Find the electrostatic force of interaction between two parallel non conducting wires each of length l , charge density per unit length λ , and separated by a distance d .
Give your answer as the value of this force in Newtons using λ = 1 0 μ C/ m , l = 1 m , d = 1m , 4 π ϵ 0 1 = 9 × 1 0 9 N m 2 / C 2
Note :
The wires completely face each other (like if their equations were 0 ≤ x ≤ L , y , z = 0 and 0 ≤ x ≤ L , y = d , z = 0 )
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Can someone explain where i went wrong? I considered a small element d x on one rod, x distance from one end, with charge d q and integrated, ie, the field at that point due to the second rod times d q (considering just the perpendicular component), and got 0 . 9 as the answer...
Check out my solution.
Why did u take two unit particles diagonally apart
He choose them for the case of generality, You could have just as easily chosen a straight line.
Dude i did tht and taking d charge as lambda × l..n applied d formula (k×(lambda×l)^2)/d^2
@Samarth Rastogi – Hi friend, here we are taking force between two small elements, not the whole wires. You cannot apply the point charge force equation to a distribution of charges. Note that in the expression(in box) if you use l < < < d , you get the answer same as that given by coloumbic force between two charges. This is because if l < < < d , the wire are so small that they can be considered point charges.
@Jatin Yadav – True tht thnks man
@Samarth Rastogi – Try also this inspred problem
Can someone please post a solution for the double integral?
Sure.
First, you should know that ∫ ( a 2 + z 2 ) 3 / 2 d z = a 2 1 z 2 + a 2 z
Here, if a = d , Then the double integral is changed to:
4 π ϵ 0 d λ 2 ∫ 0 l ( ( l − x ) 2 + d 2 l − x + x 2 + d 2 x ) d x
Now, using ∫ 0 a f ( x ) d x = ∫ 0 a f ( a − x ) d x ,
We get 2 π ϵ 0 d λ 2 ∫ 0 l x 2 + d 2 x d x
= 2 π ϵ 0 d λ 2 ( l 2 + d 2 − d )
Nice one. Thanks, Jatin.
We can solve the problem without using the double integral method by using the generalized formula for electric field by finite line of charge.
Hey, I did it in the same manner!
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Consider two elements on the wires of thickness d x and d y respectively on the wires as shown:
Their charges are λ d x and λ d y respectively. Distance between these elements is clearly ( y − x ) 2 + d 2
Hence, the coloumbic force of intersection between the elements is:
d F = 4 π ϵ 0 ( ( y − x ) 2 + d 2 ) λ 2 dx dy
Now, by symmetry, we know that the force would be vertical, so we take only sin θ component.
sin θ = ( y − x ) 2 + d 2 d
F net = ∫ d F sin θ
= ∫ 0 l ∫ 0 l 4 π ϵ 0 ( ( y − x ) 2 + d 2 ) 3 / 2 λ 2 d dx dy
This was tagged calculus due to use of double integral. I leave it on you. Its simple.
Solving this, we get:
F = 2 π ϵ 0 d λ 2 ( l 2 + d 2 − d )
You can verify it by using approximation l < < < d , in which case it gives the force as 4 π ϵ 0 d 2 ( λ l ) 2 (Compare to F = 4 π ϵ 0 r 2 q 1 q 2 )
_Note : _ Anyone unable to solve the definite double integral can freely ask as comment.