(1) First Law of Thermodynamics, Basic Introduction - Internal Energy, Heat and Work - Chemistry
Introduction to the First Law of Thermodynamics
The first law states that energy cannot be created or destroyed; it can only be transferred between systems.
Energy Transfer Mechanisms
Energy can be transferred into or out of a system in two ways:
Heat (Q): When heat flows into a system, it increases the internal energy of that system.
Work (W): When work is performed on a system, it also increases the internal energy.
Example: If 300 joules of work is done on a system, its internal energy increases by 300 joules.
Conceptual Example
Analogy with Money:
Selling a laptop for $500 means your bank account increases by $500 while the buyer's account decreases by $500.
The concept of energy follows this model: energy is not created; it is transferred.
Different System Types
Open System:
Matter and energy can enter and exit.
Closed System:
Only energy can flow in and out; matter cannot.
Isolated System:
Neither matter nor energy can enter or leave; the total energy and mass remain constant.
Change in Internal Energy Equation
The formula for change in internal energy is:
ΔU = Q + W (Chemistry Perspective)
ΔU = Q - W (Physics Perspective)
Significance of Q and W
Q: Heat energy transfer
Positive when heat is absorbed (endothermic)
Negative when heat is released (exothermic)
W: Work done
Positive when work is done on the system
Negative when work is done by the system
Perspectives on Work
Chemistry Perspective:
From this viewpoint:
When work is done by the system, W is negative; internal energy decreases.
Physics Perspective:
From this viewpoint:
When work is done by the system, W is positive; surroundings gain energy.
Important Notes on System Energies
Q is positive for endothermic reactions (heat absorbed) and negative for exothermic (heat released).
W is negative when work is done by the system and positive for work done on the system.
Conclusion
Understanding the sign conventions of Q and W is essential for applying the first law of thermodynamics in practical scenarios, particularly when solving problems related to internal energy changes.