In case of one dimensional heat conduction in a medium with constant properties, T is a temperature at position x, at time t. then \(\frac{\partial T}{\partial t}\) is proportional to

1
\(\frac{T}{x}\)
2
\(\frac{\partial T}{\partial x}\)
3
\(\frac{\partial^2 T}{\partial x\partial t}\)
4
\(\frac{\partial^2 T}{\partial x^2}\)
5
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