The magnitude of the magnetic field (\( |\vec{B}| \)) is related to the electric field magnitude (\( |\vec{E}| \)) by:
\[ |\vec{B}| = \frac{|\vec{E}|}{c}, \]
where \( c = 3 \times 10^8 \, \text{m/s} \) is the speed of light in free space. Substituting the given values:
\[ |\vec{B}| = \frac{6.6}{3 \times 10^8} = 2.2 \times 10^{-8} \, \text{T}. \]
In an electromagnetic wave, the electric field (\( \vec{E} \)), magnetic field (\( \vec{B} \)), and propagation direction (\( \vec{C} \)) are mutually perpendicular and follow the right-hand rule:
\[ \vec{E} \times \vec{B} = \vec{C}. \]
Combining the magnitude and direction, the magnetic field is:
\[ \vec{B} = (2.2 \times 10^{-8}) \, \hat{k} \, \text{T}. \]
\( \vec{B} = 2.2 \times 10^{-8} \, \hat{k} \, \text{T} \).
The dimension of $ \sqrt{\frac{\mu_0}{\epsilon_0}} $ is equal to that of: (Where $ \mu_0 $ is the vacuum permeability and $ \epsilon_0 $ is the vacuum permittivity)

In the first configuration (1) as shown in the figure, four identical charges \( q_0 \) are kept at the corners A, B, C and D of square of side length \( a \). In the second configuration (2), the same charges are shifted to mid points C, E, H, and F of the square. If \( K = \frac{1}{4\pi \epsilon_0} \), the difference between the potential energies of configuration (2) and (1) is given by: