Electric field of infinite sheet with time dependent charge

In summary, the electric field produced by an infinite sheet with a time-dependent charge density can be analyzed using Maxwell's equations. When the charge density varies with time, it creates a displacement current, which affects the electric field in the surrounding space. The resulting electric field is dependent on both the instantaneous charge density and the rate of change of charge over time. This situation illustrates the interplay between static and dynamic electromagnetic fields, emphasizing the significance of time-varying charge distributions in generating electric fields.
  • #1
ramazkhomeriki
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Consider infinite charged sheet in xy plane and suppose that charge is gradually and uniformly removed from the sheet. Electric field outside the sheet obviously do not depend on x and y variables, thus the Maxwell equation divE=0 reduces to the simpler form ∂Ez/∂z=0, this means that z component of electric field is uniform along z at any moment. But then it follows that the change of charge of the sheet is felt simultaneously at any point along z. I have no idea where a mistake is.
 
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  • #2
Can charge change without a current?
 
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  • #3
Dale said:
Can charge change without a current?
Ok, let us suppose that there is a current as well, but the equation in free space divE =0 remains the same.
 
  • #4
ramazkhomeriki said:
Ok, let us suppose that there is a current as well, but the equation in free space divE =0 remains the same.
Yes, but now you have a source, the current, that causes the change in E. And it does so, according to Jefimenko’s equation, in a way that preserves causality
 
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  • #5
Dale said:
Yes, but now you have a source, the current, that causes the change in E. And it does so, according to Jefimenko’s equation, in a way that preserves causality
Ok, I have a source, but from the symmetry reasoning still there is no dependence on x and y variables in free space (it is supposed that the charge is removed uniformly from any part of the sheet). thus, we still have the equation dEz/dz=0 and the homogeneous electric field along z at any time.
 
  • #6
Where is the charge going? I think the current must be flowing away in the Z-direction It can't really flow away in the X and Y direction in a way that preserves X,Y symmetry. So if there is a charge flowing away in the Z-direction, then there is charge in the Z-direction away from the initial charge sheet, no?
 
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  • #7
phyzguy said:
Where is the charge going? I think the current must be flowing away in the Z-direction It can't really flow away in the X and Y direction in a way that preserves X,Y symmetry. So if there is a charge flowing away in the Z-direction, then there is charge in the Z-direction away from the initial charge sheet, no?
Yes, sure... Then it follows that z component of electric field does not change in time?
 
  • #8
ramazkhomeriki said:
but from the symmetry reasoning still there is no dependence on x and y variables in free space
Yes, that is correct and desired, by symmetry.

ramazkhomeriki said:
we still have the equation dEz/dz=0 and the homogeneous electric field along z at any time.
That no longer holds except in the special case where the current has been constant forever. In that special case the homogeneity in z is correct.

If the current varies over time, however, then the field is no longer homogenous in z and the changes in the z direction propagate causally

Look at all three terms in Jefimenko’s equation for the E field.
 
  • #9
ramazkhomeriki said:
Consider infinite charged sheet in xy plane and suppose that charge is gradually and uniformly removed from the sheet. Electric field outside the sheet obviously do not depend on x and y variables, thus the Maxwell equation divE=0 reduces to the simpler form ∂Ez/∂z=0, this means that z component of electric field is uniform along z at any moment. But then it follows that the change of charge of the sheet is felt simultaneously at any point along z. I have no idea where a mistake is.
But ##\vec{\nabla} \cdot \vec{E}=0## is a contradiction to your setup, because you say you have a surface charge on the sheet. The correct equation is (in SI units)
$$\vec{\nabla} \cdot \vec{E}=\rho/\epsilon_0=\delta(z) \sigma(t,x,y)/\epsilon_0.$$
Of course everything else said in this thread so far is correct too, i.e., if ##\partial_t \sigma## you also must have a current density such that the continuity equation, ##\partial_t \rho+\vec{\nabla} \cdot \vec{j}=0## is fulfilled. Given both the charge and current density you get the fields via the retarded potentials (or, usually more cumbersome directly the em. field using the corresponding "Jefimenko equations").
 
