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In electrostatics we consider the curl of B to be equal to conductivity multiplied with current density and the time varying Electric field component to be 0. but Electric fields are created by charges. And if there is a current i.e. i = dq/dt this means that the charge is varying with time. So how can the Electric field be independent of time ?

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  • $\begingroup$ By the way, the term you're looking for where currents are non-zero but the electric field does not vary over time is "magnetostatics," not "electrostatics." Electrostatics means you have no currents at all. $\endgroup$
    – Chris
    Commented Feb 1, 2018 at 0:59
  • $\begingroup$ A current doesn't imply a time varying charge. A gradient of current density does. $\endgroup$
    – The Photon
    Commented Feb 1, 2018 at 1:00

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A current doesn't necessarily mean charge is changing over time. A wire has a net charge density of zero throughout, and the electrons moving through it doesn't change that.

Basically, as an electron leaves a particular location, a new one takes its place. So there's no net change in charge density.

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If we are considering electrostatics,then yes the time varying component of the Electric field is zero and thus no magnetic field.

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  • $\begingroup$ But two wires with steady current through them are said attract/repel magnetically. $\endgroup$ Commented Feb 1, 2018 at 0:44
  • $\begingroup$ That's true, current is not an electrostatic phenomenon, also the magnetic field caused by a current is caused by a length contraction in the reference frame of a stationary particle. $\endgroup$ Commented Feb 2, 2018 at 1:44
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You have to differentiate between stationary, divergence-free currents and currents due to a locally changing charge density. In a stationary loop current there is no accumulation or depletion of charge anywhere. This is typically the case in all dc electrical circuits. In general, from the Maxwell law you mentioned follows the general law of conservation of charge $$ \nabla\cdot(\nabla\times{\vec B})= \mu_0\nabla\cdot(\vec J +\epsilon_0 \epsilon_r\frac{\partial \vec E}{\partial t})=0 $$ $\implies$ $$ \nabla\cdot{\vec J}=-\frac {\partial \rho}{\partial t}$$ Thus you can have divergence-free currents without any charges changing anywhere. You have just a charge flow constant in time without any time varying charge anywhere.

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