Electric Field: Continuous Charge Distribution

In summary: I'm not sure what you mean by "the equation for the electric field of the sphere". It would help to see what you are thinking of using.If you are talking about the field at some point P, and the point of interest is not within the charged sphere, then you can use:##\vec{E} = \frac{1}{4 \pi \epsilon_0} \frac{Q}{R^2} \hat{r}##Where ##\vec{r}## points from the center of the sphere to the point P, and ##\hat{r}## is the unit vector in the direction of ##\vec{r}##.(You have to be careful with this.
  • #1
sxal96
15
1

Homework Statement


A nonconducting sphere 1.3 m in diameter with its center on the x axis at x = 4 m carries a uniform volume charge of density ρ = 4.8 µC/m3. Surrounding the sphere is a spherical shell with a diameter of 2.6 m and a uniform surface charge density σ = -1.2 µC/m2. Calculate the magnitude and direction of the electric field at the following locations.
1) x = 4m, y = 1.2m
2) x = 2m, y = 3m
Both answers are in components of i[hat] and j[hat] vectors with units of N/C.

Homework Equations


Well, the textbook solutions use the following equations...
Eshell = kQshell/r2 r[hat]
It uses three different equations for the sphere for each part. Not sure where it got most of these equations as in the textbook itself, these are the equations. I can include the solutions' equations but when I tried their way of solving, my answer was wrong.
Esphere = Qk/r2 (when r is greater than or equal to R)
Esphere = Qkr/R3 (when r is less than or equal to R)

The Attempt at a Solution


I know that the x component of 1) is 0 because that's where the center of the sphere is at. However I'm honestly stumped on how to solve for the y component of 1) and subsequently how to solve 2) in general. As I already mentioned I tried the equations in the textbook solutions but they gave me the wrong answer and didn't explain why they used certain numbers or equations.

For 1), the electric field of the shell is 0 since the point is within the shell. I tried the equations in the textbook itself and I guess (and am absolutely confident this is wrong) the equation for the sphere's electric field is

Esphere = k*ρ*4πr4/R3 r[hat]

I have limited tries on the online homework so detailed help would be greatly appreciated. I tried reading the textbook as well as other textbooks and websites and online videos and I'm still stuck. Thanks.
 
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  • #2
If you draw a vector from the center of the spheres to a given point, how would you find the x and y components of that vector (think right triangles)? How do you form a unit vector from a given vector?

Layout.png
 
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  • #3
gneill said:
If you draw a vector from the center of the spheres to a given point, how would you find the x and y components of that vector (think right triangles)? How do you form a unit vector from a given vector?

View attachment 90419
The x and y components would be the radius (which is the hypotenuse, if I'm not mistaken) times cos θ and sin θ respectively. And the unit vector of a given vector is the x and y components of that vector divided by the magnitude of the vector itself.
 
  • #4
Sure. But you are given the actual points so you have a way to determine the components directly. Here's the same image with one of the vectors drawn:
Layout2.png


You should be able to see the vector components. Use the given point location coordinates to calculate the components.
 
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  • #5
gneill said:
Sure. But you are given the actual points so you have a way to determine the components directly. Here's the same image with one of the vectors drawn:
View attachment 90421

You should be able to see the vector components. Use the given point location coordinates to calculate the components.

So I got that the magnitude of the vector is approximately 3.606m at an approximate angle of 56.309°.

##\vec{r} = -3.606 \cos(56.309) \hat{i} + 3.606 \sin(56.309) \hat{j}##

Thus ##\hat{r} = -0.5547 \hat{i} + 0.83205 \hat{j}##.

Would I use that ##\hat{r}## for the equation of the sphere's electric field?
 
  • #6
You've done a lot of extra work using trig functions. You don't need to find the angle. You have a right angle triangle whose sides ARE the components of the vector. The starting and ending points of the vector are all you need: Δx and Δy.

You use the magnitude of the actual vector in the field magnitude part of the expression, the unit vector (##\hat{r}##) just gives the directional component. Since it has unit magnitude it doesn't change the magnitude of the result.
 
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  • #7
gneill said:
You've done a lot of extra work using trig functions. You don't need to find the angle. You have a right angle triangle whose sides ARE the components of the vector. The starting and ending points of the vector are all you need: Δx and Δy.

You use the magnitude of the actual vector in the field magnitude part of the expression, the unit vector (##\hat{r}##) just gives the directional component. Since it has unit magnitude it doesn't change the magnitude of the result.
So would that mean that I only use the fact that ##\hat{r} = - \hat{i} + \hat{j}##?

