Direction of Work: Electron-Electron Repulsion

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Discussion Overview

The discussion revolves around the concept of work in the context of electron-electron interactions, specifically addressing the direction of work done during repulsion. Participants explore the relationship between force, energy transfer, and the implications of scalar versus vector quantities in this scenario.

Discussion Character

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

Main Points Raised

  • Some participants suggest that the direction of work corresponds to the vector between two electrons, while others emphasize that work is a scalar quantity and does not have a direction.
  • One participant notes that during interactions, one electron gains energy while the other loses an equal amount, implying a transfer of energy without a directional component.
  • There is a discussion about the nature of forces in electron interactions, with references to Coulomb's law and Lienard-Wiechert potentials, indicating that forces are generally repulsive but may not always point directly away from each other due to relativistic effects.
  • Some participants question how to define the direction of force when considering moving charges and the concept of radial force in this context.
  • There is a contention regarding whether work can be considered a vector in non-conservative forces, with some arguing that it remains a scalar.
  • Participants express uncertainty about how to reconcile the direction of work with the path taken by a test particle influenced by a source particle.

Areas of Agreement / Disagreement

Participants do not reach a consensus on the direction of work or the implications of scalar versus vector quantities in this context. Multiple competing views remain, particularly regarding the nature of forces and the definition of work in electron interactions.

Contextual Notes

Limitations include unresolved assumptions about the nature of interactions, the definitions of work and force, and the implications of relativistic effects on electron interactions.

nouveau_riche
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how can we account for the direction in which the work is being done by a particle while it is interacting?
say as an example,electron -electron repulsion,we know that there is a repulsive force but in which direction is the electron working(in direction of motion of force/any other)?
justify your answer
 
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I would expect

The direction along the vector between the two electrons.

The force is in all directions but the force acting on another electron is along this vector. The sign depends on if your taking the electron to work on the other electron or itself.
 
Hi, when work is done, there must be some kind of enregy transfer or transformation eg from kinetic to kintec or potential to kinetic etc.
For two electrons interracting, say colliding, then one electron will gain an amount of energy due to the interraction and the other will loose an equal amount.
Because work deals with energy which is a scalar, then there is no direction associated with this. One electron does work on the other and vis versa. It just depends on the question.
 
LostConjugate said:
I would expect

The direction along the vector between the two electrons.

The force is in all directions but the force acting on another electron is along this vector. The sign depends on if your taking the electron to work on the other electron or itself.

which direction are you talking about,there will be many in between?

magpie5 said:
Hi, when work is done, there must be some kind of enregy transfer or transformation eg from kinetic to kintec or potential to kinetic etc.
For two electrons interracting, say colliding, then one electron will gain an amount of energy due to the interraction and the other will loose an equal amount.
Because work deals with energy which is a scalar, then there is no direction associated with this. One electron does work on the other and vis versa. It just depends on the question.

but you missed the nature of interaction ,repulsion/attraction
with collision an energy is gained/lost but the collision can occur from various direction,say head on or at 90 degree
what i mean to say is even if it is a head on,can u say it will always be repulsion?
 
Work does not have a direction. It is a scalar, not a vector.
 
DaleSpam said:
Work does not have a direction. It is a scalar, not a vector.

okay,let us talk about force in the same context,i mean electron electron interaction?
 
The force will be along a line joining the electrons. The work will correspond to the integral of that force times distance (∫fdx)along that line.
 
nouveau_riche said:
okay,let us talk about force in the same context,i mean electron electron interaction?
The force between two stationary electrons is given by Coulomb's law and is always repulsive. The force between two moving electons is given by the Lienard Wiechert potentials and will also always be approximately repulsive, but due to the finite speed of light it may not always be pointing exactly directly away from the current position of the other electron.
 
Yes, that must be right but will not each electron still 'see' a force which is radial? You would need to do a slightly modified line integral, possibly, but each electron would be accelerated along the line that it 'sees' the other one.
 
  • #10
sophiecentaur said:
Yes, that must be right but will not each electron still 'see' a force which is radial?
How would you would define a "radial force" in the case of an arbitrarily moving charge?
 
  • #11
It would be the same direction that the electron would look in order to see the other. That wouldn't be difficult to calculate, given the inclination, using a bit of SR. (Would it?)
 
  • #12
sophiecentaur said:
but each electron would be accelerated along the line that it 'sees' the other one.
Electrons are bad example for seeing each other. Take two negatively charged space ships at high relative speed.
 
