 1 moles of an ideal gas, respectively. In the left compartment the piston is attached by a spring with spring constant $k$ and natural length $\frac{2L}{5}$. In thermodynamic equilibrium, the piston is at a distance $\frac{L}{2}$ from the left and right edges of the container as shown in the figure. Under the above conditions, if the pressure in the right compartment is $P = \frac{kL}{A} \alpha$, then the value of $\alpha$ is ____