What's the meaning of Neumann BCs in heat conduction problems?

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What's the meaning of Neumann BCs in heat conduction problems?

Such as given here:

https://web1.eng.famu.fsu.edu/~dommelen/pdes/style_a/svbex.html

Why does one specify $u_x=g_0$ at the end of the rod. Rather than $u=g_0$?

Is it because it's assumed to "change", whereas the start of rod is thought to "have an initial value"?

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You can think of Neumann BCs as fixing the heat flux and Dirichlet BCs, of course, fix the temperature.

You could generally specify either; they're just different problems. For example, $\partial_x u =0$ on the endpoints would imply perfect insulation (no heat flux). On the other hand, you could specify $u=0$ which would say that the temperature is fixed at zero at the endpoints of the rod.