Why is the curl of (E + dA/dt) equal to zero?

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SUMMARY

The discussion centers on the equation ∇ x (E + dA/dt) = 0, derived from Faraday-Lenz's law ∇ x E = d(B)/dt and the vector potential A. It highlights that in electrostatics, the curl of the electric field E is zero, indicating a scalar potential V exists such that E = -∇V. The conversation emphasizes the implications of a non-zero magnetic field B on the electric field E, particularly in terms of the relationship between scalar potential V and vector potential A, as established by Helmholtz's theorem.

PREREQUISITES
  • Understanding of vector calculus, specifically curl and gradient operations.
  • Familiarity with electromagnetic theory, particularly Faraday-Lenz's law.
  • Knowledge of Helmholtz's theorem and its application in physics.
  • Concept of scalar and vector potentials in electromagnetism.
NEXT STEPS
  • Study the implications of Helmholtz's theorem in electromagnetic fields.
  • Explore the relationship between electric fields and magnetic fields in dynamic systems.
  • Learn about the mathematical properties of curl and gradient in vector calculus.
  • Investigate the role of vector potentials in electromagnetic theory.
USEFUL FOR

Students and professionals in physics, particularly those focusing on electromagnetism, vector calculus, and classical physics. This discussion is beneficial for anyone seeking to deepen their understanding of the relationship between electric and magnetic fields.

Poirot
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Homework Statement


This isn't necessarily a question but something I found in my notes that I didn't understand.
It says that from B = x A one can plug this into Faraday-Lenz's law x E = d(B)/dt and it leads to the equation:
x (E + d(A)/dt)=0.
From this is says "Using Helmholtz theorem, one can represent the curl free field as the gradient of a scalar potential."

Homework Equations


B = x A
x E = d(B)/dt
x (E + d(A)/dt)=0

The Attempt at a Solution


I know that in electrostatics the curl of the electric field is zero and hence there is a scalar potential associated such that E = - V but I don't see the jump for the case involving the vector potential.

Any guidance/explanation would be greatly appreciated.
 
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In electrostatics, there are no electric currents, i.e., ##\vec{B}=\vec{0}## so that ##\nabla \times \vec{E} = \vec{0}##.

However, in general, ##\vec{B}=\vec{B}(\vec{x},t)## so that ##\nabla \times \vec{E} \neq \vec{0}##

See if you can work out the consequence of having a non-zero magnetic field on the form of the electric field ##\vec{E}## in terms of the scalar potential ##V## and the vector potential ##\vec{A}##.

P.S.: This does not really strike me as being a homework problem, so it's probably better suited for the 'Classical Physics' subforum.
 
Poirot said:
x (E + d(A)/dt)=0.
The curl of a gradient is always zero ##\nabla \times \nabla \Phi = 0## (this is an identity) where ##\Phi## a scalar function.
 

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