Equation of electric field line

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Discussion Overview

The discussion revolves around the interpretation of the electric field represented by the vector E⃗ =(4iˆ+4jˆ) N/C, specifically whether it can be considered as an equation of electric field lines and the implications of its uniformity. Participants explore concepts related to electric potential, the nature of electric fields, and the mathematical relationships between electric field and potential.

Discussion Character

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

Main Points Raised

  • Some participants question the meaning of the electric field vector E⃗ =(4iˆ+4jˆ) N/C and whether it represents an electric field line.
  • Others clarify that the vector indicates a uniform electric field in the x-y plane directed at a 45-degree angle, with a magnitude of 4√2 N/C.
  • There is a discussion on how to determine the uniformity of the electric field, with some stating it has no dependency on spatial coordinates, while others argue that the presence of unit vectors i and j implies a dependence on coordinates.
  • Participants provide examples of non-uniform electric fields and discuss the implications of vector components on uniformity.
  • Concerns are raised about the understanding of electric potential and its relationship with electric field, with some participants asserting that the potential at two points in a uniform field should be the same.
  • There are questions regarding the interpretation of derivatives in the context of electric potential and electric field relationships, with some participants challenging the mathematical treatment of these concepts.

Areas of Agreement / Disagreement

Participants express differing views on the uniformity of the electric field and the implications for electric potential at different points. The discussion remains unresolved, with multiple competing interpretations and no consensus reached on the correctness of the claims made.

Contextual Notes

Limitations include potential misunderstandings of vector calculus and the definitions of electric field and potential. The discussion also reflects varying levels of familiarity with the underlying mathematical concepts.

gracy
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There is a sentence

In the electric field E⃗ =(4iˆ+4jˆ) N/C, electric potential at A(4 m, 0) is more than the electric potential at B(0, 4 m)


I want to know what does it mean electric field E⃗ =(4iˆ+4jˆ) N/CIs it equation of electric field line?But how will it represent electric field line.Because it is only a point.

field line.png

 
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gracy said:
Because it is only a point.
It's not a point, it's a vector. ##\mathbf{E} = 4\hat{i}+4\hat{j}## physically means that there is a uniform electric field in the x-y plane directed 45 degree from the x (or y) axis with the strength ##4\sqrt{2}## N/C.
 
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blue_leaf77 said:
axis with the strength 4√2.
How did you know the strength?
blue_leaf77 said:
that there is a uniform electric field
How can we figure out that it's uniform?
blue_leaf77 said:
x-y plane directed 45 degree from the x (or y) axis
How can we know the direction?
 
gracy said:
How did you know the strength?
The strength or magnitude of ##\mathbf{E}## is equal to ##|\mathbf{E}|##.
gracy said:
How can we figure out that it's uniform?
It has no dependency on space coordinates.
gracy said:
How can we know the direction?
How do you normally calculate the direction of a vector?
 
blue_leaf77 said:
It has no dependency on space coordinates.
But it has i and j ,it means it depends on coordinates
 
gracy said:
But it has i and j ,it means it depends on coordinates
No. Those are unit vectors, not coordinates.
 
Gracy, I don't think PhysicsForums is helping you. You've asked us about vectors in the past, and now it's clear you haven't learned them.

The problem is that you immediately jump to asking a question here without having put much work into it, and when you are guided by someone towards the answer, you don't try and work it out for yourself, but instead ask for another hint. And another. And another. Eventually, you have been hinted all the way to the answer. Well, you've gotten the answer, but you haven't really learned.

You're going to have to decide if you want to learn or not. If you want to learn, you are going to have to spend more time thinking and working on your own. In this case, your starting point for basic vectors shouldn't be asking for more hints - it should be going back to your past materials and see if you can solve this using what you have already been told.
 
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gracy said:
How can we figure out that it's uniform?
blue_leaf77 said:
It has no dependency on space coordinates.
More explicitly, the equation \vec E = 4 \hat i + 4 \hat j does not contain x and/or y.
 
But i is for x and j is for y,right?
 
  • #10
An example of non-uniform vector field may look like ##\mathbf{E}(x,y) = 3xy\hat{i} + y^2\hat{j}##. Now you see that both the magnitude and direction of this E field is dependent on (x,y). I hope this helps.
 
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  • #11
you mean when x an y are there in the equation of E,it is non uniform?
 
  • #12
gracy said:
But i is for x and j is for y,right?

When we use ##\hat i## and ##\hat j## in a position vector, then they are associated with x and y, e.g. ##\vec r = 3 \hat i + 4 \hat j## means x = 3 and y = 4. More generally ##\vec r = x \hat i + y \hat j##.

