Non-Electrostatic Problem: Closest Distance of Approach

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Discussion Overview

The discussion revolves around a problem involving two moving charges and their closest distance of approach, exploring the implications of moving electric fields and the application of energy conservation in such scenarios. Participants examine the relationship between electric and gravitational fields, particularly in dynamic contexts.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • One participant presents a problem involving two charges and questions how to define potential in a non-static electric field when using energy conservation.
  • Another participant suggests that conservation of energy applies in the context of a harmonic oscillator, despite the non-constant force, but acknowledges that the scenario with two moving masses is more complex.
  • A participant expresses dissatisfaction with the harmonic oscillator analogy, arguing that it lacks a field concept.
  • Another participant argues that as long as the charges move slowly, the situation can be treated as quasistatic, allowing the use of electrostatic principles.
  • Concerns are raised about applying Newton's law of gravity to moving masses, with a note that it fails to account for certain phenomena, while still being applicable under specific conditions.
  • Discussion includes a mention of general relativity and its similarities to electrodynamic fields, suggesting a deeper connection between gravitational and electric interactions.

Areas of Agreement / Disagreement

Participants express differing views on the applicability of energy conservation in dynamic fields, with some supporting the use of quasistatic approximations while others challenge the analogies drawn. The discussion remains unresolved regarding the best approach to the problem and the implications of moving fields.

Contextual Notes

Participants highlight the limitations of applying static field concepts to dynamic situations, noting the need for careful consideration of conditions such as speed and mass density when using classical laws.

atavistic
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I encountered a problem which goes like this:

Two charges of mass m and charge q are initially positioned far from each other. Now one is projected towards the other with velocity v . Find the closest distance of approach.

We( in class) solved the problem using energy conservation but I had this doubt later:

Since the charges are moving, the electric field is not static in nature , so how can we define potential of such a field and use it in energy equation? And then I had this another doubt which we encounter more often in gravitation where two masses come towards each other by their mutual attraction, since gravitation is also similar to coulomb's law can we say we cannot gravitational field for a moving body?
 
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atavistic said:
I encountered a problem which goes like this:

Two charges of mass m and charge q are initially positioned far from each other. Now one is projected towards the other with velocity v . Find the closest distance of approach.

We( in class) solved the problem using energy conservation but I had this doubt later:

Since the charges are moving, the electric field is not static in nature , so how can we define potential of such a field and use it in energy equation? And then I had this another doubt which we encounter more often in gravitation where two masses come towards each other by their mutual attraction, since gravitation is also similar to coulomb's law can we say we cannot gravitational field for a moving body?

Conservation of energy certain works in your first scenario. Think of the harmonic oscillator. The "force" isn't a constant either throughout the motion of the oscillator (eg. mass on a spring). Yet, conservation of energy certainly works there.

The second problem (both masses moving) requires a bit more thought. This is the same problem as the method of images where one has a charge moving towards an infinite conducting plane. There is a difference between this, and moving a charge while keeping the other one fixed. I actually wrote this for a "vexer" contest a while back, so you may want to read this first.

Zz.
 

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I don't think I am satisfied with the harmonic oscillator analogy because there , there is nothing called field .

Awaiting more replies.
 
atavistic said:
I don't think I am satisfied with the harmonic oscillator analogy because there , there is nothing called field .

Awaiting more replies.

Er.. the harmonic oscillator potential is used in solid state physics plenty of times. These are the potential field that, to an good approximation, is what holding the crystal lattice in place. Look at the calculation involved in finding the specific heat of a solid.

Besides, what does this matter? A potential field is a potential field! Did you even look at the attached document?

Zz.
 
atavistic said:
Since the charges are moving, the electric field is not static in nature , so how can we define potential of such a field and use it in energy equation?

As long as the particle is moving sufficiently "slow" (ie not relativistic) the setup is called "quasistatic" and all the machinery of electrostatics works just fine for all practical purposes.

The situation can be treated exactly by use of retarded potential formulation (or relativistic electrodynamics) but that's hardcore stuff.
atavistic said:
And then I had this another doubt which we encounter more often in gravitation where two masses come towards each other by their mutual attraction, since gravitation is also similar to coulomb's law can we say we cannot gravitational field for a moving body?

Technically speaking no. That's why Newtons law of gravity fails to account for more exotic phenomena like black holes. But again, as long as the bodies involved moves sufficiently slow and the mass density is sufficiently low, Newtons law works just fine.

Gravity, in the formulation of general relativity on the other hand, is revealed to behave much like electrodynamic fields, introducing some other field that behaves very similar to a magnetic field
 

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