To determine the magnetic field \(\vec{B}\) associated with the given electric field \(\vec{E}\) in an electromagnetic wave, we use the relationship between the electric and magnetic fields in a plane wave in free space. The magnitude of the magnetic field \(\vec{B}\) is given by \(|\vec{B}| = \frac{|\vec{E}|}{c}\), where \(c\) is the speed of light, approximately \(3 \times 10^8\) m/s.
Given the electric field:
\[\vec{E} = 57 \cos \left[7.5 \times 10^6 t - 5 \times 10^{-3} (3x + 4y)\right] \left( 4\hat{i} - 3\hat{j} \right) \, \text{N/C}\]
The magnitude of \(\vec{E}\) is 57 N/C.
The corresponding magnitude of \(\vec{B}\) is:
\[|\vec{B}| = \frac{57}{3 \times 10^8} \, \text{T}\]
The direction of \(\vec{B}\) is perpendicular to both \(\vec{E}\) and the wave vector \(\vec{k}\). The wave propagates in the direction of \(\vec{k} = 3\hat{i} + 4\hat{j}\), perpendicular to both \(\vec{E}\) and the direction of propagation. The direction of \(\vec{B}\) can be determined using the right-hand rule. Thus, \(\vec{B}\) is directed along \(\hat{k}\).
However, using the right-hand rule considering the cross product \(\vec{k} \times \vec{E}\), \(\vec{B}\) points in the negative \(\hat{k}\) direction, hence introducing the negative sign:
\[\vec{B} = - \frac{57}{3 \times 10^8} \cos \left[7.5 \times 10^6 t - 5 \times 10^{-3} (3x + 4y)\right] (5\hat{k}) \, \text{T}\]
\(\vec{B} = - \frac{57}{3 \times 10^8} \cos \left[7.5 \times 10^6 t - 5 \times 10^{-3} (3x + 4y)\right] (5\hat{k})\)
AB is a part of an electrical circuit (see figure). The potential difference \(V_A - V_B\), at the instant when current \(i = 2\) A and is increasing at a rate of 1 amp/second is: