Problem in orienting two plates as instructed in question

  • Thread starter Thread starter gracy
  • Start date Start date
  • Tags Tags
    Plates
AI Thread Summary
The discussion revolves around calculating the electric field between two parallel metal plates with opposite surface charge densities. The key point is that the electric fields produced by each plate are equal in magnitude but opposite in direction, resulting in a net electric field of zero outside the plates and a uniform field between them. Participants clarify that the electric field does not depend on distance when considering infinite plates, as the field lines remain perpendicular and consistent across the surface. The conversation also touches on how the presence of a dielectric material affects the electric field between the plates, leading to a decrease in field strength due to polarization. Overall, the principles of superposition and symmetry in electric fields are emphasized throughout the discussion.
gracy
Messages
2,486
Reaction score
83
1.Homework Statement
Two large thin metal plates are parallel and close to each other. on their inner faces ,the plates have surface charge densities of opposites signs and magnitude 1.77 multiplied by 10^-11 coulomb per square meter.What is electric field
a)to the left of the plates
b)to the right of the plates
c)in between the plates

Homework Equations


[/B]E=σ/2ε0

The Attempt at a Solution


What is the proper orientation when the question says Two large thin metal plates are parallel and close to each other
I thought the following is correct
plane.png


But this is not correct.
The answer is Fields due to both the plates will be equal and opposite so net field will be zero.I can not differentiate between the cases that are
to the left of the plate (2) and between the plates
 
Physics news on Phys.org
In part (a), "to the left of the plates" refers to the far left region; that is, the region to the left of the left plate.
Likewise in part (b), "to the right of the plates" refers to the far right region; that is, the region to the right of the right plate.
 
  • Like
Likes gracy
TSny said:
In part (a), "to the left of the plates" refers to the far left region
Even if that's the case how come
gracy said:
The answer is Fields due to both the plates will be equal and opposite so net field will be zero.
 
I mean
Can electric field due to plate (2)go beyond the plate (1) i.e to the far left region
or even if it can ;would the electric field intensity of the charges of plate 2 be equal to that of plate one there in order to cancel the effect?
 
gracy said:
1.Homework Statement
Two large thin metal plates are parallel and close to each other. on their inner faces ,the plates have surface charge densities of opposites signs and magnitude 1.77 multiplied by 10^-11 coulomb per square meter.What is electric field
a)to the left of the plates
b)to the right of the plates
c)in between the plates

Homework Equations


[/B]E=σ/2ε0

The Attempt at a Solution


What is the proper orientation when the question says Two large thin metal plates are parallel and close to each other
I thought the following is correct
View attachment 88719

But this is not correct.
The answer is Fields due to both the plates will be equal and opposite so net field will be zero.I can not differentiate between the cases that are
to the left of the plate (2) and between the plates

Imagine one plate: When it is positively charged, the field lines emerge from it, and point away from the plate at both sides.
If the charge is negative, the field lines enter into the plate at both sides.
You can substitute the plates by planar distributions of charges. Both planes have their field everywhere, as shown in the picture. The orange lines are due to the positive charges, the blue lines belong to the negative ones. Apply he Superposition Principle: the resultant field is the sum of the fields of the individual planes.

twoplates3.jpg
 
  • Like
Likes gracy and DEvens
gracy said:
would the electric field intensity of the charges of plate 2 be equal to that of plate one there in order to cancel the effect?
 
If the charges per unit surface area are equal, the fields are of equal magnitude.
 
  • Like
Likes gracy
ehild said:
If the charges per unit surface area are equal, the fields are of equal magnitude.
But electric field also depends on r i.e distance from source charge
 
gracy said:
But electric field also depends on r i.e distance from source charge
NO, if the plates are infinite (at least their lateral sizes are much larger than the distance between them). You wrote that E=σ/(2ε0) !
 
  • #10
ehild said:
You wrote that E=σ/(2ε0) !
YES .I wrote that but I did not understand.
 
  • #11
ehild said:
if the plates are infinite (at least their lateral sizes are much larger than the distance between them)
But it's beyond them not between them
 
  • #12
ehild said:
NO, if the plates are infinite (at least their lateral sizes are much larger than the distance between them)
TSny said:
refers to the far left region
gracy said:
But it's beyond them not between them
 
  • #13
gracy said:
YES .I wrote that but I did not understand.
It is symmetry again. The charge is evenly distributed on the plane. At a point the fields of the individual charges add as vectors. The parallel components cancel and only the perpendicular components remain. As the plane is of infinite extension, the field is the same above each points. If you integrate the contribution of all charges you will get the same result, independently how far the point is from the plate.
 
  • #14
gracy said:
But it's beyond them not between them
The field of an infinite plate with even surface charge distribution is the same at both sides, only of opposite sign.
 
  • #15
Ok.One more question If these are metal plates ,why charges are spread throughout the surface;charges should reside on borders/outer surface
 
  • #16
gracy said:
Ok.One more question If these are metal plates ,why charges are spread throughout the surface;charges should reside on borders/outer surface
The plates were assumed of infinite sizes.
Even in case of real metal plates, not all charge reside along the borders. But it is true that they are spread on the surfaces.
 
