2 equations for electric field

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The discussion centers on the two equations used to describe the electric field: the negative gradient of the potential (-∇V) and the negative partial derivative of the vector potential A with respect to time (-∂A/∂t). It is confirmed that both equations can describe the electric field depending on whether the field is static or changing over time. The conversation also touches on Maxwell's equations, which govern the behavior of electric and magnetic fields, emphasizing that the electric field must satisfy these equations at all times. Additionally, it is noted that the magnetic field can always be expressed as the curl of the vector potential A, regardless of time dependence. Understanding these relationships is crucial for comprehending electromagnetism.
Isaac0427
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Hi guys!
I have noticed that the electric field has 2 equations to it- the negative gradient of the potential, and the negative partial derivative of A with respect to time. Is this like e=mc^2 and e=hν, where only one equation can be used at a time? Can an electric field be described by -∇v OR -∂A/∂t (in which case you are getting an electric field from changing a magnetic field).
 
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Good observation !

At school we use Gauss's law to find E (or the potential V) for given charge distributions (that's usually the electrostatics chapters) and use ##\vec E = -\nabla V## to link the two.

And in the magnetism chapters we encounter Faraday's law of induction to find an e.m.f. (again, a V and an E!) as a consequence of a changing magnetic field.
So yes, the corny answer is: yes the field can be described by both.

Further on in the curriculum we have electromagnetism and things are heavily intertwined and we have the Maxwell equations

But you are right: the electric field has to satisfy all the Maxwell equations at all times.
 
If it is an electrostatic field, only then it can be equal to the negative gradient of a potential. If it is changing with time, then you need a term -∂A/∂t to calculate the electric field. A is called the vector potential, which is also related to the changing magnetic field that you talked about.
 
BvU said:
Good observation !

At school we use Gauss's law to find E (or the potential V) for given charge distributions (that's usually the electrostatics chapters) and use E⃗ =−∇V\vec E = -\nabla V to link the two.

And in the magnetism chapters we encounter Faraday's law of induction to find an e.m.f. (again, a V and an E!) as a consequence of a changing magnetic field.
So yes, the corny answer is: yes the field can be described by both.

Further on in the curriculum we have electromagnetism and things are heavily intertwined and we have the Maxwell equations

But you are right: the electric field has to satisfy all the Maxwell equations at all times.
Is there another way to define the magnetic field other than the curl of A. I know from Ampere's law, the curl of B relies on two things: the change in E with time, and the current density J. Is it like the electric field, where only one of those can describe any given magnetic field. Would that mean there is another part to B=∇XA? I may be completely off, but it seems as though there are 2 mutually exclusive ways to define each of the fields in electromagnetism. I'm sorry if this is a stupid observation.
 
There are two "equations" here. The dependence of the curl of B on dE/dt and the current density J, is one of Maxwell's equations and is always satisfied. This has nothing to do with writing B as the curl of A. The relation B = curl A follows from another Maxwell equation, which says that the divergence of B is always zero. This is also always satisfied, though there is a lot of discussion about it, because that Maxwell equation says that there are no magnetic monopoles. If we accept that, then the divergence of B is zero, and B can always be written as the curl of a vector field, which is called the vector potential A. This part has nothing to do with time dependence. Whether B is time dependent or not, you can always write it as the curl of A.
 
Chandra Prayaga said:
There are two "equations" here. The dependence of the curl of B on dE/dt and the current density J, is one of Maxwell's equations and is always satisfied. This has nothing to do with writing B as the curl of A. The relation B = curl A follows from another Maxwell equation, which says that the divergence of B is always zero. This is also always satisfied, though there is a lot of discussion about it, because that Maxwell equation says that there are no magnetic monopoles. If we accept that, then the divergence of B is zero, and B can always be written as the curl of a vector field, which is called the vector potential A. This part has nothing to do with time dependence. Whether B is time dependent or not, you can always write it as the curl of A.
But is ∇X(∇XA) equal to J OR ∂E/∂t or J PLUS ∂E/∂t?
 
The plus sign. See the Maxwell equations link.
 
BvU said:
The plus sign. See the Maxwell equations link.
Correct. Maxwell equations are always correct, so curl (curl A) = J + ∂E/∂t. Particular case of that equation: If the fields are time independent, then the second term is zero and curl (curl A) = curl B = J, which is Ampere's law.
 

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