The problem given involves finding the temperature of the Sun's surface using the Stefan-Boltzmann law. The Stefan-Boltzmann law states that the power radiated per unit area of a black body in terms of its temperature is given by:
\( P = \sigma \cdot A \cdot T^4 \cdot \varepsilon \)
where:
Given:
Using the formula:
\( P = \sigma \cdot A \cdot T^4 \cdot \varepsilon \)
Substituting in the known values:
\( 3.9 \times 10^{26} = 5.67 \times 10^{-8} \cdot 6.1 \times 10^{18} \cdot T^4 \cdot 1 \)
Solving for \( T \), we rearrange the equation:
\( T^4 = \frac{3.9 \times 10^{26}}{5.67 \times 10^{-8} \cdot 6.1 \times 10^{18}} \)
\( T = \left(\frac{3.9 \times 10^{26}}{5.67 \times 10^{-8} \cdot 6.1 \times 10^{18}}\right)^{1/4} \)
Calculating the right-hand side:
\( T = \left(\frac{3.9 \times 10^{26}}{3.46 \times 10^{11}}\right)^{1/4} \)
\( T = \left(1.127 \times 10^{15}\right)^{1/4} \)
Taking the fourth root:
\( T \approx 5800 \) K
The correct temperature of the Sun's surface is therefore 5800 K, matching the option: 5800 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 ____