  • #17
ehild said:
As the plane is of infinite extension, the field is the same above each points.
Could you please elaborate this?
 
  • #18
I am using this to understand
http://people.rit.edu/jdasps/jdainfo/313_tp/UniformlyChargedFinitePlane.pdf
 
  • #19
I spoke about infinite plate.
 
  • #20
Isn't there a little similarity between the two cases i.e finite plane when electric field is taken at mid point and infinite plate
 
  • #21
ehild said:
As the plane is of infinite extension, the field is the same above each points
I am not able to comprehend this.
 
  • #22
I am afraid ;It could be very silly question but I am serious about it.Will there be electric field intensity or force even when something comes in between(in the way of source charge to the point of interest) as in my question there is plate (1) in between the charges of plate 2(source charge) and the far left region but still electric field intensity is same as if nothing is in between.
 
  • #23
The superposition principle says that you can calculate the resultant field of several objects separately, as if the other objects were not there, and then sum the individual fields. One plate has its own field, the other one has its own field, too. And the field of two plates is the sum of these contributions.
 
  • Like
Likes gracy
  • #24
ehild said:
The superposition principle says that you can calculate the resultant field of several objects separately, as if the other objects were not there, and then sum the individual fields
Exactly What I wanted.Thanks @ehild
 
  • #25
gracy said:
Exactly What I wanted.Thanks @ehild
Watch this video
 
  • Like
Likes gracy
  • #26
Now only one thing is remaining
Why doesn't the electric field of an infinitely large plane depend on the distance from the plane?Please can you somehow make me understand.I will give my best.
 
  • #27
The electric field lines are perpendicular to the infinite plane if the surface charge density is the same everywhere. That comes from symmetry. The plane is the same in every direction, so the field lines can not bend in any direction.
Assume a Gaussian surface as a cylinder, with axis perpendicular to the plane and enclosing an area A of the plane. The flux of field lines is due to the bases only, and it is Φ = 2EA = Aσ/ε0, that is, E=σ/(ε0) regardless of the distance from the plane.
 
  • #28
ehild said:
it is Φ = 2EA = Aσ/ε0, that is, E=σ/(ε0) regardless of the distance from the plane
As far as derivation of this formula is concerned I understand .But I want to understand the concept,I want to understand how the effect of distance is nullified?I find this helpful.But still have something to ask.
https://www.quora.com/Why-doesnt-the-electric-field-of-an-infinitely-large-plane-depend-on-the-distance-from-the-plane
can I?
 
Last edited by a moderator:
  • #29
No field line crosses the side of the cylinder. It can be of any length, the flux across it is zero.
 
  • #30
ehild said:
No field line crosses the side of the cylinder. It can be of any length, the flux across it is zero.
Sorry
 
  • #31
gracy said:
Sorry
?
You can move away the bases of the cylinder to a longer distance, still the same field line will cross them. The flux does not depend on the length of the cylinder.

infiniteplane.JPG
 
  • Like
Likes gracy
  • #32
But from where is cylinder coming up?We were talking about plane/plate,right?
 
  • #33
gracy said:
But from where is cylinder coming up?We were talking about plane/plate,right?
And applying Gauss' Law.
 
  • Like
Likes gracy
  • #34
I know electric field due to uniformly charged infinite plane sheet is E=σ/(2ε0).Is this formula applicable always whether the sheet is conducting or non conducting?
 
  • #35
gracy said:
I know electric field due to uniformly charged infinite plane sheet is E=σ/(2ε0).Is this formula applicable always whether the sheet is conducting or non conducting?
If a uniformly charged sheet is infinite then, by symmetry, the component of the electric field parallel to the plate is zero everywhere. It does not matter whether the plate is conductive or not -- uniformly distributed charge will not flow to become non-uniform.
 
  • #36
jbriggs444 said:
It does not matter whether the plate is conductive or not -- uniformly distributed charge will not flow to become non-uniform.
So I can use the formula E=σ/(2ε0) in conducting as well as non conducting sheet,right?
 
  • #37
gracy said:
So I can use the formula E=σ/(2ε0) in conducting as well as non conducting sheet,right?
please say "yes"
 
  • #38
ehild said:
The superposition principle says that you can calculate the resultant field of several objects separately, as if the other objects were not there, and then sum the individual fields.
The why when dielectric is placed between the plates of capacitor there is decrease in electric field between the plates?
 
  • #39
gracy said:
The why when dielectric is placed between the plates of capacitor there is decrease in electric field between the plates?
Decrease with respect to what?
 
  • #40
ehild said:
Decrease with respect to what?
I meant electric field between the plates is less when dielectric is placed between them than when it is not.
 
  • #41
gracy said:
I meant electric field between the plates is less when dielectric is placed between them than when it is not.
Supposing the capacitor is connected to a battery. You insert dielectric between the plates.What happens to the electric field?
 
  • #42
gracy said:
I meant electric field between the plates is less when dielectric is placed between them than when it is not.
It happens because of the dielectric polarization. If instead of a dielectric, there were a conducting material, all the field would vanish.
 
Back
Top