To find the temperature of a star acting as a black body, we can use the Stefan-Boltzmann law, which states that the power emitted per unit area by a black body is proportional to the fourth power of its temperature. Mathematically, it is expressed as:
E = \sigma T^4where E is the energy radiated per unit area, T is the temperature of the black body, and \sigma is Stefan's constant.
If the star is a sphere with radius R, the surface area A is given by:
A = 4\pi R^2The total energy emitted by the star per unit time (rate of energy production) is Q. Thus, we have:
Q = A \cdot E = 4\pi R^2 \cdot \sigma T^4Rearranging this equation to solve for T, we get:
T^4 = \frac{Q}{4\pi R^2 \sigma}Taking the fourth root of both sides, we find:
T = \left(\frac{Q}{4\pi R^2 \sigma}\right)^{1/4}Therefore, the correct answer is:
\left(\frac{Q}{4\pi R^2 \sigma}\right)^{1/4}A particle is moving in a straight line. The variation of position $ x $ as a function of time $ t $ is given as:
$ x = t^3 - 6t^2 + 20t + 15 $.
The velocity of the body when its acceleration becomes zero is: