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The following equations are equations of electrostatics: $$\nabla \times \vec E=0$$ $$\nabla\cdot\vec E=\dfrac{\rho}{\epsilon_0}.$$

These are 4 independent equations, while $\vec E$ has only 3 independent components. Yet these equations do not completely specify the field, as after adding the gradient of a scalar $\nabla \lambda$ that satisfies Laplace equation ($\nabla^2 \lambda$=0) to $\vec E$ leaves the equations unchanged: $$\cases{\nabla \times \vec E=0\\\nabla\cdot\vec E=\dfrac{\rho}{\epsilon_0}}\xrightarrow[\nabla^2\lambda=0]{\vec E'=\vec E+\nabla \lambda}\cases{\nabla \times \vec {E'}=0\\\nabla\cdot\vec {E'}=\dfrac{\rho}{\epsilon_0}}$$ (note the primes on the RightHandSide $\vec E$s)

The system should be overdetermined (4 equations, 3 unknowns) but apparently it is underdetermined.

  • Is the system overdetermined or underdetermined?
  • How do we usually choose the arbitrary $\lambda$ in a problem with $\rho$ given and (say) Neumann boundary condition?
  • Why the first equation (curl) is not enough?
user215721
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1 Answers1

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We normally choose $\lambda$ in a way that makes our calculations easiest purely because nothing says we can't do that.

The first equation is not enough to determine the system for the same reason that $\frac{\partial y(x)}{\partial x}=f(x)$ can never uniquely determine $y(x)$. We can always add a constant offset that changes $y(x)$ but not $f(x)$.

As for why we need the second equation, simply stating that an electrostatic field is curl-less is not sufficient to describe the physics. Both equations act as constraints on each other to allow us to determine an electrostatic field given some boundary conditions as well as determine the physics associated with it.

Jim
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