How Do You Calculate the Electrostatic Force Between Two Charged Lines?

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SUMMARY

The discussion focuses on calculating the electrostatic force between two charged lines, specifically an infinite line of charge with charge density 'a' and a line AB with charge density 'b'. The key formula used is F=qE, which is expanded to F_vec = integral (dq E_vec). The discussion emphasizes the importance of diagrams for visualizing the problem, labeling quantities, and understanding the radial E-field behavior as described by Gauss's law. The integration limits and the direction of the electric field are critical for accurate calculations.

PREREQUISITES
  • Understanding of electrostatics, specifically electric fields from line charges.
  • Familiarity with Gauss's law and its application to infinite charge distributions.
  • Proficiency in calculus, particularly integration techniques for variable limits.
  • Ability to construct and interpret diagrams in physics problems.
NEXT STEPS
  • Study the application of Gauss's law to various charge distributions.
  • Learn about the concept of electric field lines and their properties.
  • Explore advanced integration techniques in physics, focusing on variable limits.
  • Practice constructing diagrams for electrostatic problems to enhance problem-solving skills.
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This discussion is beneficial for physics students, educators, and anyone interested in mastering electrostatics and the calculation of forces between charged objects.

mousesgr
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Electricity and Magnetism urgent!pls!

An infinite long line of charge of constant charge density a is located near the line AB which carries uniform charges with charge density b. Suppose both two lines are in the same plane, calculate the electrostatic force exerted on the line AB.

i don't know how to start...
 
Last edited:
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Always start with a diagram, with labels
and a coordinate system. Label the items
described in the problems' situation,
and the quantity being asked about.

F=qE becomes F_vec = integral (dq E_vec).
Gauss says the infinitely-long charge density
carries a radial E-field that drops off as 1/r,
so unless AB is parallel to it, E=E(r).

If this sounds like gobbledy-gook, drop.
If this sounds like simple stuff you already knew,
the don't say "I don't know how to start".
 
the diagram

what is the limit of the integal then?
a to b or 0 to b?
 

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you only need to integrate where the charges are ...
Your Diagram should include a dx (label it!)
and an E-field (presuming lamda_1 >0) at dx

F_on_dq = (dq)(E_at_dq)

If you integrate from 0 to A, use dq =0 there!
between A and B , dq = "b"dx .
 
lightgrav said:
you only need to integrate where the charges are ...
Your Diagram should include a dx (label it!)
and an E-field (presuming lamda_1 >0) at dx

F_on_dq = (dq)(E_at_dq)

If you integrate from 0 to A, use dq =0 there!
between A and B , dq = "b"dx .

what is the direction of dx & e-field then?
 
Come on! E-field due to the infinite line of charge
points _away_ from the positive charges there.

dx or dr is the coordinate (NOT vector) along line AB,
which is a geometric way of keeping track of the charges.
You're just adding F_vectors for each charge on AB ...
the total amount of charge on line AB is :
integral(dq) = integral(lamda_2 * dx) = lamda_2 * Length.

But don't expect F_total to be E(a+b/2) * lamda_2 * L !
 

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