Eliminating arguments from a function

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The discussion centers on the mathematical problem of eliminating arguments from functions in the context of thermodynamics. Specifically, it addresses the relationship between functions f1, f2, and f3, where f1 and f2 are dependent on a variable z, and f3 is set to zero. The conclusion drawn is that if f3 equals zero, it is possible to define functions g1 and g2 such that g1(x) equals g2(y), effectively demonstrating that f1 and f2 can be reduced to forms independent of z. This reduction is crucial for establishing the independence of the functions involved.

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thegreenlaser
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My issue comes from thermodynamics (https://www.physicsforums.com/threads/zeroth-law-of-thermodynamics-and-empirical-temperature.774255/), but I guess this is really a math problem rather than a physics problem:

Let [itex]\boldsymbol{x} \in \mathbb{R}^m[/itex], [itex]\boldsymbol{y} \in \mathbb{R}^n[/itex], [itex]\boldsymbol{z} \in \mathbb{R}^p[/itex].

Given
[tex]f_1 (\boldsymbol{x}, \boldsymbol{z} ) = f_2 (\boldsymbol{y}, \boldsymbol{z})[/tex]
and
[tex]f_3(\boldsymbol{x}, \boldsymbol{y}) = 0,[/tex]
how can we show that there exist functions [itex]g_1, g_2[/itex] such that
[tex]g_1(\boldsymbol{x}) = g_2(\boldsymbol{y})[/tex]

(i.e., [itex]f_3 = 0[/itex] means that [itex]f_1[/itex] and [itex]f_2[/itex] can be reduced so they're independent of [itex]\boldsymbol{z}[/itex])

In my physics class, we were given a sort of "hand-waving" argument, but I'm having trouble finding a more rigorous explanation. Can anyone help me out?
 
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I have trouble understanding the question, but I'll take a stab at it. The last comment says f1 and f2 can be reduced to be independent of z. In that case wouldn't g1 and g2 simply be these reduced versions of f1 and f2?
 

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