To determine the dimensions of \( \epsilon_0 E^2 \), we need to understand the dimensions of each component:
Now, let's calculate the dimensions of \( \epsilon_0 E^2 \):
Performing dimensional multiplication, we have:
Thus, the dimensions of \( \epsilon_0 E^2 \) are \([M L^{-1} T^{-2}]\).
The correct answer is therefore: \([M L^{-1} T^{-2}]\).
The electric field is given by:
\[E = \frac{KQ}{R^2}.\]
Substituting \(K = \frac{1}{4\pi \epsilon_0}\), we get:
\[E = \frac{Q}{4\pi \epsilon_0 R^2}.\]
From this, the permittivity of free space (\(\epsilon_0\)) can be expressed as:
\[\epsilon_0 = \frac{Q}{4\pi R^2 E}.\]
Now, calculate \(\epsilon_0 E^2\):
\[\epsilon_0 E^2 = \frac{Q}{4\pi R^2 E} \cdot E^2 = \frac{QE}{4\pi R^2}.\]
Analyzing the dimensional formula:
\[[\epsilon_0 E^2] = \frac{[Q][E]}{[R^2]}.\]
Substituting the dimensional formulas:
\[[Q] = [W], \quad [E] = \frac{[W]}{[R^2][Q]}.\]
\[[\epsilon_0 E^2] = \frac{[W]}{[R^3]} = \frac{ML^2T^{-2}}{L^3}.\]
Simplifying:
\[[\epsilon_0 E^2] = [ML^{-1}T^{-2}].\]
Thus, the dimensions of \(\epsilon_0 E^2\) are \([ML^{-1}T^{-2}]\).
A black body is at a temperature of 2880 K. The energy of radiation emitted by this body with wavelength between 499 nm and 500 nm is U1, between 999 nm and 1000 nm is U2 and between 1499 nm and 1500 nm is U3. The Wien's constant, b = 2.88×106 nm-K. Then,

What will be the equilibrium constant of the given reaction carried out in a \(5 \,L\) vessel and having equilibrium amounts of \(A_2\) and \(A\) as \(0.5\) mole and \(2 \times 10^{-6}\) mole respectively?
The reaction : \(A_2 \rightleftharpoons 2A\)