Capacitance Between a Power Line and a Conducting Sphere
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Joel - 01 Jul 2009 16:38 GMT Hello,
I am trying to calculate the capacitance between an AC power line and a conducting sphere (0.1 m in diameter). The sphere is approx 1 meter away from the power line.
I would appreciate any suggestions.
Thanks.
-Joel
Wimpie - 01 Jul 2009 19:30 GMT > Hello, > [quoted text clipped - 7 lines] > > -Joel Hello Joel,
As D << (distance from sphere to long AC power line), you can use the formula for a sphere.
C = 2*pi*eps0*D result in Farad.
Best regards,
Wim PA3DJS www.tetech.nl Remove the obvious 3-letter combination in the PM
Joel - 02 Jul 2009 03:13 GMT > > Hello, > [quoted text clipped - 20 lines] > PA3DJSwww.tetech.nl > Remove the obvious 3-letter combination in the PM Hi Wim,
Thank you for your response. It looks like the equation is derived from V = Q/(4*Pi*eps0*r). It seems though that r (D in your equation) would be related to the distance the sphere is from the other object, not the diameter of the sphere. Why do you define D this way?
This equation is from electrostatics, why is it not necessary to consider the AC current through the power line?
-Joel
Don Kelly - 02 Jul 2009 05:16 GMT On Jul 1, 12:30 pm, Wimpie <wimabc...@tetech.nl> wrote:
> On 1 jul, 17:38, Joel <joel.stee...@gmail.com> wrote: > [quoted text clipped - 22 lines] > PA3DJSwww.tetech.nl > Remove the obvious 3-letter combination in the PM Hi Wim,
Thank you for your response. It looks like the equation is derived from V = Q/(4*Pi*eps0*r). It seems though that r (D in your equation) would be related to the distance the sphere is from the other object, not the diameter of the sphere. Why do you define D this way?
This equation is from electrostatics, why is it not necessary to consider the AC current through the power line?
-Joel ----- Capacitance is a geometrical relationship- the capacitance of the sphere with respect to the line is independent of the frequency. That doesn't mean the the relationship given is correct - some thought required here as the relationship apparently reduces a 3 dimensional problem to a 2 dimensional problem. It seems to me that the solution is a bit messier than indicated.
 Signature Don Kelly dhky@shawcross.ca remove the x to reply
Wimpie - 02 Jul 2009 15:00 GMT > > > Hello, > [quoted text clipped - 32 lines] > > -Joel Hello Joel,
D = diameter of sphere. Formula can be derived from the field distribution from a sphere in a sphere.
For a sphere in sphere capacitor: C = 4*pi*eps0/(1/ri - 1/ro)
ri = inner radius, ro is outer radius. ro > ri
When outer radius becomes very large, the formula converges to 2*pi*eps0*Diameter.
In your case diameter of sphere is small with respect to distance to power line, so the formula gives a reasonable value. Note that when there are other conductors clos to the sphere, capacitance may change as you get mutual capacitance issues. when other conductors are sufficiently far away, the formula is still a good estimation of capacitance between a sphere and a long wire.
Best regards,
Wim
Don Kelly - 05 Jul 2009 01:16 GMT On 2 jul, 04:13, Joel <joel.stee...@gmail.com> wrote:
> On Jul 1, 12:30 pm, Wimpie <wimabc...@tetech.nl> wrote: > [quoted text clipped - 36 lines] > > -Joel Hello Joel,
D = diameter of sphere. Formula can be derived from the field distribution from a sphere in a sphere.
For a sphere in sphere capacitor: C = 4*pi*eps0/(1/ri - 1/ro)
ri = inner radius, ro is outer radius. ro > ri
When outer radius becomes very large, the formula converges to 2*pi*eps0*Diameter.
In your case diameter of sphere is small with respect to distance to power line, so the formula gives a reasonable value. Note that when there are other conductors clos to the sphere, capacitance may change as you get mutual capacitance issues. when other conductors are sufficiently far away, the formula is still a good estimation of capacitance between a sphere and a long wire.
