Electric Field outside a cylinder

AI Thread Summary
The discussion revolves around calculating the electric field and charge per unit length of a cylindrical wire using Gauss' law. Initially, the electric field outside the wire is given as 40 kV/m, leading to a charge per unit length of approximately 1.112 x 10^-9 C/m. Participants explore how to find the electric field at a radius of 2 mm and the potential difference between two points, ultimately arriving at a potential difference of -27.73 V, which is validated through energy considerations. The conversation shifts to a coaxial cable scenario, where the charge on the inner surface of a cylindrical sheath is discussed, concluding that it will be negative to offset the positive charge of the wire, ensuring the electric field inside the sheath is zero. The calculations and principles discussed emphasize the application of Gauss' law throughout the problem-solving process.
t_n_p
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Homework Statement
Immediately outside a very long cylindrical wire of radius Ri = 0.5 mm, the electric field (in air) is E = 40 kV/m,
away from the wire’s surface. Use clearly labelled diagrams, explain any principle/law used, for all parts.
a) What is the charge per unit length along the wire?

The attempt at a solution

I'm not sure which formula I should apply, can somebody direct me? :confused:
 
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There's an important law that relates the charge to electric flux (which is field strength*area)... can you think of the law? That's what you need to use here.
 
Gausses?.....
 
t_n_p said:
Gausses?.....

Yes. :smile: That's what you need to use here. Take an arbitrary length x of the cylinder... Then use gauss' law over that cylinder over that length... You should be able to solve for charge per unit length...
 
I'm still confused. Which formula exactly should I be using?
 
t_n_p said:
I'm still confused. Which formula exactly should I be using?

It's Gauss' law... what does Gauss' law say?
 
Ok, so I should be using

Φ = EA = Q/εo
= 40*2*pi*0.0005*x = Q/εo

Therefore Q/x=1.112*10^-12 C/m

Correct?
 
t_n_p said:
Ok, so I should be using

Φ = EA = Q/εo
= 40*2*pi*0.0005*x = Q/εo

Therefore Q/x=1.112*10^-12 C/m

Correct?

Yes, looks correct to me.
 
Cool!
How about if I wanted to find the field at a radius of 2mm from the centre of the wire?

Using Gauss again, I know all values but x (length of wire), Q, and E (which is what I want to find).

If I use the Q/x value I just found out from the previous question, I get 1.24*10^-25 V/m.

Sounds like quite a far out number, could it be right?
 
  • #10
t_n_p said:
Cool!
How about if I wanted to find the field at a radius of 2mm from the centre of the wire?

Using Gauss again, I know all values but x (length of wire), Q, and E (which is what I want to find).

If I use the Q/x value I just found out from the previous question, I get 1.24*10^-25 V/m.

Sounds like quite a far out number, could it be right?

Oops... before for E, you needed to use 40,000... not 40 (you have to convert to volts). So that would give Q/x=1.112*10^-9 C/m

For this part, I get 10,000V/m or 10kv/m.
 
  • #11
Good spot with the kV/m!

I got 10kv/m for part 2 as well, just a silly arithmatic error!

Thanks ALOT!
 
  • #12
t_n_p said:
Good spot with the kV/m!

I got 10kv/m for part 2 as well, just a silly arithmatic error!

Thanks ALOT!

You're welcome.
 
  • #13
Managed to do one part by myself (good acheivement by my standards) before being getting stuck again.

How is it possible to calculate the potential diff betweem r=2 and r=0.5?
As the length of the wire is supposedly the same and the E for r=0.5 is 40000 and the E for r=2 is 10000, is it simply 40000-10000 = 30000V?
 
  • #14
t_n_p said:
Managed to do one part by myself (good acheivement by my standards) before being getting stuck again.

How is it possible to calculate the potential diff betweem r=2 and r=0.5?
As the length of the wire is supposedly the same and the E for r=0.5 is 40000 and the E for r=2 is 10000, is it simply 40000-10000 = 30000V?

No. The potential diff is found using an integral. Your text should have that integral.
 
  • #15
I think this is the one?

http://img245.imageshack.us/img245/1862/untitledkr7.jpg

where f = 2
and i = 0.5

I'm not sure how to do the actual mathematics part of it and there is no example in the book.

edit: my understanding is that the test charge is moving parallel to E and hence angle will be 0degrees.
 
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  • #16
t_n_p said:
I think this is the one?

http://img245.imageshack.us/img245/1862/untitledkr7.jpg

where f = 2
and i = 0.5

I'm not sure how to do the actual mathematics part of it and there is no example in the book.

edit: my understanding is that the test charge is moving parallel to E and hence angle will be 0degrees.

Yes, you take a path radially outward from the wire... and E is parallel to that path. cos 0=1. So it is just -integral Edr
 
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  • #17
So basically...
next steps

=-∫Edr (with terminals 0.5 and 2)

=-∫Er (with terminals 0.5 and 2)

= -([E*0.5]-[E*2])

Do I use the corresponding E values for each radial distance?

Am I even on the right track?
 