When we use ##\hat i## and ##\hat j## in an electric field vector, then they are associated with the vector components ##E_x## and ##E_y##, e.g. ##\vec E = 5 \hat i + 6 \hat j## means ##E_x = 5## and ##E_y = 6##. More generally ##\vec E = E_x \hat x + E_y \hat y##.

In the example above, ##E_x## and ##E_y## do not depend on position (x and y), so this ##\vec E## is uniform.

In blue_leaf77's example ##\vec E = 3xy \hat i + y^2 \hat j##, we have ##E_x = 3xy## and ##E_y = y^2##, both of which depend on position, so this ##\vec E## is not uniform.

Going further with blue_leaf77's example, at the position ##\vec r = 3 \hat i + 4 \hat j##, i.e. at (x,y) = (3,4), we have ##\vec E = 36 \hat i + 16 \hat j##. At the position ##\vec r = 5 \hat i + \hat j##, i.e. at (x,y) = (5,1), we have ##\vec E = 15 \hat i + \hat j##. Etc.
 
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  • #13
It may be non-technical advice but I think you should really first try to put your own effort up to the point where you are really really in impasse in dealing with the problem you are facing with all resources in your hand. Meaning, if there is still opportunity to get the answer from passive sources like books or internet site, the last one being abundant in our current age, go for this option. I just tried typing "uniform vector field" in google and the first site to result is found in this very forum you are asking the same question, it's this one https://www.physicsforums.com/threads/what-is-a-uniform-vector-field.483218/. It has been more than 4 hours since you asked what non-uniform vector means, and imagine what you would have gotten done had you done what I just did with my browser. I believe the answer to the other 2 questions you asked in post #3 can also quickly be retrieved with the help of your browser. Prioritizing to be independent is the first key to being full-fledged in whatever field one is pursuing.
 
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  • #14
Actually I do search on browser first then come up with my specific doubts/questions(may be silly at times)but today I was really busy in some personal matter .I asked the question then closed the window then I found out I got a reply,I read it and wrote what first thought came in my mind after reading that.I have also tried to search for this topic I had written the topic only to realized that there is no internet access .

I should not have done that.I am extremely sorry.I won't do it again.If any such situation comes again I will totally detach myself from studies for some time until I am all free for my studies.I promise.:smile:
 
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  • #15
gracy said:
In the electric field E⃗ =(4iˆ+4jˆ) N/C, electric potential at A(4 m, 0) is more than the electric potential at B(0, 4 m)
I think this statement is wrong because potential at both the points will be same
##\vec{E}##=##\frac{dV}{dr}##

Since electric field is uniform here we can use

##\vec{E}##=##\frac{V}{r}##

##V##=##\vec{E}##×##r##

As E and r both are same for given two points A and B.

Potential should also be same for both.
Right?
 
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  • #16
gracy said:
Right?
NO, it is not an explanation.
What does r mean? What are the points between the potential difference is asked?
Look after how is electric potential difference defined.
What is the relation between electric potential and electric field.
 
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  • #17
ehild said:
What does r mean?
dv/dr is the the derivative of voltage with respect to position. It represents the magnitude of the electric field at a point. r is the position of the point
ehild said:
What are the points between the potential difference is asked?
Actually potential is asked not potential difference.
ehild said:
What is the relation between electric potential and electric field.

##\vec{E}##=##\frac{dV}{dr}##
 
  • #18
gracy said:
dv/dr is the the derivative of voltage with respect to position. It represents the magnitude of the electric field at a point. r is the position of the point

Actually potential is asked not potential difference.##\vec{E}##=##\frac{dV}{dr}##
How do you differentiate a function with respect to position?
The question is where the potential is greater. You have to compare potentials at two different points.
What is the potential function in this case?
 
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  • #19
Dear Gracy,
Can you help me understand your ##\vec E = {dV\over dr}## ? The thing on the left is a vector. How do I have to interpret the thing on the right ? Because of the equals sign, it has to be a vector, but I don't see it !
 
  • #20
##\vec E## = ##\frac{dV}{\vec dr}##
 
  • #21
r is position vector.
 
  • #22
Doesn't work! See Ehild post :smile:

When you look up the definition of a derivative you will find that you can't apply it this way.
 
  • #23
gracy said:
r is position vector.
How can the position vectors of points A(4,0) and B(0,4) the same?
 
  • #24
My point (and Elizabeth's point as well) was that you can't differentiate wrt a vector. So you can write $$
V_A - V_B = \int_A^B \vec E {\bf \cdot } d\vec s
$$ (Note that now you have a scalar on the left side and on the right side of the = sign).