Best regards,
Wim ------------------------ The power line sphere problem is not a sphere in sphere problem. The power line is essentially a line of charge rather than an enclosing sphere of charge. The sphere to sphere case involves a radially symmetrical situation with uniform field in all directions. The line to sphere situation doesn't fit this model.
 Signature Don Kelly dhky@shawcross.ca remove the x to reply
Wimpie - 05 Jul 2009 10:09 GMT > On 2 jul, 04:13, Joel <joel.stee...@gmail.com> wrote: > [quoted text clipped - 73 lines] > d...@shawcross.ca > remove the x to reply Hello Don,
You right, there is no radial symmetry. When assuming: power line very large with respect to the sphere's diameter and distance between power line large with respect to sphere's diameter, most of int(E*ds) is close to the sphere.
Close to the sphere there is reasonable radial symmetry. So as a first estimate, you can use the capacitance for a sphere, where diameter of outer sphere goes to infinity.
When requiring better accuracy, you need to do the math, and also taking into account mutual capacitances via other structures.
Best regards,
Wim
Salmon Egg - 05 Jul 2009 20:02 GMT In article <fc5d36ce-19c7-4d37-9048-3d145dbefb6f@g1g2000yqh.googlegroups.com>,
> Hello Don, > [quoted text clipped - 9 lines] > When requiring better accuracy, you need to do the math, and also > taking into account mutual capacitances via other structures. There is an example given in Ramo and Whinnery's "Fields and Waves in Modern Radio." The same techniqu can be extended to cover this case.
The potential for a sphere in the presence of other conductors is going to be a sum of spherical harmonics of unknown coefficients. This sum has to equal the potential on the sphere and the cylindrical wire. There should be sufficient symmetry to set some of the harmonics to zero amplitude. Matching potentials at 1000 points will give a linear equation set. Even modest computers these days can handle the solution of such equations.
I am not saying that it would be easy but it is certainly feasible.
Bill
 Signature Most people go to college to get their missing high school education.
Don Kelly - 06 Jul 2009 01:51 GMT Hi, Wim,
We have two fields (a) a field E=rho/(2*pi*eps0)*r) due to the line (radial with respect to the line) and (b) a field E=q/(4*pi*eps0**r^2) due to the conductor charge. rho is the charge per unit length of the line and q is the charge on the sphere. Assuming the theoretical infinite line on which the line charge is based and assuming that the line/ sphere system is "isolated" then it appears that the sphere's charge will be rather large so that its field will dominate in the near region and your expression gives a valid limit based on completely ignoring the field due to the line charge (assuming that the line has some physical radius).
On that basis, I agree with you.
However, power "lines" invariably have more than one conductor (and or images)and also do involve a ground plane and images so I also have to agree with your caveat. If, as indicated, the sphere is small and its net charge is near 0, it will not disturb the field due to the line(s). Then only the first field above need be considered- naturally this will give a quite different result- but one than may well be more realistic. An approach using potential coefficients can be used as for a conductor instead of a sphere and either get the open circuit voltage for a given line charge or a short circuit current for sphere at ground potential (in this case it is per unit length so an approximation would be a conductor of length twice the sphere radius) . This, of course is an approximation that will give a different answer than your approximation based on the original question so all that I can suggest is something in between or the approach that Salmon Egg suggests.
Don dhky@shawcross.ca remove the x to reply
On 5 jul, 02:16, " Don Kelly" <d...@shaw.ca> wrote:
> "Wimpie" <wimabc...@tetech.nl> wrote in message > [quoted text clipped - 75 lines] > d...@shawcross.ca > remove the x to reply Hello Don,
You right, there is no radial symmetry. When assuming: power line very large with respect to the sphere's diameter and distance between power line large with respect to sphere's diameter, most of int(E*ds) is close to the sphere.
