Thermal energy is the energy that a system has because of the energy present in its moving particles. Several particles interact amongst themselves in complicated ways, but if they meet the right criteria, the system is said to be in equilibrium. This leads to the creation of the first, second, and third laws of thermodynamics.
The branch of science that deals with the quantitative relationship between heat and other forms of energy is called thermodynamics.
The chemical energy stored by the molecules generates heat in the chemical reactions when a fuel burns in the air. Herein, several energies are interrelated and may transform into each other, and the study of this energy transformation forms the basis of thermodynamics.
The first, second, and third laws of thermodynamics apply only when a system is in equilibrium or moves from one equilibrium state to another.
Internal Energy (E or U) is the total energy within the substance. It is the sum of several types of energies like vibrational energy, translational energy, etc.
For an exothermic process, ΔU = -ve, whereas for an endothermic process, ΔU = +ve.
The work done by a system is the quantity of energy that is exchanged between a system and its surroundings.
The heat in thermodynamics is the kinetic energy of the molecules of the substance.
This law states that if the two systems are in thermal equilibrium with a third system, they are in turn in thermal equilibrium with each other. The temperature is recorded to find out whether the system is in thermal equilibrium or not.
The first law is often formulated as ΔU = Q − W, where:
Now if,
The limitations of the first law of thermodynamics are as follows:
Question: Determine the internal energy of a system that has constant volume, and the heat around the system is increased by 50 J.
Solution: Given, q = 50 J
Since the gas has constant volume, ΔV = 0
So work done
W = PΔV = 0
The equation for internal energy is ΔU = q + W
ΔU= q + 0
ΔU = q = 50 J
The second law is also known as the “law of increased entropy.”
Mathematically,
ΔSuniv > 0
where ΔSuniv is the change in the entropy of the universe.
Some factors may cause an increase in the entropy of the closed system. These are as follows:
Question: A heat pump uses 300 J of work to remove 400 J of heat from the low-temperature reservoir. How much heat is being delivered to a higher temperature reservoir?
Solution:
W = 300 J
QC = 400 J
QH = W + QC
QH = 300 J + 400 J
QH = 700 J
The heat delivered to the higher temperature reservoir is 700 J.
The temperature at which all particle motion almost stops is absolute zero. It is the lowest possible temperature, and is equivalent to -273.15 degrees Celsius, -459.67 degrees Fahrenheit, and 0 Kelvin.
These laws are being observed regularly in everyday life.
Every day, ice needs to be maintained at a temperature below the freezing point of water to remain solid. The first and second laws of thermodynamics act in this process. It is the total amount of heat in the system that is the same and has just moved towards the equilibrium at the same temperature.
An example of a closed system in thermodynamics can be a room full of sweaty people where no heat is lost and is only transferred, thus approaching equilibrium with maximum entropy.
Thermodynamics deals with energy changes in chemical or physical processes which enable us to study these changes quantitatively to make successful predictions. For such purposes, the universe is divided into systems and surroundings. The chemical or physical processes lead to the formation of heat (q), part of which may be converted into work (w). Entropy will increase with softer and less rigid solids, that is, solids that contain larger atoms and solids with a complex molecular structure.
In a thermodynamic sense, a living cell can be viewed as a low-entropy system that is not in equilibrium with the surroundings and is capable of replicating itself. A constant input of energy is needed to maintain the cell’s highly organised structure, its wide range of biomolecules, and its intricate system of thousands of chemical reactions.