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.

gracy
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There is charge ##q_0## which is fixed.from a distance far away another charge ##q_1## is fired towards it with speed ##V_0## then we know as both of these are positive charges these will repel each other as the charge ##q_1## comes closer. While coming closer to ##q_0##, it's speed decreases and after reaching a closest distance ##r_0## it's speed becomes zero . Now this is the position when , both of these charges will be at rest and there won't be any kinetic energy in ##q_1## left at this position.
My first question is how charge ##q_0## must have been fixed such that it does not move due to repulsion?
 
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I'm not sure, but one way to do this would be putting the charge q0 on a spherical shell (non conducting) such that it uniformly distributes over it. This way, the charge q0 will be fixed on the shell as q1 approaches it.
 
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gracy said:
My first question is how charge q0q0q_0 must have been fixed such that it does not move due to repulsion?
The situation mentioned in your problem description is the instant moment when the charge ##q_1## is at rest during its course of motion. Of course as you may have predicted, after this infinitesimally short moment of stoppage, ##q_1## will be experiencing repulsion and will thence move back to where it came from (assuming the impact parameter is 0).
 
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Ok.We consider a charge ##q_1## which is again fixed, and always kept at rest. and from this charge particle at an impact parameter d another charge, which is having mass m and charge ##q_2## is thrown with the speed ##V_0##. We know that as the charge ##q_2## gets closer to. ##q_1## due to repulsion it's path will be deviated .We wish to find out the distance of closest approach of the 2 particles.I have read that
distance of closest approach 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##
I want to know why ?
 
blue_leaf77 said:
q1q1q_1 will be experiencing repulsion and will thence move back to where it came from (assuming the impact parameter is 0).
But you are talking about ##q_1## and I had asked about ##q_0## .
 
Ah my bad, I misunderstood your question. I thought you were questioning how charge ##q_1## can be fixed all the time after it reached the closest distance with ##q_2##. It turns out that your question is about the way to hold ##q_0## fixed. Well to answer this, just imagine ##q_0## is held by something, like hypothetical human's hand.
 
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I would also like to understand /know why ##q_1## stops?Does repulsive force balance the force with which ##q_1## was moving?
 
gracy said:
I would also like to understand /know why ##q_1## stops?Does repulsive force balance the force with which ##q_1## was moving?
##q_1## can stop during its motion only when the impact parameter is 0. You can understand this from the conservation of energy, ##T(x)+U(x) = C## where ##C## is constant. Charge ##q_1## started from infinity with certain initial velocity, also initially ##U(-\infty) = 0##. As ##q_1## approaches the fixed charge at the origin, ##U(x)## will be increasing, on the other hand ##T(x)## will decrease in order to keep the energy conservation satisfied. At some point ##T(x)## will equal 0, that's the moment when ##q_1## stops.
gracy said:
distance of closest approach will be at a position when the velocity vector of. the charge q2q2q_2 will be at right angle to the line joining q1q1q_1and q2q2q_2
I want to know why ?
Solving the equation of motion, you will see that elastic collision due to Coulomb repulsion yields a hyperbolic trajectory of the moving body. You should be able to see intuitively that the closest distance occurs when the velocity vector is perpendicular to the position vector of ##q_2##.
 
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The only difference between the situations I mentioned in OP and in my post #4 is impact parameter.In OP it is zero .Right?
 
  • #10
gracy said:
The only difference between the situations I mentioned in OP and in my post #4 is impact parameter.In OP it is zero .Right?
If in your OP the impact parameter is 0, then yes there will certain instant when ##q_1## is at rest.
 
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  • #11
gracy said:
distance of closest approach will be at a position when the velocity vector of. the charge q2q2q_2 will be at right angle to the line joining q1q1q_1and q2
Does this happen only when impact parameter has some non zero value?
 
  • #12
In post #8 by ##T(x)## did you mean kinetic energy ?
 