Close to the sphere there is reasonable radial symmetry. So as a first estimate, you can use the capacitance for a sphere, where diameter of outer sphere goes to infinity.
When requiring better accuracy, you need to do the math, and also taking into account mutual capacitances via other structures.
Best regards,
Wim
John Polasek - 10 Jul 2009 21:19 GMT >Hi, Wim, > [quoted text clipped - 31 lines] > >"W Merciless snip
I don't see any discussion of one essential feature, which is that what is being charged in a pair of capacitors like this is the space in between. Therefore, we should require that the sphere be grounded and also one leg of the powerline, which now makes it possible for a potential difference to stress space in between the sphere and wire. If the sphere is ungrounded, it becomes merely a spectator, and there is no meaningful attributable capacitance, simply a short circuit for the electric field. Or so it seems to me. Furthermore, it seems to be as if only the surface facing the wire would be involved, and thus a factor of 2 pi rather than 4 pi, not? It would be helpful if the OP would tell a little more about the experiment or what he is trying to accomplish. John Polasek
Salmon Egg - 11 Jul 2009 01:47 GMT > I don't see any discussion of one essential feature, which is that > what is being charged in a pair of capacitors like this is the space [quoted text clipped - 9 lines] > experiment or what he is trying to accomplish. > John Polasek Again, I refer to Smythe's Static and Dynamic Electricity. There are self capacitances and mutual capacitance, A sphere sitting by itself has a self capacitance to infinity. Add another conductor, and it has a self capacitance as well as a mutual capacitance to the sphere.
Bill
 Signature Most people go to college to get their missing high school education.
Don Kelly - 11 Jul 2009 04:51 GMT In fact a conducting sphere will distort the field in its vicinity and an isolated sphere will have some charge. Such a charge is needed to modify the field in its vicinity in order to make its surface an equipotential surface. In theory this will might lead to a series of charges. but for a small sphere these can be ignored. However, with or without the power line, the sphere has both self and mutual capacitance as Salmon Egg indicates. If the sphere is very small, then one can assume that it has 0 radius and has a potential due only to the fields of the line(s). A large sphere will distort the field in its vicinity. more than the surface facing the wire is involved.
The sphere-to line problem is a lot messier than a line to line problem.
Now if you are dealing with a grounded sphere, you can state that its potential is 0 and a short circuit current (AC case) will flow. Again this will distort the field. Generally for hazard work, the ground level field is found without any object then the capacitance of the object (sphere, truck, human, fence wire) and the ground level field are used to find the ground current. knowledge of the object's self and mutual capacitances is needed to determine this current (EPRI Power Transmission 345KV and up) This works for objects near ground.
Don Kelly dhky@shawcross.ca remove the x to reply
>>Hi, Wim, >> [quoted text clipped - 59 lines] > experiment or what he is trying to accomplish. > John Polasek Benj - 06 Jul 2009 21:26 GMT > Close to the sphere there is reasonable radial symmetry. So as a first > estimate, you can use the capacitance for a sphere, where diameter of > outer sphere goes to infinity. Wimpie nearly gets the prize. There is a lot of w.nking going on here, but a real scientist/engineer/physicist knows how to THINK about the problem and home in on some reasonable approximations. In this case there is a sphere and a power line forming a capacitor. If we think about this we can see that this situation is sort of half way between the self-capacitance (the sphere and infinity) and a spherical capacitor where the inner radius is .05m and the outer radius is 1 meter. [in essence the power line is expanded and stretched to form a terminal all about the inner sphere]. These represent the lower and upper limits of the capacitance of the capacitor in question. Interestingly, if you calculate this you find the self-capacitance is about 5.56 pf and that of the spherical capacitor is roughly 5.86 pf. Hence the capacitance of the system in question will be somewhere between those two values. I'm guessing the true value will be closer to the low value than the high one.
