Electromagnetism, vector calculus.

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Discussion Overview

The discussion revolves around the calculation of electric fields and charge density from electrostatic potential energy in the context of electromagnetism and vector calculus. Participants explore the differentiation of constants and the implications for electric field and charge density calculations.

Discussion Character

  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • One participant questions whether the constant n should be differentiated when calculating the electric field from the electrostatic potential energy, expressing concern about maintaining correct units.
  • Another participant emphasizes that constants are not differentiated and clarifies the distinction between electric potential and potential energy.
  • A later reply corrects the terminology, stating that v(r) represents electrostatic potential, not potential energy, and confirms that n is indeed a constant with dimensions m^-3.
  • One participant expresses doubt about the implications of their calculations for electric charge density, noting that their result appears to indicate a uniform charge density without spatial dependence.
  • Another participant reassures that the calculated charge density being constant is valid within the specified region and suggests a visualization involving an infinitely long cylinder to support this interpretation.

Areas of Agreement / Disagreement

Participants generally agree on the treatment of constants in differentiation and the distinction between potential and potential energy. However, there is uncertainty regarding the implications of the calculated charge density and its spatial dependence.

Contextual Notes

Limitations include the assumption that the region of interest is uniform and the potential dependence on spatial coordinates, which may not be fully resolved in the calculations presented.

Spoony
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Hey i was wondering about a paticular problem i found in a textbook. Specifically just one little niggle i have with it.

i am given that the electrostatic potential energy in a region of space is given by
v(r) = ((q*n)/(epsilon-0))(x^2+y^2)
(where n is a constant of dimensions m^-3)

It then goes on to say calculate the electric field, so E= -grad(V)

since v is a scalar field then grad(v) is simply
-gradv = E = -( d/dx (v)i + d/dy (v)j + d/dy (v)k )
and in this case the d/dx is a partial derivative.

So i have to partial differeniate V with respect to all co-ords and then stick a vector on each direction respective of what its been differentiated by.
But i have a problem, the n is a constant so it's constant througout the region of space, but does it get differentiated?
common sense says no as to keep the dimensions required for an electric field E it'd need to have 1/distance^2 as the actual final units of distance (after cancelling the quotants)
and not differenctiating the n would make this so.

BUT I am unsure as i rarely trust common sense with physics anymore :P especially since starting quantum physics this year :(.

Thanks guys
 
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The key phrase to consider is n is a constant...do you ever differentiate a constant?!

Also, you want to make sure you differentiate the electric potential (aka voltage), not the potential energy...the two quantities are related, but distinct.

If v(r) really represents the potential energy, then the units of n must be meters, not meters cubed.

In addition, even if n was a function ox x and y, when you use the product rule to differentiate V, you should still get the correct units-- when you consider the term involving the derivative of n, the rest of the stuff multiplying n is not differentiated in the same term, so the units still work out fine.
 
v(r) represents the electrostatic potential (sorry shoudlve been more precise and actually accurate), also the units of n are actually m^-3, typo above which is corrected.
I was almost sure that i would not have to differentiate the n at all as it was constant and remains the same throughout the electrostatic potential, scalar field, therefore logically itd stay the same throughout the electric, vector field.
But i just doubted myself because i wanted to be 100% sure about this trival thing.
 
No worries, it's always a good idea to ask when you're not 100% sure about something. :smile:
 
Thanks for the help mate :)
one more thing though, it then asks to calculate the electric charge density which is simply div(E) = p / (epsilon-0)

where p is the charge density.

All well and good its simply:

d/dx (Ex) + d/dy(Ey) + d/dz(Ez) = p / (epsilon-0)

But it asks for the electric charge density in terms of (x,y,z) when i do the above computation i arrive with a solution that contains no x,y,z terms so this would mean that the electric charge density at any point in space is the same. Which would make not much sense.

i tried to visulise it as a wire going up the z axis that is infinatley long with an electric field induced towards the centre.

This is what i get from calculating the charge density p

p= -4nq

But no x,y,z terms.

Am i doing things right and the awnser is that the charge density at ANY given point is -4nq or have i missed something?
 
Your answer looks fine to me ...remember, v(r) is only ((q*n)/(epsilon-0))(x^2+y^2) in a certain region, so the charge density is only constant in that region.

An infinitely long cylinder along the z-axis of constant charge density -4nq should give you the same v(r) anywhere inside the cylinder, so I would say that is a good way to visualize the problem.
 

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