  • #13
gracy said:
Does this happen only when impact parameter has some non zero value?
In general, you can say that when the closest distance is reached, the vector relation
$$
\mathbf{r} \cdot \frac{d\mathbf{r}}{dt} = 0
$$
,with ##\mathbf{r}## the position vector, holds. When the impact parameter is different from zero, that equation is satisfied because the of the dot product between two perpendicular vectors. When the impact parameter is zero, that equation is satisfied because ##\frac{d\mathbf{r}}{dt} = 0##.
gracy said:
In post #8 by ##T(x)## did you mean kinetic energy ?
Yes.
 
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  • #14
blue_leaf77 said:
with r the position vector
position vector of charge body which is not moving ?
 
  • #15
blue_leaf77 said:
that equation is satisfied because the of the dot product between two perpendicular vectors.

Something seems missing in the above sentence.
 
  • #16
gracy said:
position vector of charge body which is not moving ?
In general ##\mathbf{r}## is the relative vector between the fixed charge and the moving charge. If the fixed one is held at the origin, this vector becomes the position vector of the moving charge.
gracy said:
Something seems missing in the above sentence.
It should be "that equation is satisfied because of the dot product between two perpendicular vectors."
 
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  • #17
blue_leaf77 said:
between two perpendicular vectors.
Which two perpendicular vectors?
 
  • #18
##\mathbf{r}## and ## \frac{d\mathbf{r}}{dt}##.
 
  • #19
You mean rate of change of position vector i.e ##\frac{dr}{dt}## is also a vector?
 
  • #20
Yes, it's also a vector. Because the change of a vector may involve the change of its direction and this change of direction must be accounted for in its rate of change.
 
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  • #21
blue_leaf77 said:
When the impact parameter is zero, that equation is satisfied because dr/dt = 0.
Did you mean when the impact parameter is zero,rate of change of position vector is also zero?But I think magnitude of rate of change of position vector will change.
 
  • #22
The rate of change of the position vector (which is the velocity, by the way) will be zero at the point of minimum distance only. This is, for impact parameter equal to zero.
For this case, the velocity is initially directed towards the fixed charge. Its magnitude decreases until it reaches zero at the minimum distance and then start increasing, but in the opposite direction. For this case the velocity is all radial, there is no component perpendicular to the line connecting the two charges.

For non-zero impact parameter, the radial component of the velocity have a similar behavior. But there is a normal component as well. This component does not vanish. The electrostatic force is always radial so there is no normal component of the force.
The dot product ## \vec{r} \cdot \frac{d \vec{r}}{dt} = \vec{r} \cdot \vec{v} ## is zero when the velocity has no radial component, so the mobile charge it is neither approaching nor moving away form the fixed charge. But it still have some normal component.

By "normal" in the above I mean perpendicular to the radial direction, with center in the fixed charge.
 
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  • #23
Thank you so much the above answer is really helpful.

##q_1## is always fixed and the line of action of force will always pass through ##q_1##.

I did not understand this.

I know the line of force is a geometric straight line in the direction of the direction of the force and through the point at which the force is being applied.

Here the force is force of repulsion and the line of action of this repulsive force will always pass through ##q_1## Right?
 
  • #24
gracy said:
I know the line of force is a geometric straight line in the direction of the direction of the force and through the point at which the force is being applied.
Right.
 
  • #25
gracy said:
Thank you so much the above answer is really helpful.

q1q1q_1 is always fixed and the line of action of force will always pass through q1q1q_1.
gracy said:
Here the force is force of repulsion and the line of action of this repulsive force will always pass through q1q1q_1 Right?
Please someone tell me am I right ?
 
  • #26
  • #27
nasu: q1q1q_1 is what you get when you quote ##q_1##.

gracy said:
Please someone tell me am I right ?
yes, the electrostatic force between two charges is collinear with the vector joining the charges.
 
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  • #28
And then

We can use angular momentum conservation as the electric force won't apply any torque with respect to the charge ##q_1## in the whole system

Please help me to understand this line.
 
  • #29
Do you know the definition of angular momentum and in what conditions will be conserved?
 
  • #30
nasu said:
Do you know the definition of angular momentum
It is the product of its moment of inertia and its angular velocity.
nasu said:
and in what conditions will be conserved
When there is no torque.
 

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