Chapter 2: Problem 140
What kinds of differential equations can be solved by direct integration?
Chapter 2: Problem 140
What kinds of differential equations can be solved by direct integration?
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Get started for freeThe variation of temperature in a plane wall is determined to be $T(x)=110 x-48 x\( where \)x\( is in \)\mathrm{m}\( and \)T\( is in \){ }^{\circ} \mathrm{C}$. If the thickness of the wall is \(0.75 \mathrm{~m}\), the temperature difference between the inner and outer surfaces of the wall is (a) \(110^{\circ} \mathrm{C}\) (b) \(74^{\circ} \mathrm{C}\) (c) \(55^{\circ} \mathrm{C}\) (d) \(36^{\circ} \mathrm{C}\) (e) \(18^{\circ} \mathrm{C}\)
What is the difference between an algebraic equation and a differential equation?
What is heat generation? Give some examples.
Consider a \(1.5-\mathrm{m}\)-high and \(0.6-\mathrm{m}\)-wide plate whose thickness is \(0.15 \mathrm{~m}\). One side of the plate is maintained at a constant temperature of \(500 \mathrm{~K}\), while the other side is maintained at \(350 \mathrm{~K}\). The thermal conductivity of the plate can be assumed to vary linearly in that temperature range as \(k(T)=k_{0}(1+\beta T)\) where \(k_{0}=25 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K}\) and $\beta=8.7 \times 10^{-4} \mathrm{~K}^{-1}$. Disregarding the edge effects and assuming steady onedimensional heat transfer, determine the rate of heat conduction through the plate.
A spherical shell with thermal conductivity \(k\) has inner and outer radii of \(r_{1}\) and \(r_{2}\), respectively. The inner surface of the shell is subjected to a uniform heat flux of \(\dot{q}_{1}\), while the outer surface of the shell is exposed to convection heat transfer with a coefficient \(h\) and an ambient temperature \(T_{\infty}\). Determine the variation of temperature in the shell wall, and show that the outer surface temperature of the shell can be expressed as $T\left(r_{2}\right)=\left(\dot{q}_{1} / h\right)\left(r_{1} / r_{2}\right)^{2}+T_{\infty}$
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