Voltage derivation for charged particles

In summary, the electric field on a particle is Coulombs law, and the voltage is the work done divided by the magnitude of the charge.
  • #1
Logical Dog
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I have a very weak understanding of the particle modelling of electrical phenomena.1:[tex]
Electric field =\frac{Force}{Magnitude of charge} [/tex]
1 is The definition of electric field on a particle (?)

2:[tex] Force = \frac{Q1*Q2*K}{R^2}\\[/tex]
2 is Coulombs law, to find force between two particles.

3:[tex] {\frac{(Q1*Q2*K)}{R^2}} / (Q2) = \frac{Q1*k}{R^2}[/tex]
3 is the substitution of 2 onto 1s numerator, Force

4:[tex] \frac{Q1*k}{R^2} * D = Work done[/tex]
4 is the formula for work done. D here meaning distance, or should one use S for displacement?

5:[tex] [\frac{Q1*k}{R^2} * D] /Q2 = Voltage [/tex]
5 is work done divided by magnitude of charge, which is voltage.

My question is, since, in 5, this:
[tex] [\frac{Q1*k}{R^2}] [/tex]

Is the electric field on a particle,
it fair to say, that the voltage is the electric field on a charge * distance moved as a result of fields force divided by the magnitude of that charge?
 
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  • #2
Bipolar Demon said:
4 is the formula for work done. D here meaning distance, or should one use S for displacement?
You can't use diplacement directly as S. You have to consider infinitesimal displacement ds because force is not constant. Work done in an electric field is given by integrating F⋅ds along a certain path. It is a line integral where F may be variable.

For what system are you using these equations? Two charges Q1 and Q2, out of which Q2 is fixed and Q1 is moved?
 
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  • #3
cnh1995 said:
For what system are you using these equations? Two charges Q1 and Q2, out of which Q2 is fixed and Q1 is moved?
Yes.
 
  • #4
cnh1995 said:
Two charges Q1 and Q2, out of which Q2 is fixed and Q1 is moved?
It doesn't matter; the Potential is the same if one, the other or both are moved in an inertial frame.
 
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  • #5
sophiecentaur said:
It doesn't matter; the Potential is the same if one, the other or both are moved in an inertial frame.

Os the derivation correct? :eek:
 
  • #6
Bipolar Demon said:
Os the derivation correct? :eek:
The Potential Energy at separation x is the work done to change the separation between the two from Infinity to x. The "derivation" is wrong as it fails to calculate the work done. It assumes that the field doesn't change as the separation changes.
It amazes me that people don't find this sort of information themselves, rather than trying to work it out from scratch. There are hundreds of sources for this information. Why not try this Hyperphysics Page? or this Wiki Link? Q and A is just not the way to learn Science. Getting from A to B by Brownian motion takes an awful long time.
 
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  • #7
In equation 4 you have multiple errors. You introduced D for distance, but R in the denominator is also the distance. The force and the field depend on the distance, so you need to integrate over R.
Also, you left off Q2 in the work done. Work is calculated from the force, which has both Q1 and Q2. The voltage is the work divided by Q2, so the Q2 will cancel out from the equation.
 
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  • #8
sophiecentaur said:
The Potential Energy at separation x is the work done to change the separation between the two from Infinity to x. The "derivation" is wrong as it fails to calculate the work done. It assumes that the field doesn't change as the separation changes.
It amazes me that people don't find this sort of information themselves, rather than trying to work it out from scratch. There are hundreds of sources for this information. Why not try this Hyperphysics Page? or this Wiki Link? Q and A is just not the way to learn Science. Getting from A to B by Brownian motion takes an awful long time.
thanks, I will re read everything. I thought I understood but it was clear I had no idea. I read books but sometimes I am always confused, no deriving things from scratch. I think I will take questions elsewhere :)
 
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  • #9
Bipolar Demon said:
I think I will take questions elsewhere :)
You can try but there's no guarantee that you will be asking the right questions in the right order to give you better understanding. I suggest that you come to terms with reading textbooks and get an appropriate path through this stuff. Perhaps the textbooks you have tried are too advanced for you at present? Good luck.
 
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  • #10
It might help your thinking to simplify your model
by changing from the complicated field that exists between two charges

http://www.pstcc.edu/nbs/WebPhysics/Chapters%2025%20and%2026.htm
upload_2017-2-14_21-8-38.png

to a simpler uniform electric field such as exists between two large parallel plates.
same link, http://www.pstcc.edu/nbs/WebPhysics/Chapters%2025%20and%2026.htm
upload_2017-2-14_21-7-43.png

Think "Millikan Oil Drop Experiment " for a minute ...
It should be intuitive that in the bottom diagram,
if the field is E volts per meter
a single electron will acquire or give up E electron volts for each meter in moves along a field line.
Electron volts to Joules is straightforward enough. Hmm, it looks mighty close to ~1/6.2E18 , a familiar enough number...

