Related Formula
B₀ = (E₀)/(c)$$B_0 = \frac{E_0}{c}$$
c = E × B$$\hat{c} = \hat{E} \times \hat{B}$$
Where c$\hat{c}$ is the direction of wave propagation.
Core Logic
From the argument of sine (kz - ω t)$(kz - \omega t)$, the wave is propagating along the positive z-axis. Thus, c = k$\hat{c} = \hat{k}$.
The electric field oscillates along the y-axis, so E = j$\hat{E} = \hat{j}$.
Step 1: Find Magnetic Field Direction
Using the cross-product relation for directions:
B = c × E = k × j = - i$$\hat{B} = \hat{c} \times \hat{E} = \hat{k} \times \hat{j} = -\hat{i}$$
Step 2: Find Magnetic Field Amplitude
B₀ = (E₀)/(c) = (54)/(3 × 10⁸) = 18 × 10⁻⁸ = 1.8 × 10⁻⁷ T$$B_0 = \frac{E_0}{c} = \frac{54}{3 \times 10^8} = 18 \times 10^{-8} = 1.8 \times 10^{-7} \text{ T}$$
Step 3: Assemble the Final Vector
B = 1.8 × 10⁻⁷ (kz - ω t) (- i) = -1.8 × 10⁻⁷ (kz - ω t) i T$$\vec{B} = 1.8 \times 10^{-7} \sin (kz - \omega t) (-\hat{i}) = -1.8 \times 10^{-7} \sin (kz - \omega t) \hat{i} \text{ T}$$
Pattern Recognition
Always use E × B = c$\hat{E} \times \hat{B} = \hat{c}$. Given c = k$\hat{c} = \hat{k}$ and E = j$\hat{E} = \hat{j}$, B$\hat{B}$ must be - i$-\hat{i}$ to satisfy j × (- i) = k$\hat{j} \times (-\hat{i}) = \hat{k}$.
Chapter Mix
Class 12 Physics: Electromagnetic Waves