| 1 | \documentclass{article} |
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| 2 | \usepackage{pstricks} |
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| 3 | \usepackage{fullpage} |
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| 4 | \begin{document} |
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| 5 | \begin{enumerate} |
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| 6 | \item Freezing by radiation and convection |
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| 7 | |
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| 8 | Castings with large open tops often ``freeze off'' by radiation and |
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| 9 | convection, forming a solid shell on top and trapping the liquid beneath it. |
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| 10 | (Because the liquid shrinks during solidification, this results in a large |
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| 11 | shrinkage cavity.) Here you will analyze the rate of solidification downward |
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| 12 | from the top surface in an low-carbon steel ingot casting due to these |
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| 13 | factors. |
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| 14 | |
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| 15 | \begin{center} |
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| 16 | \input{ingotcast} |
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| 17 | \end{center} |
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| 18 | |
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| 19 | Assume that the temperature is uniform, and for part \ref{qtotal}, the |
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| 20 | environment around the casting is gray along with the solid shell. |
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| 21 | |
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| 22 | Iron data: |
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| 23 | \begin{itemize} |
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| 24 | \item Electrical conductivity near melting point: $\rm\sigma=5\times10^{5} |
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| 25 | (\Omega\cdot m)^{-1}$. |
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| 26 | \item Wiedmann-Franz constant: $L=2.45\times10^{-8} \frac{\rm W\Omega}{\rm |
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| 27 | K^2}$. |
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| 28 | \item Density: $\rm\rho=7500\frac{kg}{m^3}$. |
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| 29 | \item Heat capacity: $c_p=500\frac{\rm J}{kg\cdot K}$ |
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| 30 | \item Melting point: $T_m=1800{\rm K}$. |
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| 31 | \item Heat of fusion: $\Delta H_f=2.67\times10^5\frac{J}{kg}$ |
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| 32 | \item Radiative emissivity: $\epsilon=0.6$ |
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| 33 | \item Radiation constant: $\rm\sigma=5.67\times10^{-8}\frac{W}{m^2K^4}$. |
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| 34 | \item Heat transfer coefficient to air: $h=100\frac{\rm W}{\rm m^2\cdot K}$. |
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| 35 | \end{itemize} |
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| 36 | |
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| 37 | \begin{enumerate} |
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| 38 | \item Estimate the thermal conductivity of iron near its melting point. |
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| 39 | \item \label{qtotal} Write an expression for the total radiative and |
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| 40 | convective heat flux from the top surface of the solidifying metal shell to |
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| 41 | the surrounding environment. |
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| 42 | \item \label{htotal} Assuming the environment is much colder than the shell |
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| 43 | and absorbs all radiation ({\em i.e.} is ``black''), calculate a total |
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| 44 | ``heat transfer coefficient'' which is the ratio between heat flux and |
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| 45 | absolute temperature. |
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| 46 | \item \label{unifthick} Use your heat transfer coefficient from part |
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| 47 | \ref{htotal} to estimate the thickness of solid metal $Y$ at which |
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| 48 | temperature can no longer be considered uniform (where the Biot number |
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| 49 | reaches 0.1). |
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| 50 | \item Estimate the rate of growth of the solid while solidification rate is |
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| 51 | limited by radiation/convection from the top surface (that is, while solid |
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| 52 | temperature can be considered uniform). How long does it take to reach the |
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| 53 | thickness calculated in part \ref{unifthick}? |
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| 54 | \item Set up the equation for solidification rate limited by both |
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| 55 | radiation/convection from the top and also (quasi-steady-state) conduction |
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| 56 | through the solid. |
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| 57 | \end{enumerate} |
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| 58 | \end{enumerate} |
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| 59 | \end{document} |
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