First Law of Thermodynamics – To understand the relation between heat and work first we need to understand the concept of internal energy. Just like mass, energy is always conserved i.e. it can neither be created nor destroyed but it can be transformed from one form to another. Internal energy is a thermodynamic property of the system that refers to the energy associated with the molecules of the system which includes kinetic energy and potential energy.
Whenever a system goes through any change due to interaction of heat, work and internal energy, it is followed by numerous energy transfer and conversions. However, during these transfers, there is no net change in the total energy.
What is the First Law of Thermodynamics?
The first law of thermodynamics states that the energy of the universe remains the same. Though it may be exchanged between the system and the surroundings, it can’t be created or destroyed. The law basically relates to the changes in energy states due to work and heat transfer and defines the conservation of energy.
First Law of Thermodynamics Equation
The equation for the first law of thermodynamics is given as;
ΔU = q + W
- ΔU = change in internal energy of the system.
- q = algebraic sum of heat transfer between system and surroundings.
- W = work interaction of the system with its surroundings.
Points to Remember
- For an isolated system, energy (E) always remains constant.
- Internal Energy is a point function and property of the system. Internal energy is an extensive property (mass-dependent) while specific energy is an intensive property (independent of mass).
- For an ideal gas, the internal energy is a function of temperature only.
First Law of Thermodynamics Limitations
The first law of thermodynamics states that whenever a system undergoes any thermodynamic process it always holds certain energy balance. However, the first law fails to give the feasibility of the process or change of state that the system undergoes.
For instance, the first law fails to explain why heat flows from hot end to cold end when a metallic rod is heated at one end and not on other and vice-versa. The first law only quantifies the energy transfer that takes place during this process. It is the second law of thermodynamics which provides the criterion for the feasibility of the various processes. We will take an example and understand the concept further.
Perpetual Motion Machine of First Kind (PMM1)
It is impossible to construct a machine that can continuously supply mechanical work without consuming any energy simultaneously. Such a hypothetical machine is known as the perpetual motion machine of the first kind. These types of machines violate the 1st law of thermodynamics and do not exist in reality.
Work done for a closed system is the product of pressure applied and the change in volume that occurs due to applied pressure :
w = − P ΔV
where P is the constant external pressure on the system, and ΔV is the change in volume of the system. This is specifically called “pressure-volume” work.
The internal energy of a system increases or decreases depending on work interaction that takes place across its boundaries. The internal energy would increase if work is done on the system and decreases if work is done by the system. Any heat interaction that takes place in the system with its surroundings also changes its internal energy. But since energy remains constant ( from the first law of thermodynamics ), the total change in internal energy is always zero. If energy is lost by the system, then it is absorbed by the surroundings. If energy is absorbed into a system, then it implies that the energy was released by the surroundings:
ΔUsystem = −ΔUsurroundings
where ΔUsystem is the change in the total internal energy of the system, and ΔUsurroundings is the change in the total energy of the surrounding.
Carefully study the table given below:
|Process||Sign Convention for heat(q)||Sign Convention for work(w)|
|Work done by the system||N/A||–|
|Work done on the system||N/A||+|
|Heat extracted from the system||–||N/A|
|Heat added to the system||+||N/A|
For a closed system;
|Process||Internal energy change||Heat (q)||Work(w)||Example|
|Adiabatic (q=0)||+/-||0||+/-||An isolated system in which heat neither enters nor leaves|
|+/-||+/-||0||A hard, pressure isolated system like a bomb calorimeter|
|+/ –||Enthalpy||− p ΔV||Most processes occur in constant external pressure|
|Isothermal||0||+/-||-/+||There is no change of temperature like a temperature bath|