  • #13
sophiecentaur said:
It would be the same direction that the electron would look in order to see the other. That wouldn't be difficult to calculate, given the inclination, using a bit of SR. (Would it?)
I would have to work out the math to be sure, but I don't think that the force necessarily comes from that direction. For example, I think that the force from a charge moving at constant velocity comes from its actual position, but due to abberation you would look at a different position to see it. I am not certain about this, however, so don't rely too strongly on it.
 
  • #14
DaleSpam said:
I would have to work out the math to be sure, but I don't think that the force necessarily comes from that direction. For example, I think that the force from a charge moving at constant velocity comes from its actual position, but due to abberation you would look at a different position to see it.
This is correct. For inertial movement the field itself in the rest frame of the charge is static and radial, so the force is towards/from the charge. But light is a disturbance of the field that travels c. So the moving charge sees aberration.

In the rest frame of the "watching" charge the directions are different too, because the light comes from an old position of the light emitting charge. The field is Lorentz contracted, but moves with the charge and the force still points directly to the moving charge.
 
  • #15
sophiecentaur said:
The force will be along a line joining the electrons. The work will correspond to the integral of that force times distance (∫fdx)along that line.

how can you say that the force will be along the line joining the electrons?,i guess the direction of motion of electron is not the answer
DaleSpam said:
The force between two stationary electrons is given by Coulomb's law and is always repulsive. The force between two moving electons is given by the Lienard Wiechert potentials and will also always be approximately repulsive, but due to the finite speed of light it may not always be pointing exactly directly away from the current position of the other electron.

how can you say that the force will be along the line joining the electrons?,i guess the direction of motion of electron is not the answer
 
  • #16
nouveau_riche said:
how can you say that the force will be along the line joining the electrons?
I didn't say that. I said the force would be given by the Lienard Wiechert potential.
 
  • #17
DaleSpam said:
I didn't say that. I said the force would be given by the Lienard Wiechert potential.

can u explain that a bit?,and work will be a vector if the force is non conservative
 
  • #18
I can't see how a scalar can suddenly become a vector.??
 
  • #19
nouveau_riche said:
DaleSpam said:
I didn't say that. I said the force would be given by the Lienard Wiechert potential.
can u explain that a bit?
Here is a good place to start: http://tinyurl.com/3aovkjz

nouveau_riche said:
and work will be a vector if the force is non conservative
No.
 
  • #20
I don't quite understand your question. What do you meant by direction of work? You can consider displacement as its direction, or you can consider the direction of the force as its direction. I think there is no difference between two vectors of the dot product or dot product integrated.
 
  • #21
ZealScience said:
I don't quite understand your question. What do you meant by direction of work? You can consider displacement as its direction, or you can consider the direction of the force as its direction. I think there is no difference between two vectors of the dot product or dot product integrated.

well direction of work mean the path that will be followed by the test particle under the influence of source particle

DaleSpam said:
Here is a good place to start: http://tinyurl.com/3aovkjz

No.

i can prove this -- if a force is non conservative a line integral between two points will be different for different paths,so i will have to specify the directions along which a test particle moves under the influence of source

sophiecentaur said:
I can't see how a scalar can suddenly become a vector.??

i can prove this -- if a force is non conservative a line integral between two points will be different for different paths,so i will have to specify the directions along which a test particle moves under the influence of source
 
  • #22
nouveau_riche said:
i can prove this -- if a force is non conservative a line integral between two points will be different for different paths,so i will have to specify the directions along which a test particle moves under the influence of source
Just because work done is path dependent in some cases does not make it a vector.
 
  • #23
Work is the integral of F dot dr. That's the definition, plain and simple. What the dot product means is that the answer is the scalar magnitude of the force vector F projected along the length vector r. Because of this definition, the work done becomes a vector with one dimension of direction, + or -. So we make the important distinction that Energy is a scalar while Work is a vector. I just finished my AP Physics class not 3 months ago, so this is pretty fresh in memory. Work can either add or subtract from KE, PE, etc. In the case of a repulsive force, negative work is done, decreasing the KE and increasing PE. I believe what you're thinking of is the direction in which KE(Kinetic Energy) or the like is changing. If the electron is "climbing" a potential spike, then work done subtracts from KE, and if the electron is "falling" into a well, then the opposite is true. The justification is the definition of work and the nature of the force.

Also related is momentum, which is a vector quantity, and may be more what you're looking for. Momentum is the product of the scalar mass and vector velocity, which yields a second vector representing momentum. Force acting over time changes momentum.
 