Approach: Make your math work for a simple model, then hone it for the more general case.

Any help ?

old jim
 
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  • #11
jim hardy said:
It might help your thinking to simplify your model
by changing from the complicated field that exists between two charges

http://www.pstcc.edu/nbs/WebPhysics/Chapters%2025%20and%2026.htm
View attachment 113224
to a simpler uniform electric field such as exists between two large parallel plates.
same link, http://www.pstcc.edu/nbs/WebPhysics/Chapters%2025%20and%2026.htm
View attachment 113223
Think "Millikan Oil Drop Experiment " for a minute ...
It should be intuitive that in the bottom diagram,
if the field is E volts per meter
a single electron will acquire or give up E electron volts for each meter in moves along a field line.
Electron volts to Joules is straightforward enough. Hmm, it looks mighty close to ~1/6.2E18 , a familiar enough number...

Approach: Make your math work for a simple model, then hone it for the more general case.

Any help ?

old jim
thanks sir, may I take some time and reply later? I am re reading the fundamentals and doing questions of schaums college physics..
 
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  • #12
Ok, I think I understood a lot.
So, I understood that I can't really derive voltage in the electric field between two point particles or one charge and one point particle, as the maths background and understanding needed is beyond my capabilities, furthermore the electric field isn't constant, hence the integral. I got the formula for potential and voltage though, but only for point particles and an electric charge distribution of a “sheet” (?).

I can derive the voltage in a constant electric field like the one between the capacitors (that is fairly easy and stems from the definition of the electric field between two parallel plate capacitors)...easy electric field there.

What I do not understand yet is the electric field inside a circuit, though I have looked for it and am reading some other stuff on it, I feel it can help me if I read more on it…even if it’s an approximation. I also get confused due to circuit analysis conventions like negative and positive voltages etc. Yes I really struggle with this stuff for some reason :-(. I see no alternative but to keep learning more electromagnetism on my own (to the minimum level of maxwells equations) . Unfortunately its not offered for my degree. Thanks for the help.

today I will read this thouroughly: http://science.uniserve.edu.au/school/curric/stage6/phys/stw2002/sefton.pdf
http://www.abc.net.au/science/articles/2014/02/05/3937083.htm
 
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  • #13
jim hardy said:
Approach: Make your math work for a simple model, then hone it for the more general case.
That would be the ideal approach but, if you are like me, you can work through the simple case and that can often allow you to 'believe' that it would work for a more difficult case.
Haha - do as I do - not necessarily as I say. It just depends on where you need to take this, of course.
Bipolar Demon said:
I also get confused due to circuit analysis conventions like negative and positive voltages etc.
That's only a problem if you insist on including ELECTRONS in the argument. They are totally unnecessary for nearly all circuit analysis. Charges (i.e. Positive Charges) flow 'downhill' from + to - unless they are 'pumped uphill' by a generator / emf / battery etc. That is actually NOT confusing, surely, any more than balls roll down a slope unless you actually carry them uphill.
 
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  • #14
sophiecentaur said:
That would be the ideal approach but, if you are like me, you can work through the simple case and that can often allow you to 'believe' that it would work for a more difficult case.

When i hit "real world" I soon learned that the textbook problems given in 'university' were carefully designed to be solvable.
When we go to work in industry we find out Mother Nature is seldom so accommodating,
and i appreciated why EE's in my school took Fluid Mechanics over in Civil Engineering department - for the graphical approach to working out pressure and flow profiles around irregular shapes.

Here's an example that relates to OP's plight... (Oh No , another Boring Anecdote !)

There exists around reactors a need for a gamma ray radiation detector that has electrically adjustable sensitivity.
Those WW2 geniuses figured out how to do it.