Also, if my equation for the electric field of the sphere is correct, would I plug in r = 3.606m and R = 1.2m?
 
  • #8
sxal96 said:
So would that mean that I only use the fact that ##\hat{r} = - \hat{i} + \hat{j}##?
No, the unit vector here is a vector of unit length that points in the direction of the vector in question. ##- \hat{i} + \hat{j}## does not have a magnitude of unity, and it doesn't point in the direction of either of the vectors of interest in this problem.

The use of unit vectors is a way to separate the magnitude and direction parts of a given vector. Say that you have some vector ##\vec{R}##. It has a magnitude ##R = |\vec{R}|##. Now, if ##\vec{r}## is unit vector in the same direction as ##\vec{R}##, then you can write:

##\vec{R} = R \vec{r}##

You can then use scalar operations to handle the magnitude calculations (avoiding all that slogging through vector dot and cross products), and then tack on the correct unit vector to give the direction.

You found the unit vector for the case under discussion as ##\hat{r}## in post #5.
Also, if my equation for the electric field of the sphere is correct, would I plug in r = 3.606m and R = 1.2m?
I'm not sure if I'm interpreting your meaning correctly. Can you be more explicit? How about showing the full calculation for the point at (2,3) m ?
 
  • #9
I have an attempted equation (excluding values) for the electric field of the sphere toward the end of my original post,

Esphere
= k*ρ*4π*r4/R3 r[hat]

I don't know how to do the full calculation at point (2m, 3m). but the above equation is my guess of what to use to find the electric field of the sphere at the point (4m, 1.2m)
 
  • #10
sxal96 said:
I have an attempted equation (excluding values) for the electric field of the sphere toward the end of my original post,

Esphere
= k*ρ*4π*r4/R3 r[hat]

I don't know how to do the full calculation at point (2m, 3m). but the above equation is my guess of what to use to find the electric field of the sphere at the point (4m, 1.2m)

Okay, that doesn't look right to me. Perhaps the meaning of r and R are changing as we go along? There are a lot of different radii in this problem.

Can you spell out the definitions of various r's in that equation? I'm thinking that I should be able to spot the calculation for the volume of the inner sphere in there (for calculating the total charge of the sphere), but I'm not seeing it. Perhaps you should detail your derivation. Start with defining the variables and then proceed to calculate the charge on the sphere.
 
  • #11
Here is a picture from my textbook that would probably illustrate what the differences between r and R are better than I could by explaining it. I used the equation of the electric field when r is less than or equal to R and set Q = ρV. Since the volume of a sphere is 4πr3, I substituted all of those things and got that really crazy equation.

When I plug in my numbers (with r = 0.65 m and R = 1.2m) I obtain 56004.61984 N/C but that doesn't seem correct.
 

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  • #12
Check your formula for the volume of a sphere. You're missing a constant.

The point you are dealing with is outside the sphere, so r > R. The spherical charge should "look like" a point charge to the observer at the point in question, so the usual Coulomb's law version for point charges will work fine there.

You can check the sanity of an equation by making sure that the units balance and work out to what you expect. Plug in unis for the variables and see if they boil down to what you expect.
 
  • #13
Ahhh I forgot to divide by 3. I checked the variables and the units should come out to N/C if I am working on the electric field of the sphere at (4m, 1.2m).

Are you referencing the point (2m, 3m) as being outside of the sphere?
 

Related to Electric Field: Continuous Charge Distribution

What is an electric field?

An electric field is a physical quantity that describes the force exerted by electrically charged particles on other charged particles within the field. It is a vector quantity, meaning it has both magnitude and direction.

How is an electric field created?

An electric field is created by electrically charged particles, such as protons and electrons. When these particles are in motion or are in proximity to each other, they create an electric field. The strength of the field is determined by the magnitude of the charges and the distance between them.

What is a continuous charge distribution?

A continuous charge distribution refers to a system of charged particles that are distributed continuously throughout a given space. This is in contrast to a discrete charge distribution, where the charges are located at specific points.

How is the electric field calculated for a continuous charge distribution?

The electric field for a continuous charge distribution is calculated by integrating the electric field contributions from each infinitesimal charge element within the distribution. This integration takes into account the magnitude and location of each charge, as well as the distance between the charge and the point at which the electric field is being measured.

What are some practical applications of understanding electric fields in continuous charge distributions?

Understanding electric fields in continuous charge distributions is important for many practical applications, such as designing electronic devices, predicting the behavior of charged particles in electric and magnetic fields, and calculating the forces experienced by charged objects in different scenarios. It also has applications in fields such as electromagnetism, electronics, and electrical engineering.

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