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A long metallic bar is carrying heat from one of its ends to the other end under steady state. The variation of temperature θ along the length x of the bar, measured from its hot end, is best described by which of the following?

Asked in AIEEE 2009 · Temperature profile along a bar

Figure: Temperature profile along a bar
Answer: (2) θ falls linearly with x

Step-by-step solution

Idea: in the steady state no heat piles up anywhere, so the same current (dQ)/(dt) crosses every cross-section of the bar.

With the sides insulated, (dQ)/(dt)=-KA(dθ)/(dx) with K, A and (dQ)/(dt) all constant.

So (dθ)/(dx) is a constant, and θ falls along a straight line from the hot end to the cold end.

θ(x)=θₕₒₜ-((θₕₒₜ-θ_cold)/ℓ)x.

If instead the bar were left bare, heat would leak from the sides, the current would fall as x grew, and the graph would bend into the exponential θ-θ₀=(θ₁-θ₀)e^-mx.

Why the other options are wrong

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