Field of non-uniformly charged ring

In summary: The electric field points positive towards the center of the ring, with a magnitude of 4.7 C and a direction of 0 degrees.
  • #1
skyrolla
5
0

Homework Statement



A thin rubber ring of radius R lies in the xy-plane and is centered at the origin. The ring carries line charge density λ=λo*sin(Ø), with a constant λo with units C/m. define tan(Ø)=y/x. Calculate the magnitude and direction of the electric field E(z) created by the ring on points on the positive z axis.



Homework Equations



E=kq/r^2

The Attempt at a Solution



Symmetry implies only the component Ez will be nonzero along the z axis.
Desiring to integrate over Ø, my limits of integration will be 0 to pi.

Now dE=k*dq/r^2 with r=(R^2+z^2).

Q/R=λo*sin(Ø) so dQ=R*λo*cos(Ø) dØ

and dEz= k*R*λo*cos(Ø) dØ/(R^2+z^2)

however, integrating this over Ø results in multiplying everything by sin(pi)-sin(0) = 0, so clearly I've made at least one mistake here.

All help is appreciated!
 
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  • #2
the result must be zero for the sake of symmetri. Your result is correct (I think)
 
  • #3
Symmetry in the x and y directions makes sense, as an equal amount of ring and angle phi are distributed to both the positive and negative halves. However the field would certainly have a Z component at points along the Z axis, as the full ring exerts charge in either a positive or negative z direction.
 
  • #4
the charge is ditributed in iqual amount in each semi-circle but with defferent signs, so symmetry implies that the z component must be zero. However I now realize that there must be a component in the x-y plane
 
  • #5
skyrolla said:
Desiring to integrate over Ø, my limits of integration will be 0 to pi.

I think you should draw a picture...the angle [tex]\phi[/itex] is measured entirely in the xy-plane, and any point on the ring is given by [itex]x=R\cos\phi[/itex], [itex]y=R\sin\phi[/itex] and [itex]z=0[/itex].

If the ring is an entire circle, the limits on [itex]\phi[/itex] will be zero to [itex]2\pi[/itex]

Now dE=k*dq/r^2 with r=(R^2+z^2).

Q/R=λo*sin(Ø) so dQ=R*λo*cos(Ø) dØ

Not quite. By definition of linear charge density, [itex]dq=\lambda ds=\lambda_0 \sin\phi Rd\phi[/itex]

and dEz= k*R*λo*cos(Ø) dØ/(R^2+z^2)

No, not only should the cosine be a sine, but you haven't properly selected the z-component of [itex]d\textbf{E}[/itex].

Again, draw a picture...the field [itex]d\textbf{E}[/itex] from a tiny piece of the ring points from that piece, to the point on the z-axis at which it is measured...you want to find the z-component of that vector.

Even after you do the calculation properly, you will still find that [itex]E_z=0[/itex], however, if you also calculate the other components you should find that [itex]E_y\neq0[/itex].
 
  • #6
Thanks. After figuring out I had the wrong component, I was able to solve the problem.
 

FAQ: Field of non-uniformly charged ring

What is a field of non-uniformly charged ring?

The field of non-uniformly charged ring refers to the electric field created by a ring of charges that are not evenly distributed. This results in an electric field that varies in magnitude and direction at different points in space.

How is the electric field of a non-uniformly charged ring calculated?

The electric field of a non-uniformly charged ring is calculated using Coulomb's Law, which states that the electric field at a point is equal to the sum of the electric forces exerted by each individual charge at that point. This calculation can be complex and often requires the use of vector calculus.

What is the significance of the non-uniform distribution of charges in a ring?

The non-uniform distribution of charges in a ring allows for a more varied and interesting electric field. It can create regions of higher and lower electric field strength, which can have practical applications in areas such as particle accelerators and electric motors.

How does the electric field of a non-uniformly charged ring differ from that of a uniformly charged ring?

A uniformly charged ring has a constant electric field at all points in space, while a non-uniformly charged ring has a varying electric field. The electric field of a non-uniformly charged ring also has both radial and tangential components, while a uniformly charged ring only has a radial component.

What are some real-world examples of the field of non-uniformly charged rings?

The field of non-uniformly charged rings has many practical applications in fields such as physics, engineering, and chemistry. Some examples include particle accelerators, ion traps, and electric motors. It is also important in understanding the behavior of charged particles in a magnetic field.

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