Non symmetric case of Ampere's law

In summary, Ampere's law is commonly used to evaluate the magnetic field at a distance r from an infinite current carrying wire. However, it can also be used for non-symmetric scenarios such as a finite current carrying loop. While solving for these non-symmetric cases may involve the second term of Ampere's law, it cannot be used for a finite wire as it would violate the continuity equation. Instead, the issue can be resolved by considering charge accumulation at the ends of the wire and incorporating the concept of displacement current.
  • #1
ubergewehr273
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When we use Ampere's law, the most basic case that of an infinite current carrying wire is taken whose magnetic field is evaluated at a distance r from the wire. However there's nothing wrong in using the law for non symmetric scenarios. If this is the case how do you explain the B field at a distance r from a "finite" current carrying wire using Ampere's law ?
 
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  • #2
You cannot have a finite current carrying wire. It would violate the continuity equation at the ends.

You could have a finite current carrying loop. Perhaps that is what you meant.
 
  • #3
Dale said:
You cannot have a finite current carrying wire. It would violate the continuity equation at the ends.
But in my senior class, we did derivations based on finding B field at a distance r from a finite section of a wire whose ends subtend angles ##\theta_{1}## and ##\theta_{2}## at the point. Is it correct to find the B field due to a finite portion of an infinite current carrying wire?
 
  • #4
Ashes Panigrahi said:
But in my senior class, we did derivations based on finding B field at a distance r from a finite section of a wire whose ends subtend angles ##\theta_{1}## and ##\theta_{2}## at the point. Is it correct to find the B field due to a finite portion of an infinite current carrying wire?

But what did you use? Ampere's law, or Biot-Savart Law?

Zz.
 
  • #5
ZapperZ said:
But what did you use? Ampere's law, or Biot-Savart Law?

Zz.
We used Biot savart law, but how do I do it using Ampere's law?
 
  • #6
Ashes Panigrahi said:
We used Biot savart law, but how do I do it using Ampere's law?

Not easily. You need to learn numerical analysis, because you have to solve it numerically.

Again, refer back to Gauss's law. Did you ever solve for the E-field of a finite line charge using Gauss's law?

The reason why Gauss's law and Ampere's law are used in highly-symmetric situations is because you have to do very minimal calculus due to the geometry of the field. Otherwise, you do not have an analytical solution and you will have to solve it numerically.

If you continue in physics and end up doing advanced E&M using something like the Jackson's text, you WILL solve not only non-symmetric sources, but also solving for "off-axis" locations. Try solving the field for a circular loop of current, but NOT just along the axis of the loop. It is not easy, and you'll end up with an infinite series.

So my advice at the moment is, enjoy and appreciate these simpler situations while you can. It gets real ugly real soon enough.

Zz.
 
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  • #7
ZapperZ said:
Not easily. You need to learn numerical analysis, because you have to solve it numerically.

Again, refer back to Gauss's law. Did you ever solve for the E-field of a finite line charge using Gauss's law?

The reason why Gauss's law and Ampere's law are used in highly-symmetric situations is because you have to do very minimal calculus due to the geometry of the field. Otherwise, you do not have an analytical solution and you will have to solve it numerically.

If you continue in physics and end up doing advanced E&M using something like the Jackson's text, you WILL solve not only non-symmetric sources, but also solving for "off-axis" locations. Try solving the field for a circular loop of current, but NOT just along the axis of the loop. It is not easy, and you'll end up with an infinite series.

So my advice at the moment is, enjoy and appreciate these simpler situations while you can. It gets real ugly real soon enough.

Zz.
Thanks for the advice but just out of curiosity does finding for such a non symmetric case involve the second term of ampere's law ? Because well let's just say that charge accumulation takes place at the ends of the finite wire and this would induce a changing electric field till ##\vec E## becomes zero. Is this right?
 
  • #8
ubergewehr273 said:
Thanks for the advice but just out of curiosity does finding for such a non symmetric case involve the second term of ampere's law ? Because well let's just say that charge accumulation takes place at the ends of the finite wire and this would induce a changing electric field till ##\vec E## becomes zero. Is this right?

Actually, no. That is the displacement current, and it has more to do with the transient effects in space when a capacitor is charging or discharging. If you are curious on why that term has to be there, read ahead on the topic of displacement current.

Zz.
 
  • #9
ZapperZ said:
Actually, no. That is the displacement current, and it has more to do with the transient effects in space when a capacitor is charging or discharging. If you are curious on why that term has to be there, read ahead on the topic of displacement current.

Zz.
Isn't the case that I described above a scenario of transient effect ?
 