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  • #10
Dale said:
If the current varies over time
It must, because eventually you will run out of charge.

If I were asked to solve this, I would start by modeling the charge density as exponentially decaying with time. Physically plausible, and I have a hope of getting a solvable differential equation.
 
  • #11
ramazkhomeriki said:
Yes, sure... Then it follows that z component of electric field does not change in time?
How could that possibly be true? As @Vanadium 50 pointed out, the amount of charge is decreasing, so the current has to be decreasing, so the electric field must be a function of time.
 
  • #12
I think the OP is getting tangled up in knots by making mutually contradictory assumptions - a static system, instantaneous reaction time, etc.

Consider you have an infinite sheet, open on top, and attached to a resistive medium on the bottom, and grounded underneath that. That's an RC circuit - your capacitor will discharge into ground. As this happens, the field above it will decrease.

Normally, we consider the approximation that everything happens slowly compared to the light travel time between the elements: true for most typical RC time constants and the size of capacitors. If that approximation isn't good enough, you have to roll up your sleeves and use retarted potentials or similar.
 
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  • #13
Vanadium 50 said:
I think the OP is getting tangled up in knots by making mutually contradictory assumptions - a static system, instantaneous reaction time, etc.

Consider you have an infinite sheet, open on top, and attached to a resistive medium on the bottom, and grounded underneath that. That's an RC circuit - your capacitor will discharge into ground. As this happens, the field above it will decrease.

Normally, we consider the approximation that everything happens slowly compared to the light travel time between the elements: true for most typical RC time constants and the size of capacitors. If that approximation isn't good enough, you have to roll up your sleeves and use retarted potentials or similar.
The entire problem is to have two sheets of charges (one positive and one negative), i.e. capacitor and then one shortens those two sheets. Of course, some electromagnetic waves will propagate inside the capacitor, but those waves are transverse, not changing z component of electric field. My problem is to calculate how E_z changes in time by simplest argument that the problem is homogeneous in xy plane, but it seems that it is not possible. I thought that this problem should be simpler than the one with point like time dependent charge...
 
  • #14
ramazkhomeriki said:
The entire problem is to have two sheets of charges (one positive and one negative), i.e. capacitor and then one shortens those two sheets. Of course, some electromagnetic waves will propagate inside the capacitor, but those waves are transverse, not changing z component of electric field. My problem is to calculate how E_z changes in time by simplest argument that the problem is homogeneous in xy plane, but it seems that it is not possible. I thought that this problem should be simpler than the one with point like time dependent charge...
Can you explain further? If the two sheets extend in the X and Y directions, what do you mean by "one shortens those two sheets"? Do you mean they move closer together in Z? Or do you mean their X,Y extent is reduced?
 
  • #15
phyzguy said:
Can you explain further? If the two sheets extend in the X and Y directions, what do you mean by "one shortens those two sheets"? Do you mean they move closer together in Z? Or do you mean their X,Y extent is reduced?
I mean just to connect those two sheets by wire.
 
  • #16
OK. So then what's the question? As @Vanadium 50 said, "Normally, we consider the approximation that everything happens slowly compared to the light travel time between the elements: true for most typical RC time constants and the size of capacitors."

In that approximation, Ez just decays exponentially.
If you're not satisfied with that approximation, then the problem is much more complicated. Electromagnetic waves will propagate laterally from the connection point of the wire, and vertically between the plates.
 
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  • #17
phyzguy said:
OK. So then what's the question? As @Vanadium 50 said, "Normally, we consider the approximation that everything happens slowly compared to the light travel time between the elements: true for most typical RC time constants and the size of capacitors."

In that approximation, Ez just decays exponentially.
If you're not satisfied with that approximation, then the problem is much more complicated. Electromagnetic waves will propagate laterally from the connection point of the wire, and vertically between the plates.
You say, Ez varies much slower than E_y and E_x, because the change of E_z is caused by slow movement of charges, while E_y and E_z are changing due to wave propagation. Do I understand correctly? It would simplify the problem but one has to be sure that the propagation of electromagnetic waves will not alter E_z.
 
