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PHYS140 - Ch15.pptx
PHYS140 - Ch15.pptx

... (b)  If  6.3×103  J  is  exhausted  to  the  low  temperature  reservoir,  how  much  work   does  the  engine  do? The  heats  exchanged  at  the  reservoirs  are  related  to  each  other  through       ...
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Thermo-regulation - Learning Central

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... 5.4 cm and is wrapped with a thickness of 5.2 cm of fiberglass insulation. A length D = 6.2 m of the pipe passes through a room in which the temperature is TR = 11C. (a) At what rate does heat energy pass through the insulation? (b) How much additional insulation must be added to reduce the heat tr ...
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15-2 Thermodynamic Processes and the First Law

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... When a substance is heated, its temperature rises. Heat decreases or increases the temperature of a body. For instance, when heat is added the temperature will become higher (Halliday & Resnick, 2013). In a similar manner, when heat is removed, the temperature will become lower. It is worth noting t ...
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... until a temperature in the middle is reached (thermal equilibrium). Big picture – Energy flows from warm objects to cold objects. This flow of energy is called heat (Q). Details – Molecules in the warmer object collide with molecules in the colder object and transfer their kinetic energy to them ...
heat
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... until a temperature in the middle is reached (thermal equilibrium). Big picture – Energy flows from warm objects to cold objects. This flow of energy is called heat (Q). Details – Molecules in the warmer object collide with molecules in the colder object and transfer their kinetic energy to them ...
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... If there's nonzero net heat flow per unit area out of the slab, this heat must be generated internally in the slab. In that case:  d 2T  dq q(y  y)  q(y)  y  yk 2  yH, dy  dy  ...
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Heat pipe



A heat pipe is a heat-transfer device that combines the principles of both thermal conductivity and phase transition to efficiently manage the transfer of heat between two solid interfaces.At the hot interface of a heat pipe a liquid in contact with a thermally conductive solid surface turns into a vapor by absorbing heat from that surface. The vapor then travels along the heat pipe to the cold interface and condenses back into a liquid - releasing the latent heat. The liquid then returns to the hot interface through either capillary action, centrifugal force, or gravity, and the cycle repeats. Due to the very high heat transfer coefficients for boiling and condensation, heat pipes are highly effective thermal conductors. The effective thermal conductivity varies with heat pipe length, and can approach 7002100000000000000♠100 kW/(m⋅K) for long heat pipes, in comparison with approximately 6999400000000000000♠0.4 kW/(m⋅K) for copper.
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