  • #18
t_n_p said:
So basically...
next steps

=-∫Edr (with terminals 0.5 and 2)

=-∫Er (with terminals 0.5 and 2)

= -([E*0.5]-[E*2])

Do I use the corresponding E values for each radial distance?

Am I even on the right track?

No, you need a formula for E in terms of r... ie you need E(r)... then you'd calculate:

=-∫E(r)dr (with terminals 0.5 and 2)
 
  • #19
Well in my textbook I have found

E=(λ)/(2pi*εo*r)

where lambda is Q/x.

Is this equation still suitable even though lambda has been brought in?
 
  • #20
t_n_p said:
Well in my textbook I have found

E=(λ)/(2pi*εo*r)

where lambda is Q/x.

Is this equation still suitable even though lambda has been brought in?

Not sure... do exactly what you did to calculate the field at 2mm... except instead of 2mm just leave the radius as r. So solve for E, and you'll have an expression in terms of r.
 
  • #21
Yeah the formula: E=(λ)/(2pi*εo*r)

Is what I did to find E @ 2mm. Just wondering if I use the lambda value (Q/x) I found in the first question (i.e. 1.112*10^-9)

If yes, then my equation in terms of E and r will look like this..

E = (1.112*10^-9)*(1/5.56r)

hence
-integral Edr becomes
-∫[(1.112*10^-9)*(1/5.56r)]dr

solving leads to...
Vf-Vi = -3.75*10^10.
Is a negative figure feasible? (if not, will swapping the terminals, i.e. make f=0.5 and i=2, fix this?)
 
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  • #22
t_n_p said:
Yeah the formula: E=(λ)/(2pi*εo*r)

Is what I did to find E @ 2mm. Just wondering if I use the lambda value (Q/x) I found in the first question (i.e. 1.112*10^-9)

If yes, then my equation in terms of E and r will look like this..

E = (1.112*10^-9)*(1/5.56r)

The denominator seems off by a power of 10...

I get E = 20/r

What is -∫(20/r)dr

Get the formula first before you plug in the numbers...
 
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  • #23
silly me.

E = (1.112*10^-9)*(1/5.56*10^-11*r)
E = 20/r

Vf-Vi = -20∫r dr with terminals (0.5 and 2)
Vf-Vi = -20 [r²/2] with terminals (0.5 and 2)
Vf-Vi = -20 [2-0.125]
Vf-Vi = -37.5V

Hope that's right!
 
  • #24
t_n_p said:
silly me.

E = (1.112*10^-9)*(1/5.56*10^-11*r)
E = 20/r

Vf-Vi = -20∫r dr with terminals (0.5 and 2)
Vf-Vi = -20 [r²/2] with terminals (0.5 and 2)
Vf-Vi = -20 [2-0.125]
Vf-Vi = -37.5V

Hope that's right!

Nope. :wink: You should be integrating 1/r not r. also remember to convert mm to m.
 
  • #25
So many silly errors!
when u say convert mm to m, you mean the terminals correct?

Changing all that gives final answer -27.73V
Still unsure if negative value is valid!
 
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  • #26
t_n_p said:
So many silly errors!
when u say convert mm to m, you mean the terminals correct?

Yeah.

Don't feel bad about the errors. With experience, you'll make less and less of them.
 
  • #27
Sorry edited my previous post, just as you were writing your reply. Hope I'm correct!
 
  • #28
t_n_p said:
So many silly errors!
when u say convert mm to m, you mean the terminals correct?

Changing all that gives final answer -27.73V
Still unsure if negative value is valid!

Yup, that's what I got also. I'm pretty sure the negative is valid.

One thing I was wrong about... you didn't have to convert the terminals to m... you'll still get the right answer... because it is the ratio of the lengths that matters... but converting to m is better just in case...

One way to check that the negative makes sense is... think about what is happening with energy... since the field E is positive in the outward direction (direction of increasing r)... that means that as a positive test charge moves outward, the field E does positive work on it... when positive work is done on the test charge, that means it is gaining kinetic energy... but another way of looking at this is... potential energy is being converted to kinetic energy... so the positive test charge loses potential energy going outward, so it makes sense that we get a negative for potential difference...
 
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  • #29
learningphysics said:
Yup, that's what I got also. I'm pretty sure the negative is valid.

One thing I was wrong about... you didn't have to convert the terminals to m... you'll still get the right answer... because it is the ratio of the lengths that matters... but converting to m is better just in case...

Thanks! It seems as though I am once again stumped.

A hollow cylinderical metal sheath with inner radius 2mm is now placed around the wire to form a coaxial cable. what will be the charge on the inner surface of this sheath?

Really not sure where to start :confused::bugeye:
 
  • #30
t_n_p said:
Thanks! It seems as though I am once again stumped.

A hollow cylinderical metal sheath with inner radius 2mm is now placed around the wire to form a coaxial cable. what will be the charge on the inner surface of this sheath?

Really not sure where to start :confused::bugeye:

The cylindrical sheath is a conductor... how do the charges arrange themselves on a conductor... your calclations from before are still valid here... the field at 2mm is still the same (just right before the sheath). What's the field on the inside of the sheath (between the inner and outer radius)?
 
