How is the Total Electric Field Calculated for a Ring?

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The discussion clarifies the calculation of the total electric field for a ring by addressing the transition from indefinite to definite integrals in electric field equations. It emphasizes that the limits of integration depend on the geometry of the surface, specifically the ring's circumference. Each segment of the ring is treated as having an infinitesimal charge, allowing for the calculation of total charge through integration. The distinction between indefinite and definite integrals is highlighted, noting that the former is algebraic while the latter incorporates geometric properties. Understanding these concepts is crucial for accurately calculating electric fields in this context.
djMan
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Hi I am pretty confused on how my book is doing the calculus of electric fields. Basically I don't understand how their equation makes any sense (The integral equations on the second page). How does the indefinite integral become a definite integral? Is this a true equality or is it supposed to just represent a concept?
 

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It is because your limits of integration will change depending on the surface you are dealing with. In this case we are dealing with a ring, then we can consider each little bit of the ring having an infinitesimal charge, dq. We can find a linear charge density that that says there is so much charge for so much little bit of ring and call that lambda as shown in your pictures. To find the total charge then we have to sum up all of the little bits of charge over the total ring. Since this is a ring, we are only concerned with the circumference and we integrate with our upper bound being the circumference of the ring.

This obviously changes based on what you are integrating. An indefinite integral is purely algebraic, it was just describing the action done. The indefinite integral becomes definite when we are considering the analytic (geometric) properties of our object.
 
It may be shown from the equations of electromagnetism, by James Clerk Maxwell in the 1860’s, that the speed of light in the vacuum of free space is related to electric permittivity (ϵ) and magnetic permeability (μ) by the equation: c=1/√( μ ϵ ) . This value is a constant for the vacuum of free space and is independent of the motion of the observer. It was this fact, in part, that led Albert Einstein to Special Relativity.
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