Finding the net field strength due to a line of charge

In summary, the homework equation dE = λk \int_0^a \frac{dx}{r^2} is equivalent to dE_x = λk \int_0^a \frac{dx}{r^2} cosθ dE_x = λk \int_0^a \frac{dx}{r^2} \frac{x}{r} dE_x = λk \int_0^a \frac{xdx}{r^3} dE_x = λk \int_0^a \frac{x dx}{(R^2 + x^2)^{3/2}} dE_x
  • #1
Ocasta
40
0
I want to apologize ahead of time for my apparent inability to get LaTeX to display properly.

Homework Statement


prob2-33.png


λ = 3.8 x 10^(-6) C/m

R = 32m

r = magnitude of the hypotenuse (the book's convention, a poor choice IMHO)
r = [itex] \sqrt{R^2 + x^2} [/itex]

k = 8.988 x 10^9

P:(0,-32)

cosθ = x/r

a→∞

Homework Equations


[itex] dE = λk \int_0^a \frac{dx}{r^2}[/itex]

The Attempt at a Solution



We're supposed to figure out the overall field strength, which is finite.

[itex]dE = λk \int_0^a \frac{dx}{r^2} [/itex]

[itex]dE_x = λk \int_0^a \frac{dx}{r^2} cosθ [/itex]

[itex]dE_x = λk \int_0^a \frac{dx}{r^2} \frac{x}{r}[/itex]

[itex]
dE_x = λk \int_0^a \frac{xdx}{r^3}
[/itex]

[itex]
u = R^2 + x^2 → \frac{du}{2} = xdx
[/itex]

[itex]
dE_x = λk \int_0^a (u)^{-3/2} du
[/itex]

[itex]
dE_x = λk [ -2 u^{-1/2} ]_0^a
[/itex]

[itex]
dE_x = -2λk [ (R^2 + x^2)^{-1/2} ]_0^a
[/itex]

[itex]
dE_x = -2λk [ \frac{1}{\sqrt{R^2 + x^2}} ]_0^a
[/itex]

[itex]
dE_x = -2λk [ \frac{1}{\sqrt{R^2 + \inf^2}} - \frac{1}{\sqrt{R^2}} ]
[/itex]

[itex]
dE_x = -2λk [ 0 - \frac{1}{\sqrt{R^2}} ]
[/itex]

[itex]
dE_x = -2λk [ \frac{1}{R} ]
[/itex][itex]
dE_x ≈ -2.13465 x 10^3
[/itex]
 
Last edited:
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  • #2
Looks good, though the sign is important to how you're defining your coordinate system. Make sure your coordinate system is the one the program is looking for.
 
  • #3
I literally pasted all the information I was given. >.< Do you have any guidance as to how to figure out what coordinate system I should use?
 
  • #4
I mean, typically we would define y is being up and x as being right. But you could do any permutation of those. I guess I don't understand what your questions about the problem are.
 
  • #5
So I talked to my Physics professor, and he took a look at it. Evidently I forgot to carry over an x.

Ocasta said:
[itex]dE = λk \int_0^a \frac{dx}{r^2} [/itex]

[itex]dE_x = λk \int_0^a \frac{dx}{r^2} cosθ [/itex]

[itex]dE_x = λk \int_0^a \frac{dx}{r^2} \frac{x}{r}[/itex]

[itex]
dE_x = λk \int_0^a \frac{x dx}{r^3}
[/itex]

[itex]
dE_x = λk \int_0^a \frac{x dx}{(R^2 + x^2)^{3/2}}
[/itex]

[itex]
dE_x = λk [ \frac{-1}{\sqrt{R^2 + x^2}} ]_0^a
[/itex]

[itex]
dE_x = λk [ \frac{-1}{\sqrt{R^2 + ∞^2}} - \frac{-1}{\sqrt{R^2 + 0^2}} ]
[/itex]

[itex]
dE_x = λk [ 0 + \frac{+1}{\sqrt{32^2}} ]
[/itex]

[itex]
dE_x = λk \frac{1}{\sqrt{32^2}}
[/itex]

[itex]
dE_x ≈ 1.0673 * 10^3 \frac{N}{C}
[/itex]

Why the solution is positive still confounds me.
 
Last edited:
  • #6
Ah, whoops, that is easy to do. Yeah, I didn't really check all your steps, just that the integration was correct.
 
  • #7
Mindscrape said:
Ah, whoops, that is easy to do. Yeah, I didn't really check all your steps, just that the integration was correct.

The most frustrating part is that I apparently was correct the first time, but the answer they wanted was positive rather than negative. But looking at the problem, the vector is clearly negative in the X and Y directions!
 

1. What is the formula for finding the net field strength due to a line of charge?

The formula for finding the net field strength due to a line of charge is given by E = (k * Q) / r, where k is the Coulomb's constant, Q is the charge on the line, and r is the distance from the line of charge to the point where the field is being measured.

2. What units are used for the net field strength due to a line of charge?

The units for net field strength due to a line of charge are newtons per coulomb (N/C).

3. How does the distance from the line of charge affect the net field strength?

The net field strength due to a line of charge decreases as the distance from the line increases. This relationship follows an inverse square law, meaning that the strength of the field is inversely proportional to the square of the distance.

4. What is the direction of the net field strength due to a line of charge?

The direction of the net field strength due to a line of charge is radially outward from the line of charge. This means that the field lines point away from the line of charge in all directions.

5. How can we use the superposition principle to find the net field strength due to multiple lines of charge?

The superposition principle states that the total field at a point due to multiple charges is equal to the vector sum of the fields due to each individual charge. Therefore, to find the net field strength due to multiple lines of charge, we can simply calculate the field due to each line separately and then add them together to get the total field.

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