But the other way around you can only write $$
E_x = -{dV\over dx}, \ E_y = -{dV\over dy}, \ E_z = -{dV\over dz}
$$ which can also be written as $$\vec E = - \nabla V$$

In your case you have the components of ##\vec E## readily available: ##E_x = 4## and ##E_y = 4## so it's not all that difficult to find an expression for V -- except that you can't take V = 0 at infinity as a reference. In such a case, the origin can be a good place to set V = 0 there.

Back to post #1. What does "the electric field ##\vec E = (4{\bf \hat\imath} + 4 {\bf \hat\jmath}) ## N/C" mean ?

It means that at every point in the plane, the electric force per coulomb is a vector with an x-component of 4 and a y component of 4 . So it must point in a direction with an angle of ##\pi\over 4## wrt the positive x-axis. Hence the magnitude ##4\sqrt 2## in an earlier post.

upload_2015-12-11_18-52-21.png
 

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  • #25
upload_2015-12-11_18-52-21-png.93240.png

is it equivalent to the following
i.png
 
  • #26
Equivalent is ambiguous here.

There are two vectors in this exercise: one vector is the Eleftric field (the force as a function of position -- although here the function is a constant), the other is the position vector in the x-y plane (like the position vector of A is ##(4\hat\imath+0\hat\jmath)## .Anyway, now comes the hammer: when I move from point ##A = (4\hat\imath+0\hat\jmath)## to point ## B=(0\hat\imath+4\hat\jmath)## via a straight line, then it seems to me that $$
V_A - V_B = \int_A^B \vec E {\bf \cdot } d\vec s = 0 $$ because everywhere the ## \vec E {\bf \cdot } d\vec s = 0 ## !

(##d\vec s = (\hat\imath - \hat\jmath)\, ds##)

--
 
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  • #27
There are position vectors, pointing to a point from the origin, and there are free vectors, representing vector quantities which are functions of position. The independent variable is position vector and the dependent variable is a free vector.

upload_2015-12-11_22-36-17.png

The electric field is free vector, ##\vec E ## in every point P. It is the same vector at point A (position vector ##\vec a ##) and also at point B (position vector ##\vec b ##) .
The potential difference VB-VA is equal to the negative work done by the electric field when a unit positive charge moves from A to B. When the field is uniform, this work is equal to the electric field times displacement, ##W=\vec E\cdot\Delta \vec r##. ##\Delta r = \vec b-\vec a##. Calculate ##\vec \Delta r ## and multiply it by ##\vec E##.
You certainly remember what you learned about equipotential surfaces, that they are perpendicular to the field lines. Here the field lines are straight lines with slope 1. The equipotentials in the plane are lines perpendicular to the former ones, having slope -1. The displacement from ##\vec a - \vec b## is along an equipotential.
 
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  • #28
I think
##\Delta \vec r##=##\vec b## - ##\vec a##
I think there's a period "." in the text being confused as a mathematical operator.
It's two separate equations
##W##=##\vec E\cdot\Delta \vec r##

##\Delta \vec r##=##\vec b-\vec a##

Right?
 
  • #29
gracy said:
I think
##\Delta \vec r##=##\vec b## - ##\vec a##
I think there's a period "." in the text being confused as a mathematical operator.
Gracy, it is a full stop at the end of the sentence.
 
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  • #30
I had written

##\vec{E}##=##\frac{dV}{dr}##

It is wrong because on left side there is a vector quantity(##\vec{E}##)and on right hand side both quantities are scalar at least one quantity on right hand side should be vector.
And we know ##\vec{dr}## is position vector

Hence ##\vec{E}##=##\frac{dV}{\vec{dr}}##

But it is also wrong because division of vector is not allowed as direction can not be divided.

Therefore

##dV##=##\int_A^B \vec E {\bf \cdot } d\vec r ##

##V_A##- ##V_B## =##\int_A^B \vec E {\bf \cdot } d\vec r ##

##\vec{E}## is uniform and hence it can be taken out of integral

=##\vec{E}##. ##\int_A^Bd\vec r ##

=##\vec{E}##. ##\vec b##-##\vec a##

on Putting values we get..

##V_A##- ##V_B## = ##(4\hat\imath+4\hat\jmath)##.[##(4\hat\imath+0\hat\jmath)##-(##0\hat\imath+4\hat\jmath)]####V_A##- ##V_B## = ##(4\hat\imath+4\hat\jmath)##.##(4\hat\imath-4\hat\jmath)##

##V_A##- ##V_B## =(4)(4)+(4)(-4)##V_A##- ##V_B##=16-16=0

Potential difference between points A and B is 0.Hence the statement

In the electric field E⃗ =(4iˆ+4jˆ) N/C, electric potential at A(4 m, 0) is more than the electric potential at B(0, 4 m)

is wrong.

Right?
 
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