sophiecentaur said:
I am old fashioned enough to rely on Maths to give me a definitive answer and for the Logic of Maths to point me in the right direction. Without some sort of proof / derivation that works with 'Maths', I can't be happy. A proof that comes up with an A>=B type of answer is necessary for me (and a lot of people) to rely on a statement.
This alternative wording of my proof, which includes math, may be more to your liking:
Consider an arrangement of resistors, with a fixed current I
0 passing through the arrangement. Suppose this arrangement is NOT a series connection of all resistors in the given set.
Next, consider some path through the network, and sum up the voltages across each resistor along this path. Since the resistors are not all in series, the path must omit at least one resistor (*** see note below). Moreover, each resistor in the path has at most the applied current going through it. Thus, the sum of the voltages -- and therefore the resistance -- will be less than that of a complete series arrangement.
In mathematical terms:
Note that I
i ≤ I
0 for all resistors, where I
i is the current in the i-th resistor of the non-series arrangement.
Now consider the equivalent resistance,
R
equiv = ΔV / I
0 = ∑(R
i⋅I
i) / I
0
(the summation is calculated using only the resistors along the chosen path)
and compare that to the resistance in a completely series arrangement,
R
series = ΔV
series / I
0 = (∑R
i⋅I
0) / I
0
(this summation is calculated using every resistor, since the only path in the series arrangement is the one that passes through each resistor)
For every term in the sum used to calculate R
equiv, there is a term of equal or greater value in the sum used to calculate R
series. And there will be additional terms in the R
series summation, all positive, so that
R
equiv ≤ R
series
*** Note on paths: While we could make a path pass through every resistor by including closed loops in the path, any loops would have zero voltage by Kirchoff's loop rule and may therefore be removed from consideration.
As for networks with not just series and parallel components, how would you propose to take a delta of resistors and re-arrange them validly to satisfy the simple Parallel to series swap?
I'm not sure why you say we are restricted only to do parallel-to-series swaps.The title of the thread is very general: "Obtaining a maximum resistance given a set of resistors". I take that to mean all possible combinations are under consideration. We only need to compare the delta to a completely series arrangement. It's not necessary that we be able to get there via doing parallel-to-series swaps.
I was limiting my answer to something that I can actually demonstrate to be true. If someone can arrive at a simple inequality expression that's the equivalent to the one I was working with then that's fine. Talking in terms of Volts for a given current is actually precisely the same as comparing resistances and doesn't have an easier solution, imo.
I find it easier to think in terms of comparing voltages -- I guess because it's a more fundamental concept than resistance -- and then dividing by the current in the end to compare the resistances.