  • #31
Well, you say the sheath is a conductor.
So I would say that the field on the inside of the sheath between the inner and outer radius is negative.

Where do I go from there?
 
  • #32
you say the field within the material is negative ...
do you mean pointed inward?
what would happen to an electron in that material,
if there was an inward-pointing E-field?
 
  • #33
well e fields go from + to -, so if there was an inward pointing e field and electrons are in the material, they would be repelled?
 
  • #34
?? repelled ? ... from what ?
(they can't see what kind of charge is on the central wire)
do they move inward or outward?
(the Force on a qharge = qE ...)
 
  • #35
Sorry ...
what direction *did* E (used to) point ,
before the sheath was put there?

Where would an electron go (they move freely, in a conductor)
if it was immersed in such a 10 kV/m field ?
 
  • #36
Before the sheath was there, E was away from wires surface.

Hence electron would be attracted to the wire?
 
  • #37
yes ... (there are +++Q on the wire, that's why E points away from it)
so the electrons end up on the
inside of the sheath , or the outside of the sheath?

When do they stop accumulating there?

that is, what causes them to go there,
and what has to be =0
before they'll stop moving to the inside?
 
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  • #38
They want to move away from the wire, but at the same time, there are electrons inside the sheath so they will end up on the outside of the sheath. meaning the charge on the inner surface of the sheath will be neutral?
 
  • #39
??

positive Qharges, the ones that are ON the inner wire,
are "trying" to get away from the other + charges on the wire,
(trying to move along E, to location of lower Potential where +q has low PE).

But these electrons are in the sheath at 2.1 mm,
and are trying to move TOWARD the ++Q on the wire,
(against E, to location of higher Potential where -q would have LOW PE).

They'll keep moving inward until:
a) there is zero TOTAL charge inside of their location
b) there is zero E-field at the place that they are at
c) the Potential is the same to their inside as to their outside.

All 3 are the same condition. Gauss relates a) to b) .
 
  • #40
so electrons move toward the wire. Does that make the charge on the inner surface negative?
 
  • #41
yes.

And you know how much neg. charge it will take (/meter length)
to offset the charge on the inner wire.
 
  • #42
I don't get what you mean by offset the charge on the inner wire. I just want to figure out the charge on the inner surface of the sheath..

Are they the same thing?
 
  • #43
Gauss says that the total E outward thru surface A
equals the total Qharge enclosed by the surface A.

for E to be 0, the total Q inside has to add up to zero.
positives and negatives offset ...
 
  • #44
t_n_p said:
I don't get what you mean by offset the charge on the inner wire. I just want to figure out the charge on the inner surface of the sheath..

Are they the same thing?

The charge on the inner surface of the sheath offsets the charge on the wire (due to Gauss law as lightgrav explained)... so Q/x for the sheath is the negative of Q/x for the wire... From that you can get the Q/area

Or here's a different way to do it. Take a tiny cylindrical volume (or any shape doesn't matter) that goes through the inner surface of the sheath. So one end is inside the sheath and the other end is outside... Do gauss' law over that volume... The field inside the sheath is 0. The field outside, you already calculated before at 2mm. That will also give the same answer...
 
  • #45
I am really, really confused now!

Q/x of sheath = -Q/x for wire = -1.112*10^-12 C/m

Then I use Gauss?
But I want to find Q?:confused::confused::confused:
 
  • #46
t_n_p said:
I am really, really confused now!

Q/x of sheath = -Q/x for wire = -1.112*10^-12 C/m

Then I use Gauss?
But I want to find Q?:confused::confused::confused:

Total Q? Are you sure they aren't asking for charge per unit length or charge per unit area?
 
  • #47
the exact question..

"A hollow cylindrical metal sheath with inner radius 2mm is now placed around the wire, to form a coaxial cable. What will be the charge on the inner surface of this sheath?"

I'm not sure if they are after a qualitative or quantitative answer, how do you interpret the question?
 
  • #48
so the rest of the electrons are not attracted toward the inside.
Q/x is as good as you can do.

(unless you want to find the charge per Area...)

Gauss is not a new foundation equation,
it deals with the same info as Coulomb's law,
so in situations like this one (symmetry!)
you often don't actually have to COMPUTE a new result.

it is sort of like weighing a mass on a spring using Newton's 3rd law;
once you know the Force by the spring, the Force by gravity is obvious.
 
  • #49
t_n_p said:
the exact question..

"A hollow cylindrical metal sheath with inner radius 2mm is now placed around the wire, to form a coaxial cable. What will be the charge on the inner surface of this sheath?"

I'm not sure if they are after a qualitative or quantitative answer, how do you interpret the question?

If they gave the length of the cylinder (or the initial wire) then you could give a total Q... I assumed that it was an infinitely long wire and cylinder... in which case charge per unit length, or charge per unit area is the only type of answer you can give.
 
  • #50
Yeah in the initial question the wire is described as "very long", however the question states nothing about area or length. :confused:
 
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