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| 183_notes:examples:thermal_equilibrium [2014/10/28 05:02] – created pwirving | 183_notes:examples:thermal_equilibrium [2014/10/28 13:54] (current) – pwirving | ||
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| Final State: Blocks have come to thermal equilibrium, | Final State: Blocks have come to thermal equilibrium, | ||
| + | 300 gram block of aluminum which is at a temperature of 500 K | ||
| - | === Lacking === | + | 650 gram block of iron which is at a temperature of 350 K |
| + | Aluminum is placed on iron | ||
| + | Both in insulated enclosure | ||
| + | |||
| + | Specific heat capacity of aluminum is approximately 1.0 J/K/gram | ||
| + | |||
| + | Specific heat capacity of iron is approximately 0.42 J/K/gram | ||
| + | |||
| + | Metal blocks reach same temperature | ||
| + | |||
| + | |||
| + | === Lacking === | ||
| + | |||
| + | $T_{f}$ common temperature | ||
| === Approximations & Assumptions === | === Approximations & Assumptions === | ||
| Line 39: | Line 53: | ||
| The total energy of the two blocks does not change, because there is no energy transfer from or to the surroundings. | The total energy of the two blocks does not change, because there is no energy transfer from or to the surroundings. | ||
| + | |||
| + | Therefore we want to solve for $T_{f}$ which is the final temperature for both blocks. | ||
| $m_{1}C_{1}(T_{f} - T_{1i}) + m_{2}C_{2}(T_{f} - T_{2i}) = 0$ | $m_{1}C_{1}(T_{f} - T_{1i}) + m_{2}C_{2}(T_{f} - T_{2i}) = 0$ | ||
| + | |||
| + | Substitute in values for all known variables and solve for $T_{f}$. | ||
| $(300g)(1.0 J/ | $(300g)(1.0 J/ | ||