The potential due to an infinitely long line of charge is not absolute and is usually expressed relative to a reference point due to it diverging at infinity. We express it as a potential difference between two points.
Due to the cylindrical symmetry, it's often more useful to express the potential in cylindrical coordinates.
Here's the breakdown:
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Problem: Calculating the electric potential V at a distance s from an infinitely long line of charge with uniform linear charge density λ (charge per unit length).
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Challenge: The integral for potential diverges at infinity. This means we cannot define an absolute potential. Instead, we calculate the potential difference between two points.
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Potential Difference: Let's calculate the potential difference between a point s and a reference point s0.
The potential difference V(s) - V(s0) is given by:
V(s) - V(s0) = - (λ / 2πε0) ln(s / s0)
where:
- V(s) is the electric potential at a distance s from the line.
- V(s0) is the electric potential at a reference distance s0 from the line.
- λ is the linear charge density (charge per unit length).
- ε0 is the permittivity of free space (approximately 8.854 x 10-12 F/m).
- ln is the natural logarithm.
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Explanation:
- The formula shows that the potential decreases logarithmically as you move away from the line of charge.
- The potential is defined relative to a reference point s0. Choosing a different s0 simply shifts the potential by a constant.
- Due to the ln(s) dependence, the absolute potential (if we tried to define it as V(∞) = 0) would be infinite. This is why potential differences are more meaningful in this scenario.
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Important Considerations:
- This formula is valid only for an infinitely long line of charge. In reality, all lines have a finite length. However, this is a good approximation when the distance s is much smaller than the length of the line.
- The line of charge is assumed to be uniform, meaning that the charge density λ is constant along its length.
In summary, you can't define a single formula for the potential due to an infinite line of charge without specifying a reference point. The key is the potential difference, which is given by V(s) - V(s0) = - (λ / 2πε0) ln(s / s0).