They create an electric field between two plates, but one of the plates has exaggerated "corrugations". Those two plates form the walls of a gamma ray detector that's filled with ionizable gas.
Voltage is impressed between the plates.Gamma rays ionize the gas and charges migrate to the respective plates.
Somebody had to calculate the field inside those corrugations but i had to settle for drawing the field as if it were a hydraulic flow problem.
In the narrow parts of the chamber E field is simple, constant Volts/meter just like between two parallel plates.
Within the deep corrugations however it's not so simple
CIC2.jpg

please pardon my artistic awkwardness
here's a better drawing from the patent but it's rotated 90 degrees
http://pdfpiw.uspto.gov/.piw?PageNum=0&docid=02852694&IDKey=AF8EA366EA31 &HomeUrl=http://patft.uspto.gov/netacgi/nph-Parser?Sect1=PTO1%26Sect2=HITOFF%26d=PALL%26p=1%26u=%252Fnetahtml%252FPTO%252Fsrchnum.htm%26r=1%26f=G%26l=50%26s1=2852694.PN.%26OS=PN/2852694%26RS=PN/2852694
CIC1.jpg


Equipotential lines, always perpendicular to Efield lines (just as in fluid flow problems) distort over(up in good drawing ) into the corrugations.
As field inside the corrugation weakens it becomes too feeble to collect ions and they recombine instead of moving toward a plate.
By adjusting the applied voltage one controls how far into the corrugation that happens, which effectively adjusts the volume(hence sensitivity) of the detector.
That's the heart of our reactor wide range power meter. It works over eight decades of power , from just above startup to 100%.

Here's a description of the detector and ts use
https://www.google.com/url?sa=t&rct=j&q=&esrc=s&source=web&cd=1&cad=rja&uact=8&ved=0ahUKEwjo-7L6lpzSAhWn34MKHfVFBIsQFggeMAA&url=http://www.dtic.mil/cgi-bin/GetTRDoc?AD=ADA316002&usg=AFQjCNGPRkbsianSivvtCVNSzh6JWqKgxw
cic3.jpg


Anyhow my point is,
we must simplify to the point we can grasp what's going on
then use whatever math ability the Lord saw fit to grant us to describe the phenomenon.
Some will use vector calculus with its dels grads and curls;
'Children of the Lesser Gods' like myself will resort to simpler means .

I want OP to have some intuitive "feel" for fields. My old fluid mechanics course has saved my butt more than once in that regard.
If he masters Vector Calculus, and he probably will, he's a better man than me .

old jim
 
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  • #15
@Jim. You may have scared the OP off this topic for life. :biggrin:
@BD. You won't come across anything like that until you have a lot more experience of this stuff. In any case, there are computers available these days for providing some pretty good solutions to such problems.
 
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  • #16
sophiecentaur said:
@Jim. You may have scared the OP off this topic for life. :biggrin:
@BD. You won't come across anything like that until you have a lot more experience of this stuff. In any case, there are computers available these days for providing some pretty good solutions to such problems.

Its not a problem, I think when I read from the experts I get very happy, especially when they talk about the limitations and challenges they faced...when I was studying economics I read the economics anti textbook and was very happy..in particular its good to know the limitations of models or formulas I guess.

thanks again for your time..I think I studied too much today and am tired. I know one day ill get closer to a better understanding, and not have to use water analogies.
 
  • #17
Bipolar Demon said:
and not have to use water analogies.
I liked the link in your post #12. The 'surface charges and poynting vector' approach is indeed the correct approach to teach circuits instead of the water analogies. But I am not sure if high school students can grasp those concepts since they are not introduced to the concept of field (at least not in my country).
I remember how confused I used to be about this whole circuits stuff in high school and the best explanation my teacher would come up with after I asked queries was either the water analogy or the traffic analogy.
Bipolar Demon said:
Yes I really struggle with this stuff for some reason :-(. I see no alternative but to keep learning more electromagnetism on my own (to the minimum level of maxwells equations) .
If you are interested in studying it in depth for a satisfactory (not complete!) understanding, I think you'd enjoy D.J.Griffiths' Introduction to Electrodyamics and 'Matter and Interactions' by Chabay and Sherwood. (Both are available in pdf format I guess)..
 
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  • #18
cnh1995 said:
The 'surface charges and poynting vector' approach is indeed the correct approach to teach circuits instead of the water analogies.
What level were you proposing to teach 'circuits' with Poynting vectors? It's strange to include that in the same sentence as 'Water Analogies'. One is for twelve year olds (if you really must) and the other is for University Undergraduates. (I would have thought).
You seem to be missing out the normal circuit equations and Kirchoff on the way.
 
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  • #19
The water analogy really brings me out in spots. The problem is that people do not actually make the right connections between the so called analogous components in the water analogy and it tends to push understanding further away (judging from the way that people come back with 'wrong' conclusions, when they use it). I feel very strongly that the desire to 'understand' circuits without having to go through the process of V=IR, the Potential Divider, Kirchoff etc etc. is just self indulgence. The only reasonable analogy for circuits is the MATHS model. Non mathematical EE is only half a job.
 