  • #24
http://physics.info/vector-multiplication/"

Curiously, they list the dot product as producing a scalar. I guess what I'm getting from that is that there is some confusion/disagreement as to what constitutes a vector or a scalar. When I refer to a vector, it is any number with an attached direction, regardless of how many components that direction has. A scalar is any number that is independent of direction; a magnitude alone, without and direction, even + or -. Thus as I was taught, Work == Vector, Energy == Scalar. That might not be true if you choose to define vector/scalar quantities differently. If someone could clarify that inconsistency, I'd be much obliged.
 
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  • #25
FireStorm000 said:
Work is the integral of F dot dr. That's the definition, plain and simple. What the dot product means is that the answer is the scalar magnitude of the force vector F projected along the length vector r. Because of this definition, the work done becomes a vector with one dimension of direction, + or -. So we make the important distinction that Energy is a scalar while Work is a vector.
:bugeye: Yikes!

Note that another name for the 'dot' product is the scalar product of two vectors. Quoting from hyperphysics: "The scalar product of two vectors can be constructed by taking the component of one vector in the direction of the other and multiplying it times the magnitude of the other vector." (See: http://hyperphysics.phy-astr.gsu.edu/hbase/vsca.html" )
 
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  • #26
Yikes! ...
Yeah, read the post after that. What I was taught is not being consistent with what the INTERNET is saying. Could you clarify?
 
  • #27
FireStorm000 said:
Curiously, they list the dot product as producing a scalar.
Of course they do! As will any legit reference.

I guess what I'm getting from that is that there is some confusion/disagreement as to what constitutes a vector or a scalar.
Not really.

When I refer to a vector, it is any number with an attached direction, regardless of how many components that direction has. A scalar is any number that is independent of direction; a magnitude alone, without and direction, even + or -. Thus as I was taught, Work == Vector, Energy == Scalar. That might not be true if you choose to define vector/scalar quantities differently. If someone could clarify that inconsistency, I'd be much obliged.
A scalar can have a sign, just not a direction.

Do you have a published reference that states Work = vector? I'd love to see it!
 
  • #28
FireStorm000 said:
Yeah, read the post after that. What I was taught is not being consistent with what the INTERNET is saying. Could you clarify?
It's not just 'the internet' saying that. What reference do you have?
 
  • #29
FireStorm000 said:
Curiously, they list the dot product as producing a scalar. I guess what I'm getting from that is that there is some confusion/disagreement as to what constitutes a vector or a scalar.

Not at all. An inner product space over \mathbb{R} has a map <.,.>: V\times V \mapsto \mathbb{R}. The inner product over this field will always map vectors to the reals so there is no way work is a vector. You can't define it that way, it makes no sense to.
 
  • #30
A scalar can have a sign, just not a direction.
You actually clarified everything right there. Under that definition, work is a scalar with a domain from + to - infinity. Energy has a domain of 0 - +infinity. The definition of a scalar I was using in my AP physics class was that a scalar had domain 0 to +infinity, and everything else was a vector, because everything else would constitute a direction. Under this definition, which would appear to be the prevailing one, then work is a scalar. It just has a +/- sign where energy does not.

I went through the http://asd20.org/education/components/docmgr/default.php?sectiondetailid=37896&fileitem=43607&catfilter=5055" again, and the instructor specifically states that the answer is a scalar because the dot product can be simplified as [scalar * scalar * cos direction = scalar].

Generally speaking, I think my logic for coming to the conclusion I did is straightforward though: "A vector is any quantity that has direction"; few people would disagree with that statement, though apparently it isn't quite right. "magnitude is the same as the absolute value." In other words, the magnitude does not include a +/-. We use the same symbolism for the two operations. --> "Anything where |V| != V is a vector" --> "|cos pi| != cos pi." --> "Work is not a scalar, it must be a vector".

If all of those statements hold, then the logic is sound, so somewhere in there a distinction must be made that makes a quantity with 1 dimension of direction a scalar. In the end, I guess it makes sense though. You can't really consider a number line as having a direction, as there are only two choices of angle, 0 and pi. A plane has one choice of direction, that is, an angle that can take on any (real) value. A 3D coordinate system has 2 free directions along which we must define an angle. Thus a better way to define a scalar is by the number of free axises of direction it has. A vector is any value more than 0, a scalar has 0.

Curiously, we end up then with two classes of scalars, those that must be 0 or above, and those that can take on any real value. Temperature, Energy, Counts, Speed and some others fall into this first category. Things like Work, Rates of changes of the first class, and some others fall into this second class. So I guess my misconception was to group this second class in with vectors when it's really just another type of scalar.
 
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