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Work & Heat Transfer in Engineering Thermodynamics by PK NAG (Chapter 03)

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116 enrolled
5853 views
Trainers Rating
4(5)
Course type
Watch to learn anytime
Duration
217 min
Start
Anytime
Language
English , Hindi
Views
5853
  • Lifetime access
  • Foundational Learning
  • Access to Study Materials
  • Self-Paced Learning
FREE
Saurabh Kumar Gupta
Saurabh Kumar GuptaMechanical Engineer

Why enroll

People enroll in the course “Work & Heat Transfer” to build a strong foundation in the core principles of thermodynamics and energy exchange, which are essential for understanding how mechanical and thermal systems operate. The course helps learners grasp how energy is transferred as work and heat, enabling them to analyze, design, and improve systems such as engines, heat exchangers, and power plants. It is particularly valuable for students, engineers, and technicians who want to enhance their problem-solving skills, improve energy efficiency, and apply theoretical concepts to real industrial applications.

Course details

Work and heat transfer are two fundamental concepts in thermodynamics that describe the interactions between a system and its surroundings. Work is the transfer of energy through a force applied over a distance, and can be mechanical, electrical, or other forms. Heat transfer, on the other hand, is the transfer of thermal energy due to a temperature difference between systems. Both work and heat transfer can occur through various mechanisms, including conduction, convection, and radiation. Understanding the principles of work and heat transfer is crucial in designing and optimizing energy systems, such as engines, refrigeration systems, and heat exchangers. By analyzing the work and heat transfer interactions in a system, engineers can evaluate its performance, identify opportunities for improvement, and develop more efficient solutions. The study of work and heat transfer is essential in many fields, including mechanical engineering, aerospace engineering, and chemical engineering.

Course suitable for

Is this course for you?

Perfect for

  • You work in Energy & Utilities or HVAC
  • You're a Mechanical Engineering professional
  • You prefer self-paced learning you can revisit

Before you enrol

  • No prior experience needed for this course
  • Self-paced video, 217 min — watch anytime

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Course curriculum

The course is readily available, allowing learners to start and complete it at their own pace.

10 lectures3 hr 37 min
  1. Ideal Gas Equation vs Various Processes
    35 min
  2. Pdv Work or Displacement Work
    12 min
  3. Pdv Work For Various Quasistatic Process
    27 min
  4. Isothermal vs Adiabatic Curve
    6 min
  5. Polytropic Index For Various Process
    14 min
  6. Path Function & Point Function
    24 min
  7. Work Other than PdV or Displacement Work
    20 min
  8. Specific Heat & Latent Heat
    24 min
  9. PK Nag Numerical
    30 min
  10. PK Nag Numerical
    25 min

Key topics covered

  • Ideal Gas Equation vs Various Processes

  • PdV Work or Displacement Work

  • PdV Work For Various Quasistatic Processes

  • Isothermal vs Adiabatic Curve

  • Polytropic Index For Various Processes

  • Path Function And Point Function

  • Work Other than Pdv or Displacement Work

  • Specific Heat And Latent Heat

  • PK Nag Problems

Course attachments

lec-09.pdf

Lec-10.pdf

lec-11.pdf

lec-12.pdf

lec-13.pdf

lec-14.pdf

lec-15 ppt.pdf

lec-16.pdf

lec-17.pdf

lec-18.pdf

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Career opportunities

Frequently asked questions

A: The correct answer lands in the few hundred kJ/kg range, consistent with ideal-gas polytropic work using R·T and a moderate pressure ratio. Option B collapses the magnitude by confusing isothermal limits with actual polytropic behaviour. Option C over-scales linearly with pressure ratio and ignores the logarithmic/exponent relationship. Option D mixes up closed-system work with internal energy accounting.

A: The correct answer identifies shaft work as the source term that converts to internal energy when heat loss is constrained. Option B ignores insulation and assumes an external reservoir. Option C misreads the first law as enforcing equality rather than balance. Option D imports an incompressibility assumption that doesn't nullify viscous dissipation.

A: The correct answer reflects that small volume change in liquids collapses boundary work to a rounding error. Option B invents a restriction that doesn't exist in testing practice. Option C assumes ideal equipment rather than physical properties. Option D confuses accounting convenience with physical behaviour.

A: The correct answer captures direct conversion of shaft work into internal energy under adiabatic conditions. Option B confuses geometric constraint with energy balance. Option C invents a pressure response not dictated by the first law. Option D drags in second-law data that isn't required here.

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