Analyzing Maxwell's equations and electromagnetic relations:
(A) $\vec{\nabla} \times \vec{E} = 0$
From Faraday's law: $$\vec{\nabla} \times \vec{E} = -\frac{\partial \vec{B}}{\partial t}$$
This equals zero only if $\vec{B}$ is time-independent (static magnetic field). For time-varying fields, $\vec{\nabla} \times \vec{E} \neq 0$.
NOT always correct
(B) $\vec{\nabla} \cdot \vec{B} = 0$
This is Gauss's law for magnetism, stating that there are no magnetic monopoles. This is one of Maxwell's fundamental equations and is always true.
$$\vec{\nabla} \cdot \vec{B} = 0$$
ALWAYS correct
(C) $\vec{\nabla} \cdot \vec{J} - \frac{\partial \rho}{\partial t} = 0$
This is the continuity equation (charge conservation): $$\frac{\partial \rho}{\partial t} + \vec{\nabla} \cdot \vec{J} = 0$$
Rearranging: $$\vec{\nabla} \cdot \vec{J} - \frac{\partial \rho}{\partial t} = 0$$
This represents conservation of charge and is always true.
Wait, let me verify the sign. The continuity equation is: $$\frac{\partial \rho}{\partial t} + \vec{\nabla} \cdot \vec{J} = 0$$
So: $\vec{\nabla} \cdot \vec{J} = -\frac{\partial \rho}{\partial t}$
Therefore: $\vec{\nabla} \cdot \vec{J} - \frac{\partial \rho}{\partial t} = -\frac{\partial \rho}{\partial t} - \frac{\partial \rho}{\partial t} = -2\frac{\partial \rho}{\partial t} \neq 0$ in general.
Actually, the correct form is $\vec{\nabla} \cdot \vec{J} + \frac{\partial \rho}{\partial t} = 0$.
NOT always correct as written
(D) $\vec{F} = q(\vec{E} + \vec{v} \times \vec{B})$
This is the Lorentz force law, which gives the force on a charged particle moving in electromagnetic fields. This is a fundamental law and is always true.
ALWAYS correct
Answer: (B) and (D) are always correct
