Charge Particle Trajectory: How to Find It

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    Charge Trajectory
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Discussion Overview

The discussion revolves around the trajectory of charged particles in electric fields, particularly focusing on how these trajectories relate to electric field lines. Participants explore various scenarios involving charged particles, the Lorentz force, and the impact of initial conditions on particle motion.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • Some participants note that field lines do not always represent the trajectory of a charged particle in a field, prompting questions about how to determine the actual trajectory.
  • One participant questions how a negatively charged test particle would behave if released from a positive charge, particularly in relation to field lines.
  • There is discussion about the Lorentz force and its implications for particle motion, with some participants asserting that a particle released from rest will initially follow the electric field lines.
  • Others argue that if a particle has an initial velocity, it may not follow the field lines, especially if the field is curved.
  • Participants discuss the need for an acceleration component orthogonal to the field line for a particle to follow a curved path, which is not present by definition of the field line.
  • Some suggest that solving the equations of motion, potentially using the Lagrangian approach, could provide insights into the trajectory of the charged particle.
  • There is a comparison made between charged particle motion in electric fields and projectile motion under gravity, with some participants expressing skepticism about the applicability of this analogy.
  • One participant mentions that for an electron released from rest, the trajectory will closely follow the field lines, but deviations may occur for larger masses or more complex scenarios.
  • Another participant suggests that to make a charged particle follow field lines, some form of resistance, such as collisions with residual gas, would be necessary.

Areas of Agreement / Disagreement

Participants express multiple competing views regarding the relationship between charged particle trajectories and electric field lines. There is no consensus on how accurately particles follow field lines under various conditions, and the discussion remains unresolved on several points.

Contextual Notes

Participants highlight limitations in their understanding of the Lorentz force and the conditions under which charged particles deviate from field lines. The discussion also touches on the complexity of solving equations of motion for charged particles in electric fields, indicating potential challenges in obtaining analytical solutions.

UMath1
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My textbook said that field lines do not always represent the trajectory of a charged particle in a field. How would you find the trajectory then?
 
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What points? Let's say you had a field created by one positive charge and one negative charge. If a negative test charge would not flow along the field line from positive to negative, how would it flow if it started at the positive end?
 
UMath1 said:
My textbook said that field lines do not always represent the trajectory of a charged particle in a field. How would you find the trajectory then?

What field? Electric or Magnetic or both? A static field or a changing field? What it the initial trajectory of the charged particle with respect to the field(s)? Are you familiar with the Lorentz Force? Can you show us that equation?
 
Electrostatic field. The negatively charged particle is just let go from the positive end.

I am not familiar with the lorentz force.
 
UMath1 said:
Electrostatic field. The negatively charged particle is just let go from the positive end.

I am not familiar with the lorentz force.

The Lorentz Force is the vector force acting on a charged particle that is moving in magnetic and/or Electric fields:

[tex]F = qE + q(vxB)[/tex]

If you just release a charged particle from rest, yes it will follow the E-field lines, because that's the direction of the Lorentz force when there is no B field.
 
So only if it has an initial velocity, it won't follow the field lines?
 
If you shot the charged particle into a region of E-filed that was perpendicular to the motion, then the particle would follow a curved path, correct?
 
Yes
 
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but if you shot it in the direction of a field line, then?
 
  • #10
UMath1 said:
but if you shot it in the direction of a field line, then?

Now that you've seen the definition of the Lorentz force, what do you think? F=ma, right?
 
  • #11
Right, but the direction of the force constantly varies if the field line is curved as it often is between positive and negative charges. It should move tangent to the field line initially. But I am not sure if after it moves in that direction, it will still be acted on by the same field line.
 
  • #12
To find the equation of motion just write down F=ma for the system and solve. Alternatively you can use the Lagrangian to determine the equation of motion.
 
  • #13
berkeman said:
If you just release a charged particle from rest, yes it will follow the E-field lines, because that's the direction of the Lorentz force when there is no B field.
It will do that "in the first moment", but it won't do that in general, even if it starts at rest. If the field lines are curved, the particle won't follow them.
UMath1 said:
Right, but the direction of the force constantly varies if the field line is curved as it often is between positive and negative charges. It should move tangent to the field line initially. But I am not sure if after it moves in that direction, it will still be acted on by the same field line.
Your doubt is right here. To follow a curved line it would need an acceleration component orthogonal to the field line, but that does not exist by definition of the field line.

A magnetic field can change the trajectory, but in general it won't make particles follow any field lines.
 
  • #14
mfb said:
It will do that "in the first moment", but it won't do that in general, even if it starts at rest. If the field lines are curved, the particle won't follow them.

Yes, sorry. In his initial example, I thought he was talking about straight E-field lines.
 
  • #15
mfb said:
Your doubt is right here. To follow a curved line it would need an acceleration component orthogonal to the field line, but that does not exist by definition of the field line.

So how would it move?
 
  • #16
UMath1 said:
So how would it move?

Have you solved a projectile motion in gravity? I find it hard to believe that you are doing charged particle in electric field and not have already tackled a projectile motion. If you have, then you really should go back and look at it, because, believe it or not, you already know how to solve this.

If you look at the projectile motion, the "field lines" are always pointing down, because this is the field lines for gravity. If you simple let go of a mass, how does it move? Does it move in the same direction of the "field lines"?

But what if you shoot the mass out at some angle with respect to the horizontal? How does it move then?

Look at the electrostatic problem and see why it is no different.

Zz.
 
  • #17
But the field lines for gravity point in a constant direction. When you have a positive and negative charge, the field lines take a curved path. If a charge carrier is released in the direction of one of these curved lines, a force tangent to the curved line will act on it causing acceleration tangent to the line. But after that I don't see where the force will act on it.
 
  • #18
UMath1 said:
But the field lines for gravity point in a constant direction. When you have a positive and negative charge, the field lines take a curved path. If a charge carrier is released in the direction of one of these curved lines, a force tangent to the curved line will act on it causing acceleration tangent to the line. But after that I don't see where the force will act on it.

So let me get this clear. If I give you an electrostatic field that is constant everywhere, and looks just like a gravity field, you can solve this easily, correct?

Zz.
 
  • #19
yes
 
  • #20
UMath1 said:
yes

Fine.

Now tell me exactly the field lines that you have.

Zz.
 
  • #21
Lets say I release a negative charge from the top of the blue charge.
250px-VFPt_dipole_electric.svg.png
 
  • #22
UMath1 said:
Lets say I release a negative charge from the top of the blue charge.
View attachment 89785

I don't understand what you mean by "... from the top of the blue charge..."

Regardless of that, when you have a field such as this, for an electron, the trajectory will closely follow the field lines when you release the charge from rest. However, the larger the mass, the longer the path, and the more accurate you want your answer, the more it will deviate from these field lines. If you want an accurate modeling of such path, you will have to solve the equation of motion for such a system, and it may not be an analytical solution (i.e. you might only be able to solve it numerically).

It is why you were never asked to solve for the path of a spacecraft going through the solar system when you dealt with gravity.

Zz.
 
  • #23
ZapperZ said:
Regardless of that, when you have a field such as this, for an electron, the trajectory will closely follow the field lines when you release the charge from rest.
In general it will not.
Using the position description of post #21 and some rough estimate on the positions, I would expect our test mass to be unbound. It won't follow the field lines - it will not even stay in the picture, but escape nearly vertically, crossing field lines nearly orthogonally on its way out.

To make the charged particle follow field lines, you would need some resistance (like residual gas for collisions).

The mass is not relevant here, it just changes the timescale, but not the result.
 

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