Chapter 4 First Law of Thermodynamics - Thermodynamics, Mechanical Engineering Mechanical Engineering Notes | EduRev

Mechanical Engineering SSC JE (Technical)

Mechanical Engineering : Chapter 4 First Law of Thermodynamics - Thermodynamics, Mechanical Engineering Mechanical Engineering Notes | EduRev

The document Chapter 4 First Law of Thermodynamics - Thermodynamics, Mechanical Engineering Mechanical Engineering Notes | EduRev is a part of the Mechanical Engineering Course Mechanical Engineering SSC JE (Technical).
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Chapter 4

FIRST LAW OF THERMODYNAMICS

  • The First Law of Thermodynamics states that heat is a form of energy, and thermodynamic processes are therefore subject to the principle of conservation of energy. This means that heat energy cannot be created or destroyed. It can, however, be transferred from one location to another and converted to and from other forms of energy.

Chapter 4 First Law of Thermodynamics - Thermodynamics, Mechanical Engineering Mechanical Engineering Notes | EduRev

where ΔU denotes the change in the internal energy  of a closed system

Q denotes the quantity of energy supplied to the system as heat, and 

W denotes the amount of thermodynamic work done by the system on its surroundings. 

 System undergoing change of states

Qnet = ΔE +W
(Q+ Q3 – Q1) = ( ΔE +W2 +W3 - W 1- W4 )

Chapter 4 First Law of Thermodynamics - Thermodynamics, Mechanical Engineering Mechanical Engineering Notes | EduRev

  • Energy is a point function and a property of the system. Energy is an extensive property while specific energy is an intensive property.
  •  The internal energy depends only on temperature, The enthalpy also depends only on temperature for an ideal gas.

  Heat transfer at constant volume

Chapter 4 First Law of Thermodynamics - Thermodynamics, Mechanical Engineering Mechanical Engineering Notes | EduRev

Chapter 4 First Law of Thermodynamics - Thermodynamics, Mechanical Engineering Mechanical Engineering Notes | EduRev

Cv = speecific heat at constant volume

  • Heat transfer at constant volume increases the internal energy of the system.

 Heat transfer at constant pressure

Chapter 4 First Law of Thermodynamics - Thermodynamics, Mechanical Engineering Mechanical Engineering Notes | EduRev

Cp = Specific heat at constant pressure

  •  Heat transfer at constant pressure increases the enthalpy of the system.

  Heat transfer for an isolated system

dQ = 0, dw = 0 & dE = 0

  • Energy of an isolated system is always constant.
  • PMM-1 There can be no machine which would continuously supply mechanical work without absorbing some other form of energy simultaneously. Such a fictitions machine is called perpetual motion machine of first kind (PMM–1)
  • The first law states the principle of conservation of energy.
  • A PMM–1 is the impossible.
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