Electrostatics and velocity question

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Homework Help Overview

The problem involves an electric field described by the vector \(\vec{E}=x\hat{i}+y\hat{j}\) in the xy-plane, with a small charged ring projected along a smooth non-conducting rod. The objective is to determine the minimum velocity required for the ring to reach the end of the rod, assuming zero gravity.

Discussion Character

  • Exploratory, Assumption checking, Mathematical reasoning

Approaches and Questions Raised

  • Participants discuss the calculation of potential change and work done, with attempts to equate work to kinetic energy. There are questions about the correct integration path and potential maximums along the trajectory.

Discussion Status

Participants are actively exploring the potential energy changes along the path of the ring, with some guidance provided on identifying maximum potential points. There is recognition of previous errors in integration and potential calculations, leading to further clarifications and corrections.

Contextual Notes

There are indications of confusion regarding the integration process and the assumptions about potential energy changes. The discussion reflects on the need to accurately determine the potential difference along the path taken by the ring.

Saitama
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Homework Statement


Electric field given by the vector [itex]\vec{E}=x\hat{i}+y\hat{j}[/itex] is present in xy plane. A small ring carrying charge +Q, which can freely slide on a smooth non conducting rod, is projected along the rod from point (0,L) such that it can reach the other end of the rod. What minimum velocity should be given to the rod? (Assume zero gravity).
ziws28.jpg




Homework Equations





The Attempt at a Solution


I tried finding the change in potential, finding the work done and equating the work done to kinetic energy. Let's assume that it moves a very small displacement dr as shown in the figure.
15d9p54.jpg

It will have components dx[itex]\hat{i}[/itex] and -dy[itex]\hat{j}[/itex].
∴[itex]dr=dx\hat{i}-dy\hat{j}[/itex].
Change in potential, ΔV
[tex]ΔV=-\int\vec{E}\cdot\vec{dr}[/tex]
[tex]=-\int(x\hat{i}+y\hat{j})\cdot(dx\hat{i}-dy\hat{j})[/tex]
[tex]=-\int_{0}^{L}xdx+\int_L^0ydy[/tex]
[tex]=-L^2[/tex]

[tex]QΔV=\frac{1}{2}mu^2[/tex]
where u is the velocity with which ring is projected.
Solving this i get,
[tex]u=\sqrt{\frac{2QL^2}{m}}[/tex]

But this is wrong, the answer is
[tex]u=\sqrt{\frac{QL^2}{2m}}[/tex]

I don't understand where i am doing wrong.
Any help is appreciated. :smile:
 
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dr =dxi+dyj regardless of the direction of the of the path.

ehild
 
ehild said:
dr =dxi+dyj regardless of the direction of the of the path.

ehild

But then i get ΔV=0. :confused:
 
Yes. The change of potential is zero between the initial and final points, but it has a maximum somewhere in between. The kinetic energy has to overcome that maximum potential.
Think: You stand at a fence and you want to throw a ball over the other side. . How much must be the kinetic energy of the ball? You can not say that it is PE(f)-PE(i)=0...

ehild
 
ehild said:
Yes. The change of potential is zero between the initial and final points, but it has a maximum somewhere in between. The kinetic energy has to overcome that maximum potential.
Think: You stand at a fence and you want to throw a ball over the other side. . How much must be the kinetic energy of the ball? You can not say that it is PE(f)-PE(i)=0...

ehild

Is that maximum potential point at (L/2,L/2) ?
 
The field is radial so the potential difference between (0,L) and (L,0) will be 0. However. along the path, the ring will gain potential energy until it is at it's nearest to the origin and then lose it. So take the potential difference between (0,L) and where the ring is nearest the origin in a similar approach as you did.
 
Sleepy_time said:
The field is radial so the potential difference between (0,L) and (L,0) will be 0. However. along the path, the ring will gain potential energy until it is at it's nearest to the origin and then lose it. So take the potential difference between (0,L) and where the ring is nearest the origin in a similar approach as you did.

The nearest point would be then (L/2,L/2).

