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Understanding the First Law of Thermodynamics
Aug 14, 2024
Lecture Notes: First Law of Thermodynamics
Overview
First Law of Thermodynamics
: The change in internal energy of a system is equal to the heat added to the system minus the work done by the system.
Formula
: ( \Delta U = Q - W )
( \Delta U ) = change in internal energy
( Q ) = heat added to the system
( W ) = work done by the system
Example Problems
Example 1: Work done on and heat lost from the gas
Problem
: 60 J of work is done on a gas; the gas loses 150 J of heat.
Calculation
:
Heat lost: ( Q = -150 ) J (since heat left the gas)
Work done on gas: ( W = +60 ) J
( \Delta U = Q + W = -150 + 60 = -90 ) J
Conclusion
: Gas loses 90 J of internal energy; temperature decreases.
Importance of Internal Energy
Internal energy is proportional to temperature.
If internal energy decreases, temperature decreases.
Cannot directly correlate joules to degrees without further specifics of gas.
Example 2: Heat added and work done by the gas
Problem
: Gas starts with 200 J of internal energy; 180 J of heat is added; gas does 70 J of work.
Calculation
:
Heat added: ( Q = +180 ) J
Work done by gas: ( W = -70 ) J
Change in internal energy: ( \Delta U = Q + W = 180 - 70 = 110 ) J
Initial internal energy: 200 J
Final internal energy
: ( U_{final} = 200 + 110 = 310 ) J
Example 3: Work done on and internal energy decrease
Problem
: 40 J of work done on a gas; internal energy decreases by 150 J.
Calculation
:
Internal energy decrease: ( \Delta U = -150 ) J
Work done on gas: ( W = +40 ) J
Solving for heat ( Q ):
( \Delta U = Q + W )
( -150 = Q + 40 )
( Q = -150 - 40 = -190 ) J
Conclusion
: 190 J of heat left the system.
Key Takeaways
Be cautious with positive and negative signs:
Heat added to the system is positive.
Heat lost by the system is negative.
Work done on the system is positive.
Work done by the system is negative.
( Q ) is heat, ( W ) is work, and ( \Delta U ) is the change in internal energy.
Change in internal energy indicates the change in temperature, though not directly measurable as degrees without specific gas details.
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