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How many Maxwell's equations are there?

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There are four Maxwell's equations. They describe how electric and magnetic fields interact and propagate. Here’s a brief overview of each:

1. **Gauss's Law**: Relates the electric field to the charge distribution.
2. **Gauss's Law for Magnetism**: States that there are no magnetic monopoles; magnetic field lines are closed loops.
3. **Faraday's Law of Induction**: Describes how a changing magnetic field induces an electric field.
4. **Ampère-Maxwell Law**: Relates the magnetic field to electric current and the rate of change of the electric field.

Together, these equations form the foundation of classical electromagnetism.
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Maxwell's equations are a set of four fundamental equations in electromagnetism that describe how electric and magnetic fields interact and propagate. They are:

1. **Gauss's Law for Electricity**: This equation relates the electric field to the charge distribution. It states that the electric flux through a closed surface is proportional to the enclosed electric charge.
   
   \[\nabla \cdot \mathbf{E} = \frac{\rho}{\epsilon_0}\]

   where \(\mathbf{E}\) is the electric field, \(\rho\) is the charge density, and \(\epsilon_0\) is the permittivity of free space.

2. **Gauss's Law for Magnetism**: This law indicates that there are no magnetic monopoles; the magnetic flux through a closed surface is zero.
   
   \[\nabla \cdot \mathbf{B} = 0\]

   where \(\mathbf{B}\) is the magnetic field.

3. **Faraday's Law of Induction**: This law states that a changing magnetic field induces an electric field. It describes how a time-varying magnetic field creates an electric field.
   
   \[\nabla \times \mathbf{E} = -\frac{\partial \mathbf{B}}{\partial t}\]

4. **Ampère's Law with Maxwell's Addition**: This equation shows how electric currents and changing electric fields produce a magnetic field. Maxwell's addition accounts for the displacement current, which is important for understanding electromagnetic waves.
   
   \[\nabla \times \mathbf{B} = \mu_0 \mathbf{J} + \mu_0 \epsilon_0 \frac{\partial \mathbf{E}}{\partial t}\]

   where \(\mathbf{J}\) is the current density, \(\mu_0\) is the permeability of free space, and \(\epsilon_0\) is the permittivity of free space.

These equations form the foundation of classical electromagnetism, optics, and electric circuits.
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