> When requiring better accuracy, you need to do the math, and also > taking into account mutual capacitance via other structures. Exactly. If you really need extreme accuracy, everything in the area must be specified and the actually capacitance calculated either numerically with a computer or if possible by some theoretical method (which probably won't take into account other structures).
Salmon Egg - 02 Jul 2009 21:28 GMT In article <017bc4a8-23a3-4397-b4aa-d7bf7e08ad85@e21g2000yqb.googlegroups.com>,
> Hello, > [quoted text clipped - 7 lines] > > -Joel My usual hint for this kind of a problem is to refer to William Smythe's Static and Dynamic Electricity. If this can be solved rigorously, it will be easiest by inversion.
The main complication is the diameter of the wire. Off hand, it seems that it would be difficult if not impossible t find a coordinate system in which a harmonic solution (one allowing separation of variables in a PDE) is possible.
There are many programs around for solving Laplace's equation numerically. It is probably easiest to use one that handles heat transfer.
Alternating current lines should not be a problem in the calculation. Just use the electrostatic value. By the time the wave nature along the wire becomes important the wire will be so far away that the contribution from such wire is negligible. Skin effect would be a tiny effect.
Bill
 Signature Most people go to college to get their missing high school education.
Joel - 02 Jul 2009 22:57 GMT > In article > <017bc4a8-23a3-4397-b4aa-d7bf7e08a...@e21g2000yqb.googlegroups.com>, [quoted text clipped - 34 lines] > -- > Most people go to college to get their missing high school education. Wim, Thank you for the explanation of the approximate solution approach.
Bill, I will try to get a copy of Static and Dynamic Electricity from the library. I am not sure, however, what the inversion approach is. What is it? Is this related to solving Laplace's equation?
Is Maple a good tool for this type of problem?
Thanks.
-Joel
Salmon Egg - 03 Jul 2009 00:58 GMT In article <36ddc5f2-94e4-456a-a5c9-d5a962c3f520@o9g2000prg.googlegroups.com>,
> Bill, I will try to get a copy of Static and Dynamic Electricity from > the library. I am not sure, however, what the inversion approach is. > What is it? Is this related to solving Laplace's equation? > > Is Maple a good tool for this type of problem? Smythe appears to be a highly mathematical book. Indeed it is. Smythe, however, seemed to take pride in that mathematicians taking his course did not do as well as physicists and engineers.
Smythe will describe the geometrical process of inversion. He shows that if there is a solution of Laplace's equation, inverting the solution will also be a solution.
Laplace's equation is: Laplacian V = 0. It describes the electric potential in space. Typically, the potentials, on the sphere and cylinder in your case is specified. Solving the equation gives you the potential away from these surfaces. Given a medium of uniform conductivity, Laplace's equation given the temperature on the sphere and cylinder will give the temperature in the medium. That is why the thermal solution can be used to give you the electric solution.
Good luck, Your work is cut out for you.
Bill
 Signature Most people go to college to get their missing high school education.
skysearcher@gmail.com - 16 Jul 2009 18:45 GMT Hello Joel,
I was thinking about your problem a little more, and I'm a little concerned that you're not taking the effect of the ground into consideration. I think that your approximation might be more accurate if you consider the system as two potentials located over an infinite ground plane - and maybe consider three capacitance values to be of interest for making a system of equations that you can solve: C1 between one potential and the ground, C2 between another potential and the ground, and C3 between the two potentials. You could then use image theory to work out another approximate solution for your problem.
Cheers, Eve
> Hello, > [quoted text clipped - 7 lines] > > -Joel skysearcher@gmail.com - 16 Jul 2009 19:31 GMT Oh - and if you're just looking for a *really* rough estimate value, you might also look into the Method of Curvilinear Squares, which is a field mapping technique. I'd only use this for the case where you're considering your problem system to be 2D with a circular slice of the power line (with some approximate charge) and a slice of the sphere. Yay estimations!! =D
> Hello, > [quoted text clipped - 7 lines] > > -Joel
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