first law of
Thermodynamics
BY
Er. R.P. Ojha
1R.P. Sir
First law of thermodynamics
Statement 1
Energy can neither be created nor be destroyed, it can
be just changed from one form to another form
Statement 2
Heat and work are mutually convertible
First law for thermodynamic cycle
 Cyclic integral of heat is equal to
cyclic integral of work
Where
δQ = net amount of heat interaction
ΔW = net amount of work interaction
EXAMPLE
 A System undergoes a cycle composed of four
process.the heat transfer to each process are 400kJ,-
365kJ,-200kJ,25o kJ. The respective work transfer are
140kJ,0,-55kJ and 0. is data consistent with first law of
thermodynamics
δQ = 400+(-365)+(-200)+250 =85kJ
ΔW = 140+0+(-55)+0 = 85
Hence given data is consistent with first law of thermodynamics
Example
 The working fluid in a engineexecutes a cyclic process,
and two work interactions involved :10kJ to working
fluid and 30 kJ from the working fluid. The working
cycle also involves three heat transfer, two of which are
75kJ to working fluid and 40 kJ from working fluid.
Determine magnitude and direction of third
interaction
 -15kJ
First law of thermodynamics for process
 Amount of heat interaction
during a process is equal to sum
of amount of work interaction
and change in internal energy
 δQ = Δw + dU
 dU = change in internal energy
Example
 In a general compression process,2 kJ of mechanical
work is supplied to 5kg of working and 800 J of heat is
rejected to cooling jacket. Calcualte change in specific
internal energy
 δQ = Δw + dU
 240 J/kg

First law of thermodynamics

  • 1.
  • 2.
    First law ofthermodynamics Statement 1 Energy can neither be created nor be destroyed, it can be just changed from one form to another form Statement 2 Heat and work are mutually convertible
  • 3.
    First law forthermodynamic cycle  Cyclic integral of heat is equal to cyclic integral of work Where δQ = net amount of heat interaction ΔW = net amount of work interaction
  • 4.
    EXAMPLE  A Systemundergoes a cycle composed of four process.the heat transfer to each process are 400kJ,- 365kJ,-200kJ,25o kJ. The respective work transfer are 140kJ,0,-55kJ and 0. is data consistent with first law of thermodynamics δQ = 400+(-365)+(-200)+250 =85kJ ΔW = 140+0+(-55)+0 = 85 Hence given data is consistent with first law of thermodynamics
  • 5.
    Example  The workingfluid in a engineexecutes a cyclic process, and two work interactions involved :10kJ to working fluid and 30 kJ from the working fluid. The working cycle also involves three heat transfer, two of which are 75kJ to working fluid and 40 kJ from working fluid. Determine magnitude and direction of third interaction  -15kJ
  • 6.
    First law ofthermodynamics for process  Amount of heat interaction during a process is equal to sum of amount of work interaction and change in internal energy  δQ = Δw + dU  dU = change in internal energy
  • 7.
    Example  In ageneral compression process,2 kJ of mechanical work is supplied to 5kg of working and 800 J of heat is rejected to cooling jacket. Calcualte change in specific internal energy  δQ = Δw + dU  240 J/kg