The equation in post 4, f= (1/2L) * Sqrt(T/u)
tells us half the story. If we consider 2 strings of the same length L vibrating at the same frequency f, then increasing u means you must increase T.
The relationship between u and the gauge of the string is simple. u is mass per unit length. The mass, m, of a length l of guitar string (assuming it to be a cylinder) is density (p) times volume (v), which is p * (Pi*r^2) * l (Volume is cross section x length, and cross section is Pi r squared, where r is radius of wire)
As wire gauge is a measure of its diameter (d), the formula becomes
u = m/l = p * Pi * (d/2)^2 (because r=d/2)
The equation at the top tells us that sqrt (T/u) is a constant (for the same f and length of string) therefore T/u is constant. (The value of the constant is (2fL)^2)
So T=u times this constant
u=p * Pi * (d/2)^2
so
T =
If you do this you get a formula that calculates the tension (in Newton) in the string for a given gauge (d), frequency (f), length (L) and density (p)
Can you get an expression for T?
If the tension in a string is greater, then you need more force to displace it to one side in order to set it in motion. More "strum". So heavier gauge strings do not "move" so much for the same amount of applied strumming force. Or, looking at it another way, you can strum them harder and get the same displacement to one side.
This displacement of the string to one side is closely related to its amplitude once it starts vibrating. So you can strum harder without buzzing, caused by too great amplitude.
The mathematics that deals with how this string displacement then relates to the amplitude of the stable vibration is rather complex. However, in simple terms it can be said to be more or less proportional.
It is that amplitude that then determines the loudness of the sound.
Do you follow the reasoning so far?
The next stage is to look at what determines the energy of this vibration. If the problem is simplified somewhat, it can be considered to depend on the product of u, frequency squared and amplitude squared.
This then gives the relationship between the amplitude (a) of the string and the gauge, for strings of the same material, length and frequency vibrating with the same energy (loudness).
In other words, all other things being constant
amplitude squared is proportional to 1/ u
but u is proportional to gauge (d) squared, so
the amplitude is inversely proportional to the gauge.
What this means is that, all other things being equal (strings have same length, material, frequency and energy(loudness) then you can say that increasing the gauge decreases the (required) amplitude. In fact, if you double the one you half the other.
From this you can work out what changing gauge does to the amplitude.
I would stress that this is a very simplified analysis and hasn't taken account of a large number of other factors. If anyone else wants to come in on this and comment on my reasoning I would be very grateful.