  • #10
ubergewehr273 said:
Isn't the case that I described above a scenario of transient effect ?

Not from the way you described it. While it is due to a changing E-field, it has more to do with what happens at a break in the circuit during the transient period, i.e. if the surface bounded by the Amperian loop isn't crossed by the real current in the wire. The changing E-field can eventually be related to this "displacement current" if you wish, but the displacement current is the extra term in Ampere's law.

Zz.
 
  • #11
ubergewehr273 said:
We used Biot savart law, but how do I do it using Ampere's law?
In addition to what @ZapperZ said, it actually cannot be done with Ampere’s law. The violation of the continuity equation causes a serious problem.

Recall that you define a loop, then define a surface whose boundary is the loop, and that it can be any surface with the boundary. If you have a finite wire and a loop around the wire, then you can choose a surface crossing the wire or a surface going around the wire. Both surfaces are valid, but the current is different.

This can be fixed by having charge accumulate at the ends and create a dipole E field, and adding the displacement term to Amperes law.
 
  • #12
Dale said:
In addition to what @ZapperZ said, it actually cannot be done with Ampere’s law. The violation of the continuity equation causes a serious problem.
While calculating the B field using biot savart law, we never considered violation of the continuity equation but yet the approach was right. Or was it?
Dale said:
or a surface going around the wire. Both surfaces are valid, but the current is different.
Could you elaborate on the point of surface going around the wire. Also how is the current different in both cases ?
 
  • #13
ubergewehr273 said:
While calculating the B field using biot savart law, we never considered violation of the continuity equation but yet the approach was right. Or was it?
The Biot Savart law doesn’t have the same mathematical issue; the results are mathematically well defined but non-physical because of the violation of the continuity equation.

ubergewehr273 said:
Could you elaborate on the point of surface going around the wire. Also how is the current different in both cases ?
For example
Qc9pl.png


The current is different through the two surfaces, ##S_1## and ##S_2##
 

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  • #14
Dale said:
The Biot Savart law doesn’t have the same mathematical issue; the results are mathematically well defined but non-physical because of the violation of the continuity equation.

For exampleView attachment 218563

The current is different through the two surfaces, ##S_1## and ##S_2##
Thanks for the details.
P.S. Which textbook is the image from?
 
  • #15
Dale said:
The Biot Savart law doesn’t have the same mathematical issue; the results are mathematically well defined but non-physical because of the violation of the continuity equation.
Why aren't the results of Ampere's law "physical" and otherwise for Biot savart law ? Isn't the former derived from the latter ?
 
  • #16
ubergewehr273 said:
Why aren't the results of Ampere's law "physical" and otherwise for Biot savart law ?
They are non-physical because you are modeling a non-physical scenario. You cannot have a current which just stops, that is non physical. So any model which takes that non physical scenario as an input will produce non physical output.
 
  • #17
Dale said:
They are non-physical because you are modeling a non-physical scenario. You cannot have a current which just stops, that is non physical. So any model which takes that non physical scenario as an input will produce non physical output.
Mathematically speaking shouldn't Ampere's law provide the same result as Biot savart law?
 
  • #18
ubergewehr273 said:
Mathematically speaking shouldn't Ampere's law provide the same result as Biot savart law?
They are not mathematically identical, so no. Under specific conditions they are equivalent, but those circumstances do not include this non-physical scenario.
 

1) What is the non-symmetric case of Ampere's law?

The non-symmetric case of Ampere's law refers to a situation in which the current-carrying conductor is not aligned with the closed loop used in the application of Ampere's law. This means that the conductor is not parallel or perpendicular to the loop, resulting in a non-uniform magnetic field.

2) How does the non-symmetric case affect the application of Ampere's law?

In the non-symmetric case, the magnetic field is not constant along the closed loop, making the application of Ampere's law more complex. The law must be applied in small segments of the loop and then integrated to find the total magnetic field.

3) What are some examples of the non-symmetric case of Ampere's law?

One example is a current-carrying wire that is bent at an angle, creating a non-uniform magnetic field. Another example is a solenoid with a current-carrying wire passing through it at an angle, causing a non-symmetric magnetic field.

4) How is the non-symmetric case of Ampere's law solved?

The non-symmetric case can be solved by using the Biot-Savart law, which calculates the magnetic field at a point due to a small segment of current-carrying wire. This calculation is then repeated for each segment of the loop and integrated to find the total magnetic field.

5) What are the practical applications of the non-symmetric case of Ampere's law?

The non-symmetric case of Ampere's law is important in understanding and designing complex electrical systems, such as motors, generators, and transformers. It is also used in the study of electromagnetism and in the development of new technologies that rely on magnetic fields.

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