A magnetic field vector in an electromagnetic wave is represented by, B⃗=B0sin(2πvt−2πxλ)j^.\vec{B} = B_0 \sin \left(2 \pi v t - \dfrac{2 \pi x}{\lambda}\right) \hat{j}.B=B0sin(2πvt−λ2πx)j^. Its associated electric field vector is _______.
E⃗=−vλB0sin(2πvt−2πxλ)k^\vec{E} = - v \lambda B_0 \sin \left(2\pi v t - \dfrac{2\pi x}{\lambda}\right) \hat{k}E=−vλB0sin(2πvt−λ2πx)k^
E⃗=−vλB0sin(2πvt−2πxλ)i^\vec{E} = - v \lambda B_0 \sin \left(2\pi v t - \dfrac{2\pi x}{\lambda}\right) \hat{i}E=−vλB0sin(2πvt−λ2πx)i^
E⃗=vλB0sin(2πvt−2πxλ)k^\vec{E} = v \lambda B_0 \sin \left(2\pi v t - \dfrac{2\pi x}{\lambda}\right) \hat{k}E=vλB0sin(2πvt−λ2πx)k^
E⃗=vλB0sin(2πvt−2πxλ)i^\vec{E} = v \lambda B_0 \sin \left(2\pi v t - \dfrac{2\pi x}{\lambda}\right) \hat{i}E=vλB0sin(2πvt−λ2πx)i^