  • #18
ramazkhomeriki said:
You say, Ez varies much slower than E_y and E_x, because the change of E_z is caused by slow movement of charges, while E_y and E_z are changing due to wave propagation.
Where did I say that??
 
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  • #19
phyzguy said:
Where did I say that??
You said: "Ez just decays exponentially". I guess decay rate is just a time is needed for the charge to travel in the wire from one sheet to another.
 
  • #20
Let's take a strep back. You were given a setup with an approximate answer. Is that not good enough? After all - the setup is either an approximation (infinite f`or really big) or unphysical (infinite is really infinite).

You've also been given the exact solutions, if by name and not by equation (twice - once in terms of fields and once in terms of potentials) Why isn't this good enough? "Here's a tough problem - you guys solve it" tends not to generate many (often any) takers.

What do you want that hasn't already been said?
 
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  • #21
Vanadium 50 said:
Let's take a strep back. You were given a setup with an approximate answer. Is that not good enough? After all - the setup is either an approximation (infinite f`or really big) or unphysical (infinite is really infinite).

You've also been given the exact solutions, if by name and not by equation (twice - once in terms of fields and once in terms of potentials) Why isn't this good enough? "Here's a tough problem - you guys solve it" tends not to generate many (often any) takers.

What do you want that hasn't already been said?
In reality I have much more complex physical system to solve, that is multiferroic BiFeO3 domain wall structure (here is the information: https://pubs.acs.org/doi/full/10.1021/acs.nanolett.9b03484). There were some activities on generating THz radiation charging and then shortening ultimate sides of that structure. I am trying to simplify the picture by introducing capacitor system coupled in series, I thought that the problem I have formulated was well known and easily solvable, as I see it is not the case. Thank you for your answers...
 
  • #22
ramazkhomeriki said:
shortening
Just for clarity, "shortening" something means to reduce its length, while "shorting" something means to make an electrical connection with zero resistance. I think you mean the latter.
 
  • #23
Ibix said:
Just for clarity, "shortening" something means to reduce its length, while "shorting" something means to make an electrical connection with zero resistance. I think you mean the latter.
Yes, I meant that...
 

FAQ: Electric field of infinite sheet with time dependent charge

What is an electric field of an infinite sheet with time-dependent charge?

The electric field of an infinite sheet with time-dependent charge refers to the electric field generated by a large, flat surface where the surface charge density varies with time. This time dependence can introduce complexities in calculating the electric field due to the dynamic nature of the charge distribution.

How is the electric field calculated for an infinite sheet with a time-dependent charge density?

To calculate the electric field of an infinite sheet with a time-dependent charge density, one typically uses Gauss's Law, modified to account for the time dependence. The general form of Gauss's Law, combined with the symmetry of the problem, simplifies the calculation. The electric field at any point near the sheet can be expressed as E(t) = σ(t) / (2ε₀), where σ(t) is the time-dependent surface charge density and ε₀ is the permittivity of free space.

Does the time dependence of the charge density affect the symmetry of the electric field?

No, the time dependence of the charge density does not affect the symmetry of the electric field. The field remains perpendicular to the surface of the infinite sheet and uniform in magnitude at any given distance from the sheet. However, the magnitude of the electric field will vary over time in accordance with the changes in the surface charge density.

Can the electric field of an infinite sheet with time-dependent charge induce electromagnetic waves?

Yes, a time-varying electric field can induce electromagnetic waves. According to Maxwell's equations, a changing electric field can generate a changing magnetic field, which in turn can propagate as an electromagnetic wave. Therefore, an infinite sheet with a time-dependent charge density can serve as a source of such waves.

What are the practical implications of studying the electric field of an infinite sheet with time-dependent charge?

Understanding the electric field of an infinite sheet with time-dependent charge has several practical implications, particularly in fields such as electromagnetism, antenna theory, and materials science. It helps in designing and analyzing devices that involve dynamic charge distributions, such as capacitors with varying charge densities, and contributes to the broader understanding of time-varying fields and their interactions with matter.

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