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  • #20
sophiecentaur said:
@Jim. You may have scared the OP off this topic for life. :biggrin:

I hope not !
Electronics is a lot of fun... i still remember my elation when it dawned on me how that compensated ion chamber works.
@Bipolar Demon Work your basics in your head until you've resolved the seeming conflicts. When a mental model leads intuitively to the formula by a couple different thought paths you've built another powerful mental tool. Keep them sharp , like fine chisels.
 
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  • #21
sophiecentaur said:
What level were you proposing to teach 'circuits' with Poynting vectors?
Certainly not to 12 year olds.

But in junior college (grades 11 and 12 in India), we are taught about electric field, magnetic field, calculus and vectors. But when it comes to circuit theory, they start using KCL and KVL. That is the correct way of analyzing circuits as far as circuit theory is concerned . They don't even teach some basics of Poynting theorem or surface charges. Then our teachers made a couple of common mistakes. This is what my physics teacher used to say:
1) The energy is carried by the electrons in the wire and he'd compare wires with shafts in a mechanical transmission system (or pipes in water analogy).
2) The heat generated in the resistors due to current is because of the KE of the electrons.

As far as circuit theory is concerned, these two mistakes don't affect anything, but the physics taught was wrong. I am in my final year of electrical engineering degree and many of my classmates (and some professors) still make these mistakes. I was surprised to know that many of my classmates have never heard of Poynting vector and many of them still think that KE of electrons is what heats up the conductor.

I understand that I haven't used Poynting vector specifically in any engineering subject to design or analyse something (and I don't claim to be an expert in it) and not knowing about it didn't make any difference to anybody in my class so far but still, I think it is unfortunate that these misconceptions still exist. So I am wondering why we were not taught this at the junior college level where we knew about electric and magnetic fields, vectors and calculus.
 
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  • #22
cnh1995 said:
So I am wondering why we were not taught this at the junior college level where we knew about electric and magnetic fields, vectors and calculus.
In the end, it's down to the fact that you have only so many hours of tuition time and they have to choose what to include in any syllabus. You will probably find that some other stuff that you are taught is not taught elsewhere.
Often the choices are based on the sort of research programs that the University is engaged in.
 
  • #23
jim hardy said:
I hope not !
Electronics is a lot of fun... i still remember my elation when it dawned on me how that compensated ion chamber works.
@Bipolar Demon Work your basics in your head until you've resolved the seeming conflicts. When a mental model leads intuitively to the formula by a couple different thought paths you've built another powerful mental tool. Keep them sharp , like fine chisels.

yes I had done upto norton and thevinin theorems and could solve problems based on those, owever I would not get many right I think, then i got distracted in self teaching mathematics and logic which didn't really help either(not too much progress there either). I need to solve more problems everyday is all, thanks again.

I am basically an idiot and was even thinking of switching to pure math but will continue with the degree. am not trying to self indulge, must do it as I have no other choice and want to learn. Still, I feel the knowledge I got from this inquiry is very valuable.
 
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  • #24
Bipolar Demon said:
I need to solve more problems everyday is all, thanks again.

We learn by doing.
Amateur Radio might be an interesting hobby for you. "Hams" are DIY'ers. Their ARRL books (Amateur Radio Relay League) are a great mix of theory with "How To" directions.

See this thread and observe the high caliber of the help from guys here on PF.
https://www.physicsforums.com/threads/can-i-parallel-yagis.806936/

ARRL Antenna Handbook is a must-have.
 
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FAQ: Voltage derivation for charged particles

What is voltage derivation for charged particles?

Voltage derivation for charged particles refers to the process of calculating the potential difference between two points in an electric field due to the presence of charged particles.

How is voltage derived for charged particles?

Voltage is derived by considering the electric field created by the charged particles and calculating the work done to move a test charge from one point to another. This work done is equal to the potential difference or voltage between the two points.

What factors affect the voltage derivation for charged particles?

The voltage derivation for charged particles is affected by the amount of charge present, the distance between the two points, and the nature of the medium in which the charged particles are located.

Why is voltage derivation important in understanding electric fields?

Voltage derivation allows us to understand the strength and direction of the electric field created by charged particles. This is important in understanding how electric fields affect the movement and behavior of charged particles.

What are some real-world applications of voltage derivation for charged particles?

Voltage derivation for charged particles has many practical applications, such as in the design of electronic devices, power generation and distribution, and medical imaging techniques such as magnetic resonance imaging (MRI).

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