This page contains notes on Heat (Q) and derivations for Work (1W2) equations. |
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Heat (Q) |
energy transferred across the system boundary due to a temperature difference.
Heat is transferred from the system at higher temperature to the one at lower temperature.
Heat is an inexact differential -- it is path dependent.
Units |
SI | J, joule |
English | Btu, British Thermal Unit
1 Btu = 778.17 ft-lbf
1 Btu = heat required to raise 1 lb water from 59.5oF to 60.5oF.
[ 1 calorie = heat required to raise 1 gm water from 14.5oC to 15.5oC. ] |
The rate of heat transfer to/from system
Q-dot = |   Q  
  dt |
Specific heat transfer,
- Heat transferred TO a system is POSITIVE.
- Heat transferred FROM a system is NEGATIVE.
Remember,
- Work done BY a system is POSITIVE.
- Work done ON a system is NEGATIVE.
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Some comments on WORK and HEAT |
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- Both are transient
- Both are boundary phenomena
- Both are path functions
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Links to derivations for Work (1W2) equations.
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| W for a process where pV=constant
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| W for a process where pVn=constant
1W2 = |
  p2V2 - p1V1
--------------------       1 - n |
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| W for a process expanding against a LINEAR spring
1W2 = |
(1/2)(p1 + p2)(V2 - V1) = p1(V2 - V1) + (1/2)(p2 - p1)(V2 - V1) |
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- END |