To solve this problem, we need to understand the concept of black body radiation and apply Wien's law. Wien's displacement law is given by the formula:
\[\lambda_{\text{max}} \cdot T = b\]where \(\lambda_{\text{max}}\) is the wavelength corresponding to the maximum energy emitted, \(T\) is the absolute temperature of the black body, and \(b\) is Wien's constant.
Given:
First, calculate \(\lambda_{\text{max}}\):
\[\lambda_{\text{max}} = \frac{b}{T} = \frac{2.88 \times 10^6 \, nm\,K}{5760\,K} = 500 \, nm\]This means the black body emits maximum energy at a wavelength of \(500 \, nm\).
Now let's analyze the given wavelengths:
According to the concept of black body radiation, the energy emitted is highest around the peak wavelength and decreases as we move away from this peak.
Comparing the wavelengths:
From this, we know:
Given these analyses, we can conclude:
\(U_2 > U_1\).
This matches the correct option provided.
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: