Electric Field and infinite line of charge

AI Thread Summary
To solve the problem of an infinite line of charge exerting a force on an electric dipole, begin by considering a small charge element dx at a distance x from the dipole. The charge of this element is given by λ(dx), where λ is the linear charge density. Calculate the force acting on the dipole from this charge element and then integrate this force over the entire length of the line of charge. Remember to account for the vector nature of force, integrating along the appropriate components. The final expression for the force on the dipole is F = (2)(λ)(p) / (4)(π)(ε₀)(r²), assuming r is significantly larger than the dipole's charge separation.
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Can someone show me or give me an idea on how to start this problem.

Show that an infinite line of charge with linear charge density lamda exerts an attractive force on an electric dipole with magnitude F = (2)(Lamda)(p) / (4)(pie)(Epsilon knot)(r^2). Assume that r is much larger than the charge separation in the dipole.
 
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You can assume the linear charge density to be along the x-axis, and keep your origin such that the point at which force is to be calculated lies on the y-axis at a distance of r.

start with taking a small element dx at a distance x.

Since linear charge density is \lambda, the charge on that element is \lambda(dx)

Find the force on the dipole by this element and then integrate over the entire length of the charge. Don't forget that force is a vector, and integration should be done along the respective components.
 
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