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 \([ML^{-1}T^{-2}]\).
Match the LIST-I with LIST-II: 
Choose the correct answer from the options given below:
Match the LIST-I with LIST-II 
Choose the correct answer from the options given below:
MX is a sparingly soluble salt that follows the given solubility equilibrium at 298 K.
MX(s) $\rightleftharpoons M^{+(aq) }+ X^{-}(aq)$; $K_{sp} = 10^{-10}$
If the standard reduction potential for $M^{+}(aq) + e^{-} \rightarrow M(s)$ is $(E^{\circ}_{M^{+}/M}) = 0.79$ V, then the value of the standard reduction potential for the metal/metal insoluble salt electrode $E^{\circ}_{X^{-}/MX(s)/M}$ is ____________ mV. (nearest integer)
[Given : $\frac{2.303 RT}{F} = 0.059$ V]
An infinitely long straight wire carrying current $I$ is bent in a planar shape as shown in the diagram. The radius of the circular part is $r$. The magnetic field at the centre $O$ of the circular loop is :
