M's Electric Field Calculation for a Uniformly Charged Wire

In summary, the problem involves finding the y-component of the electric field at y=3m on the y-axis due to a uniformly charged wire with a charge density of 4 microCoulombs/meter lying on the x-axis between x=1m and x=3m. The solution involves treating the wire as an infinite number of point charges and calculating the y-component of the electric field caused by each of these points. This can be done by integrating the vertical component of the electric field, which can be represented in terms of dx and the linear charge density. A diagram and an equation for sin \theta in terms of x may be needed for the integration.
  • #1
hmmm
1
0
A uniformly charged wire with a charge density of 4 microCoulombs/meter lies on the x-axis between x=1m and x=3m. What is the y-component of the corresponding electric field at y=3m on the y-axis?

I'm not really sure where to go with this. I want to treat the rod as an infinite number of point charges but I'm not sure how to calculate (y-component of) the electric field caused by each of these points.
 
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  • #2
suppose there is a point charge on the point y=3 , find the electric fireld there, actually the electric field there for suppose due to the charge on the X=1 m can be broken up into two components one along -x and another along +y axis..they can be computed separately by integrating ..in this case i think you only need to compute for the y aixs one...for the integration take elemental lengths dx for the wire...

glad to be of help,
Arpan Roy
royarpan@hotmail.com
 
  • #3
Note that, for each "dx" on one side of the point, there is a corresponding "dx" the same distance on the other side. The horizontal components of force of those will cancel but the vertical components will add.
 
  • #4
Since this problem is not symmetrical, the horizontal components of the [itex]\vec{E}[/itex] do not cancel. The easiest approach is probably to calculate the vertical ( [itex]\vec{E_y}[/itex] ) component seperately.

Draw a diagram of the situation with the given axis, and choose an arbitrary piece of charge [itex]dq[/itex] of the wire.

Come up with an equation for the corresponding electric field [itex]\vec{dE}[/itex] due to [itex]dq[/itex] at the point (0,3).

Figure a way to represent [itex]dq[/itex] in terms of [itex]dx[/itex] so you can integrate with respect to x.
(hint: it involves the linear charge density )

Break the equation into the vertical component of [itex]\vec{E}[/itex] and integrate with respect to x
(hint: [itex]\vec{dE_y} = \vec{dE} sin \theta[/itex] where theta is the angle between a line parallel to the x-axis and [itex]\vec{E}[/itex] )
(another hint: you will have to come up with an equation for [itex]sin \theta[/itex] in terms of x so you can integrate )

good luck :smile:
-MS
 
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1. What is a uniformly charged wire?

A uniformly charged wire is a wire that has an equal distribution of electric charge along its entire length. This means that the amount of charge per unit length is constant along the wire.

2. How is a uniformly charged wire different from a non-uniformly charged wire?

A non-uniformly charged wire has an uneven distribution of electric charge along its length, meaning that the amount of charge per unit length varies. This can result in different electric fields at different points along the wire.

3. What causes a wire to become uniformly charged?

A wire can become uniformly charged when it is connected to a power source, such as a battery, and a current flows through it. The movement of electrons results in an accumulation of charge along the wire, creating a uniform distribution.

4. What is the electric field around a uniformly charged wire?

The electric field around a uniformly charged wire is radial, meaning it extends outward in all directions from the wire. The strength of the electric field decreases as you move further away from the wire.

5. How can a uniformly charged wire be used in practical applications?

Uniformly charged wires can be used in circuits to transport electricity and power devices. They can also be used in electrostatic experiments and as components in electronic devices, such as capacitors and antennas.

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