To solve this question, we need to use Wien's Displacement Law, which states that the wavelength of maximum intensity (\( \lambda_{\text{max}} \)) is inversely proportional to the absolute temperature (T) of a black body. The law is given by the formula:
\lambda_{\text{max}} \cdot T = b
where \( b \) is Wien's displacement constant, approximately equal to 2898 µm·K.
Therefore, when the temperature of the black body is increased to 2500 K, the maximum intensity of radiation will be observed at a wavelength of 3000 Å. Thus, the correct answer is 3000 Å.
This solution is consistent with Wien's Displacement Law, which ensures that as the temperature of a body increases, the wavelength at which it emits most intensely shifts towards the shorter end of the spectrum (reflecting higher energy radiation).
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: