Distance of Closest Approach Between Two Charges

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Discussion Overview

The discussion revolves around the concept of the distance of closest approach between two charges, specifically focusing on the dynamics of charged particles under electrostatic repulsion. Participants explore scenarios involving fixed and moving charges, the conditions under which charges stop moving, and the implications of impact parameters on trajectories.

Discussion Character

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

Main Points Raised

  • One participant describes a scenario where a charge ##q_1## is fired towards a fixed charge ##q_0##, questioning how ##q_0## can remain stationary despite the repulsive forces.
  • Another suggests that placing ##q_0## on a non-conducting spherical shell could keep it fixed as ##q_1## approaches.
  • A participant clarifies that the moment when ##q_1## is at rest occurs only briefly before it is repelled back, assuming an impact parameter of zero.
  • Another scenario is introduced where ##q_1## is fixed and a charge ##q_2## is thrown towards it, raising questions about the conditions for the distance of closest approach and the angle of velocity vectors at that point.
  • Participants discuss the conditions under which ##q_1## stops moving, with references to conservation of energy and the balance of forces.
  • There is a discussion about the significance of the impact parameter, with questions about how it affects the trajectory and the conditions for the closest approach.
  • Clarifications are made regarding the mathematical representation of motion, including the relationship between position vectors and their rates of change.
  • One participant expresses confusion about the line of action of forces in relation to the fixed charge, seeking clarification on the geometric interpretation of force lines.

Areas of Agreement / Disagreement

Participants express various viewpoints on how to conceptualize the fixed charge and the dynamics of the moving charge. There is no consensus on the best way to hold ##q_0## fixed or the implications of different impact parameters on the motion of the charges. The discussion remains unresolved with multiple competing views.

Contextual Notes

Participants reference concepts such as conservation of energy, the nature of electrostatic forces, and the geometric interpretation of force lines, but the discussion does not resolve the underlying assumptions or definitions that may affect these interpretations.

  • #31
OK, and how do you calculate torque? What is the definition?
 
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  • #32
nasu said:
OK, and how do you calculate torque? What is the definition?
Torque is the tendency of a force to rotate an object about an axis.

34be615483d01fea0d42822a7010abc7.png
 
  • #33
My question is
gracy said:
electric force won't apply any torque with respect to the charge q_1 in the whole system
Is it the same thing as electric force won't apply any torque on the charge q_1 in the whole system.
 
  • #34
gracy said:
Is it the same thing as electric force won't apply any torque on the charge q_1 in the whole system.
Angular momentum is only given by moment of inertia multiplied by angular rotation rate if we are talking about a rigid object that is rotating. We are not talking about a rotating rigid object in this case. So we have to use the more general definition for angular momentum.

The more general definition for angular momentum requires a reference point. The angular momentum of a system is the sum over all the particles in the system of the vector cross product of the momentum of the particle times its displacement from the reference point.

Taking angular momentum "with respect to" a point means using that point as the reference.

Edit: The electric force applies no net torque to the entire system because any torque applied by ##q_1## on ##q_2## will be equal and opposite to the torque applied by ##q_2## on ##q_1##. This follows because of the way the vector cross product works -- two identical forces applied along the same line of action will result in identical torques.
 
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  • #35
The whole paragraph is as follows

We consider a charge ##q_1## which is again fixed, and always kept at rest and from this charge particle .of closest approach. here, we consider a charge ##q_1## which is again fixed, and always kept at rest and from this charge particle ##q_1## at an impact parameter d another charge which is having a mass m and charge ##q_2## is thrown. with the speed ##v_0##. We know that ##q_2## as the charge gets closer to this ##q_1##. due to repulsion its path will be deviated .We wish to find out the distanceof closest approach of the 2 particles. that will be at a position when the velocity vector of. the charge ##q_2## will be at right angle to the line joining ##q_1##and ##q_2## that will be the distance of closest approach we can write as ##r_0##. and in this situation we know as this ##q_1## is always fixed and the line of action of force will always pass through .##q_1## we can use angular momentum conservation as.the electric force won't apply any torque with respect to the charge i##q_1## in the whole system.


is ##q_1## a reference point ?or location of ##q_1## is reference point ?Can we use any point as a reference point?That is in this case can I take ##q_2## as a reference point.I think No because ##q_2## is moving it's location keeps on changing.
 
  • #36
gracy said:
The whole paragraph is as follows

We consider a charge ##q_1## which is again fixed, and always kept at rest and from this charge particle .of closest approach. here, we consider a charge ##q_1## which is again fixed, and always kept at rest and from this charge particle ##q_1## at an impact parameter d another charge which is having a mass m and charge ##q_2## is thrown. with the speed ##v_0##. We know that ##q_2## as the charge gets closer to this ##q_1##. due to repulsion its path will be deviated .We wish to find out the distanceof closest approach of the 2 particles. that will be at a position when the velocity vector of. the charge ##q_2## will be at right angle to the line joining ##q_1##and ##q_2## that will be the distance of closest approach we can write as ##r_0##. and in this situation we know as this ##q_1## is always fixed and the line of action of force will always pass through .##q_1## we can use angular momentum conservation as.the electric force won't apply any torque with respect to the charge i##q_1## in the whole system.


is ##q_1## a reference point ?or location of ##q_1## is reference point ?Can we use any point as a reference point?That is in this case can I take ##q_2## as a reference point.I think No because ##q_2## is moving it's location keeps on changing.
The location of ##q_1## is a good choice for a reference point. The fact that it is not moving (in your chosen coordinates) is one reason. Another good reason is because whatever external force holds ##q_1## in place exerts no torque if we choose the location of ##q_1## as the reference point.
 
  • #37
gracy said:
Torque is the tendency of a force to rotate an object about an axis.

34be615483d01fea0d42822a7010abc7.png
So what doe this tells you about the torque when r and F are along the same direction?
 
  • #38
nasu said:
So what doe this tells you about the torque when r and F are along the same direction?
Torque=rFsin theta
theta will be zero hence torque will also be zero.
 
  • #39
I did not understand properly what purpose does reference point serve in torque?
 
  • #40
gracy said:
I did not understand properly what purpose does reference point serve in torque?
If you do not have a reference point, how can you compute the r in
gracy said:
p?image=https%3A%2F%2Fupload.wikimedia.org%2Fmath%2F3%2F4%2Fb%2F34be615483d01fea0d42822a7010abc7.png
 
  • #41
How do you define that r if you don't have a reference point? Any position vector is relative to some origin.
The torque will depend on what point do you choose for origin. It may be zero for one particular origin and non-zero for another origin.
 
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  • #42
gracy said:
The whole paragraph is as follows

"We consider a charge q1 which is again fixed, and always kept at rest and from this charge particle .of closest approach. here, we consider a charge ##q_1## which is again fixed, and always kept at rest and from this charge particle ##q_1## at an impact parameter d another charge which is having a mass m and charge ##q_2## is thrown. with the speed ##v_0##. We know that ##q_2## as the charge gets closer to this ##q_1##, due to repulsion its path will be deviated .We wish to find out the distance of closest approach of the 2 particles. That will be at a position when the velocity vector of the charge ##q_2## will be at right angle to the line joining ##q_1##and ##q_2##. That will be the distance of closest approach we can write as ##r_0##. And in this situation we know as this ##q_1## is always fixed and the line of action of force will always pass through ##q_1##. We can use angular momentum conservation as the electric force won't apply any torque with respect to the charge i##q_1## in the whole system."

I believe that you have some 'cut and paste' error in the above. I have done a 'strike-through' through the repeated text and capitalized a few words I was confident started sentences as well as removing some random periods .

Is this essentially the question you began in your OP and then expanded in post #4?

Does this paragraph come from some particular source ?
 
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  • #43
jbriggs444 said:
. This follows because of the way the vector cross product works -- two identical forces applied along the same line of action will result in identical torques.
lineof.png


I thought the two lines of action of repulsive forces are different(opposite direction).​
 
  • #44
gracy said:
I thought the two lines of action of repulsive forces are different(opposite direction).​
Yes, if two forces are identical (same direction) and on the same line of action, they yield identical torques. If two forces are equal but opposite (opposite directions) and are on the same line of action, they yield equal but opposite torques.
 
  • #45
What is line of action of force in below picture

torc.gif


Is it r?
 
  • #46
What is line of action of force in below picture
torque.gif
 
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  • #47
The "line of action" of a force is a line that goes through the point of application. It extends forward in the direction of the applied force and backward in the opposite direction. For a force applied at a distance, the line of action will go through both the source of the force and its point of application. The two forces in a 3rd law force pair will always share the same line of action.

In the drawing you show, the line of action of force F is hiding under the vector F. The artist specifically placed F where he did in order to make its point of application (and, thus, its line of action) obvious.

If you had Googled the term, you could have learned this easily. https://en.wikipedia.org/wiki/Line_of_action


 
  • #48
Is vertex of angle θ reference point in the following
torque.gif
 
  • #49
jbriggs444 said:
If you had Googled the term, you could have learned this easily. https://en.wikipedia.org/wiki/Line_of_action

That is true. She could have. But she didn't. And it turned out she didn't need to. :biggrin:

I wrote this a month ago. It's still true.

Vanadium 50 said:
Gracy, I don't think PhysicsForums is helping you. You've asked us about vectors in the past, and now it's clear you haven't learned them.

The problem is that you immediately jump to asking a question here without having put much work into it, and when you are guided by someone towards the answer, you don't try and work it out for yourself, but instead ask for another hint. And another. And another. Eventually, you have been hinted all the way to the answer. Well, you've gotten the answer, but you haven't really learned.

You're going to have to decide if you want to learn or not. If you want to learn, you are going to have to spend more time thinking and working on your own. In this case, your starting point for basic vectors shouldn't be asking for more hints - it should be going back to your past materials and see if you can solve this using what you have already been told.

You can see it here -she's on E&M but is struggling with mechanics. Why is she struggling with mechanics? Because she didn't do the work when she was taking it - she got us to do it for her. Is she learning E&M? Nope - same reason. And it's our fault.
 
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  • #50
gracy said:
Is vertex of angle θ reference point in the following
Yes.

It is common practice in high school physics is to talk about angular momentum in two dimensions only and to use the notion of an "axis of rotation" rather than a point of reference.
 
  • #51
Come on I was just getting it confirmed from you experts!
 
  • #52
gracy said:
Come on I was just getting it confirmed from you experts!
Re-read your post 46. It seems more plausible that you are just guessing.
 
  • #53
gracy said:
Come on I was just getting it confirmed from you experts!
It was for reference point.I was correct there.For Line of action of force I did go through wikipedia but did not understand.
 
  • #54
p?image=https%3A%2F%2Fupload.wikimedia.org%2Fmath%2F3%2F4%2Fb%2F34be615483d01fea0d42822a7010abc7.png


=rFsin theta

We will take location of q1 as a reference point.Reasons for this have been discussed in post #36In case of repulsive force applied by q1 on q2 F and r in same direction therefore theta is zero hence no torque is produced.

In case of repulsive force applied by q2 on q1 r i.e position vector will be zero because we have chosen q1 as a reference .Therefore no torque is produced .

And no other force is present to produce torque.Torque is absent that's why angular momentum will be conserved.Right?
 
  • #55
Google "central force".
 
  • #56
@gracy ,
Let's see ...

You made an inquiry regarding using conservation of angular momentum in analyzing the scenario here.

It makes sense to consider the angular momentum of the moving particle with respect to the fixed particle.

To see that this angular momentum is conserved, consider the torque (with respect to the same fixed point) on the moving particle.

The only force on the the moving particle being considered here, is the Coulomb force which the fixed particle (charge, q1) exerts upon the moving particle (charge, q2)).

This force, ##\ \vec{F}\,,\ ## is along the line determined by the two particles. The position vector, ##\ \vec{r}\,,\ ## from the fixed particle to the moving particle is along this same line.

What does that imply about ##\ \vec{r}\times\vec{F} \ ?\ ##
 
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  • #57
SammyS said:
What does that imply about r⃗ ×F⃗ ?
Theta is zero hence torque is also zero.
 
  • #58
When line of action of force pass through a point there is no torque (moment of force)produced about that point and that's the reason there is no torque about q1 and q2 .Even if we do not make q1 reference point or even if we will not consider q1 being static we can still conclude that there is no torque when there is system of two charges and only force present is of action -reaction type( as long as the action-reaction forces act along the line connecting the charges. That is, as long as the action-reaction forces are attractive or repulsive. And that's true for electric (Coulomb) forces.)

I hope it is correct.
 
  • #59
It is.
Also true for graviational force (the attractive part :smile:)

Comparable: with a wire you can't pull sideways, only towards you.
 
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  • #60
You're making some very general statements based on a fairly specific situation. Much care is needed with these statements.

gracy said:
When line of action of force pass through a point there is no torque (moment of force)produced about that point and that's the reason there is no torque about q1 and q2 .

(Aren't subscripts so much better to read?)
To be specific: That's the reason that the stationary charge, q1, exerts no torque (zero torque) on the moving charge, q2, when that torque is about the location of q1, the stationary charge.* This is important if you want to use angular momentum conservation to aid in analyzing the trajectory of charge q2. In this case, the angular momentum of q2, with respect to the location of charge q1, is constant.

By the way, using ##\ I\omega \ ## is not a very helpful way to calculate angular momentum for a single particle unless it has a fixed distance from some point, such as the case of circular motion. The more general way to get the angular momentum about a point (taken here as the origin) is ##\ \vec{L} = \vec{r} \times \vec{p}\ ##.
*To be sure, the torque exerted by q1 on q2 is not necessarily zero when it is calculated about some other point.
Note: I hesitated even mentioning this lest the discussion go ambling down some stray path. We're already up to the 60's in the number of posts in this thread.​
 

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