# What Am I Doing Wrong in Calculating Potential on a Grid?

• ab200
In summary, due to symmetry, the bottom-left negative charge and the bottom-right positive charge cancel out, leaving me with a triangle around the center. I'm not entirely sure how to solve for potential at the origin specifically, but I believe that the potential energy of a system is equal to the external work needed to assemble it.
ab200
Homework Statement
Five charges are arranged as shown below. Each charge is either +1.5 nC (red) or -1.5 nC (blue). They are spaced by 1 cm intervals (each dotted line is 1 cm long). What is the potential, in V, at the origin?

How much work do you have to do, in electron volts (eV), to move an electron from infinitely far away to the origin?
Relevant Equations
V = kq/r
U = qV
Looking at the image, I see that due to symmetry, the bottom-left negative charge and the bottom-right positive charge cancel out, leaving me with a triangle around the center. I'm not entirely sure how to solve for potential at the origin specifically, but I believe that the potential energy of a system is equal to the external work needed to assemble it.

Thus, U = k [(q1q2 / r12) + (q2q3 / r23) + (q1q3 / r13)]. But I got a very, very small number that doesn't seem right, plus U is in joules, not volts. If I divide by 1.6e-19 to convert to volts, I get an enormous number that doesn't seem right either.

What am I doing wrong in terms of problems setup?

#### Attachments

• potentials.PNG
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There is a problem with your strategy. The problem is asking you to find the work that you (an external agent) have to do to bring an electron from infinity to the origin. What procedure are you going to follow to find this work? Work is denoted by ##W## but see no relevant equation that involves it. How do you propose to include that? Also, in your equation for U you have q1, q2 and q3. Which one of these is the electron charge?

MatinSAR
ab200 said:
I believe that the potential energy of a system is equal to the external work needed to assemble it.
You are not asked for the potential energy of the system. You are asked for the potential energy of a test charge in the field of the system. I see that same question asked twice. Once as a request for potential and once as a request for work along a trajectory.

If it were me, I'd work on some additional cancellation.

MatinSAR
jbriggs444 said:
You are asked for the potential energy of a test charge in the field of the system.
Actually it's an electron.

kuruman said:
Actually it's an electron.
The same question is asked twice. Once asking for Volts and once asking for electron volts per electron.

kuruman said:
There is a problem with your strategy. The problem is asking you to find the work that you (an external agent) have to do to bring an electron from infinity to the origin. What procedure are you going to follow to find this work? Work is denoted by ##W## but see no relevant equation that involves it. How do you propose to include that? Also, in your equation for U you have q1, q2 and q3. Which one of these is the electron charge?
Yes, in this case work is equal to the change in potential energy. The electron charge for part 2 of the question would be q4, with the relevant U values being U14, U24, and U34.

jbriggs444 said:
You are not asked for the potential energy of the system. You are asked for the potential energy of a test charge in the field of the system. I see that same question asked twice. Once as a request for potential and once as a request for work along a trajectory.

If it were me, I'd work on some additional cancellation.
Yes, I figured this out. I was missing that the first part of the question actually asks for electric potential V rather than potential energy U. The equation for the electric potential of the system (multiple) of point charges is V = V1 + V2 + V3.

You’re right about the second part as well. I, not being the brightest, ended up solving for the potential energy of the system U = U14 + U24 + U34 (where q4 is the new electron charge). Given that U14 = V1 x q4, U24 = V2 x q4, etc. when I converted the final answer for U from joules in the electron volts, I ended up dividing by the value of q4 anyway.

ab200 said:
The equation for the electric potential of the system (multiple) of point charges is V = V1 + V2 + V3.
It’s easier than that!

The total potential at the origin can be thought of as the sum of 3 contributions:

1) from the bottom left and the bottom right charges;
2) from the top left and the bottom middle charges;
3) from the top right charge.

What can you say about 1) and 2)?

MatinSAR
Steve4Physics said:
It’s easier than that!

The total potential at the origin can be thought of as the sum of 3 contributions:

1) from the bottom left and the bottom right charges;
2) from the top left and the bottom middle charges;
3) from the top right charge.

What can you say about 1) and 2)?
I see that in 1), the two charges are symmetric about the y axis. However, in case 2) I’m a little bit confused why they cancel each other out. Yes, they are equal distances from the origin, but does that necessarily mean they cancel out? If the bottom middle and top right charges were switched, I would be totally on board, but maybe I’m still missing something.

ab200 said:
Yes, they are equal distances from the origin, but does that necessarily mean they cancel out?
Yes.

ab200 said:
However, in case 2) I’m a little bit confused why they cancel each other out. Yes, they are equal distances from the origin, but does that necessarily mean they cancel out?
Don't get potentials (scalars) mixed up with electric fields (vectors).

If you were adding fields at a point, the direction (as well as the magnitude) of each individual field would be very important. You would have an exercise in vector addition.

But adding potentials at a point is much simpler – elementary addition. That's one reason why physicists often prefer to use potentials when dealing with fields - it makes the maths much simpler.

ab200, jbriggs444, MatinSAR and 1 other person

## What is the potential of a charge on a grid?

The potential of a charge on a grid refers to the electric potential at a given point in space due to the presence of one or more electric charges. It is a scalar quantity and is typically measured in volts. The potential at a point is determined by the sum of the contributions from all individual charges on the grid, taking into account their positions and magnitudes.

## How is the electric potential calculated for multiple charges on a grid?

The electric potential at a point due to multiple charges is calculated by summing the potentials due to each individual charge. For a point at position $$r$$, the potential $$V$$ due to a set of charges $$q_i$$ located at positions $$r_i$$ is given by $$V(r) = \sum_i \frac{k q_i}{|r - r_i|}$$, where $$k$$ is Coulomb's constant. This formula assumes the charges are in a vacuum or air.

## What are the boundary conditions typically applied in grid problems involving charges?

Boundary conditions in grid problems involving charges can vary depending on the specific setup. Common boundary conditions include:1. Dirichlet boundary conditions, where the potential is fixed at the boundaries.2. Neumann boundary conditions, where the derivative of the potential (related to the electric field) is fixed at the boundaries.3. Periodic boundary conditions, where the potential repeats at the edges of the grid. These conditions help in solving the equations governing the potential distribution.

## How does the presence of a dielectric material affect the potential on a grid?

The presence of a dielectric material affects the potential on a grid by reducing the effective electric field generated by the charges. This is due to the dielectric's ability to polarize in response to the electric field, effectively reducing the field strength. The potential in a region with dielectric material is given by $$V = \frac{1}{\epsilon} \sum_i \frac{k q_i}{|r - r_i|}$$, where $$\epsilon$$ is the relative permittivity of the dielectric material.

## What numerical methods are commonly used to solve for the potential on a grid?

Numerical methods commonly used to solve for the potential on a grid include:1. Finite Difference Method (FDM), which approximates the differential equations governing the potential using discrete grid points.2. Finite Element Method (FEM), which divides the grid into smaller, simpler elements and uses variational techniques to solve the potential.3. Method of Moments (MoM), which converts the continuous problem into a discrete one by using basis functions.These methods help in obtaining approximate solutions to complex problems where analytical solutions are difficult or impossible to derive.

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