Okay so i do the integration again.
[tex]ΔV=-(\int_{0}^{\frac{L}{2}}xdx+\int_L^{\frac{L}{2}}ydy)[/tex]

Solving this i get:
[tex]ΔV=\frac{3L^2}{4}[/tex]

But i don't think this is correct. It doesn't lead to the right answer.
 
Pranav-Arora said:
Is that maximum potential point at (L/2,L/2) ?

NO. Find it. Write up the potential along the path as function of the distance from the initial point, and find the local maximum.

ehild
 
Last edited:
ehild said:
NO. Find it. Write up the potential along the path, as function of the distance from the initial point, and find the local maximum.

ehild

Local maximum? How should i go on finding it?
I don't have any equation to perform differentiation. Just a shot in the dark, do i have to use the following equation and set the derivative to zero?

[tex]ΔV=-(\frac{x^2}{2}+\frac{y^2}{2})[/tex]
 
  • #10
Never mind my previous post ehild, i just read your post carefully.
How can i write the potential as a function of distance from initial point? Should i assume that the ring reaches a point (x,y), find the distance?

(I double posted just to let ehild know that there's activity in this thread.)
 
  • #11
You need the maximum along the straight line from (0,L) to (L,0). If s is the distance from the initial point, x=s/√2 and y=L-s/√2. Write the potential energy in terms of s.

ehild
 
  • #12
ehild said:
You need the maximum along the straight line from (0,L) to (L,0). If s is the distance from the initial point, x=s/√2 and y=L-s/√2. Write the potential energy in terms of s.

ehild

I am lost here, i have no idea on this. I hope i am not annoying you. :rolleyes:
 
  • #13
The point charge moves along the blue line. The equation of that line is y=L-x. If the point has started from the upper end, and traveled s distance, it is in point x,y: x=s/√2 (as the line encloses 45°angle with the x axis) and y=L-s/√2.
You derived already that the potential is -1/2(x^2+y^2) with respect to the origin as reference point. In terms of s , it is
V=(-1/2) [(s/√2)2+(L-s/√2)2].

The maximum is when s=L/√2, and this corresponds to the point (L/2;L/2) as you wrote before. The potential is -L^2/4, but you need the change of potential from point (0,L), where it is -L^2/2. The difference is ΔV=L^2/4. You get the same result with integrating along the line from (0,L) to (L/2;L/2); you made simply a sign error in post #7.

ehild
 

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  • #14
ehild said:
The point charge moves along the blue line. The equation of that line is y=L-x. If the point has started from the upper end, and traveled s distance, it is in point x,y: x=s/√2 (as the line encloses 45°angle with the x axis) and y=L-s/√2.
You derived already that the potential is -1/2(x^2+y^2) with respect to the origin as reference point. In terms of s , it is
V=(-1/2) [(s/√2)2+(L-s/√2)2].

Where is it maximum and what is its maximum value?

ehild

Thanks for the help! :smile:
Simplifying the expression you gave me,
[tex]V=\frac{-1}{2}(L^2+s^2-\sqrt{2}Ls)[/tex]
To find the maximum, we need to set the derivative equal to zero, am i right?
[tex]\frac{dV}{ds}=\frac{-1}{2}(2s-\sqrt{2}L)[/tex]
[tex]0=2s-\sqrt{2}L[/tex]
[tex]s=\frac{L}{\sqrt{2}}[/tex]

Therefore x=L/2 and y=L/2. I am afraid that i have done something wrong because these are the same points i stated before.

EDIT:Oops, you edited your post.
 
  • #15
Pranav-Arora said:
Therefore x=L/2 and y=L/2. I am afraid that i have done something wrong because these are the same points i stated before.

EDIT:Oops, you edited your post.

Yes, and (L/2;L/2 was correct, I made some mistakes, too, sorrrrrrry...

Have you got the correct result at last?

ehild
 
  • #16
Yes you are right, i did a mistake while integrating. Thanks for all the help ehild! :smile:
I have got the right answer.
It was really fun.
 

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