Minki said:
Hi PF, Many thanks for your very comprehensive reply!
That's exactly what I meant. So I think it would be fair to say that if an expression can be represented as a linear graph going through the origin on both x and y-axis then the deltas are not needed, as in the case of Ohms Law.
Faraday's law is actually about the instantaneous rate of change of flux.
ε = -N dψ/dt
where calculus is used. dψ/dt is the slope of the ψ vs t graph at a particular instant of time t. Δψ/Δt approximates this slope if Δt is sufficiently small and the graph isn't too curvy at the point of interest.
When you say the graph is linear, then it has a constant slope so dψ/dt = Δψ/Δt = a constant. Only when the linear graph starts at the origin can the second part of each delta equal zero. A graph can still be linear and not start at the origin.
The deltas are always needed because emf is only induced when the flux *changes*. If the flux is constant so that Δψ = 0, there is no emf, ie ε=0. If you don't write these deltas, the equation is not complete and even misleading. Writing ε = -N ψ/t is neither accurate mathematically nor does it describe to anyone reading it that ε depends on the rate of change of flux.
I was about to tell you that Ohm's Law is nothing like that but of course that's not quite true and is probably why you brought this up at all :) But in the application of Ohm's law, it is understood that the voltage is the voltage across the circuit element so ΔV = V
at top of element - V
at bottom of element is understood to mean 'V'. And in a perfectly analogous way to the flux, the voltage drop across that space is the average electric field E = - ΔV/Δx
So I know the point you are making -- we've dropped the ΔV in Ohm's law. The problem with the change in flux is dropping the Δψ/Δt would make the problems harder to solve because important information would be missing (understood to be there) that would make it difficult to solve equations with derivatives in them.