Understanding Internal Energy in Thermodynamics: Definition and Equations"

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SUMMARY

Internal energy (U) in thermodynamics is defined as the energy associated with the microscopic motions of molecules within a system, including translational, rotational, vibrational kinetic energies, and potential energies. The First Law of Thermodynamics is expressed as dU = dQ + dW, while the central equation is dU = TdS - PdV. Internal energy is a state function, meaning its change between two states is independent of the process taken. Specific internal energy (s.i.e) refers to internal energy per unit mass.

PREREQUISITES
  • Understanding of thermodynamic principles
  • Familiarity with the First Law of Thermodynamics
  • Knowledge of state functions in thermodynamics
  • Basic concepts of kinetic and potential energy
NEXT STEPS
  • Study the implications of the First Law of Thermodynamics in various systems
  • Explore the concept of state functions and their significance in thermodynamics
  • Learn about the relationship between internal energy and enthalpy (H = U + PV)
  • Investigate specific internal energy calculations and applications in fluid dynamics
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Students and professionals in physics and engineering, particularly those focused on thermodynamics, energy systems, and fluid mechanics.

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Definition/Summary

In thermodynamics, internal energy, U, is the energy associated with the microscopic energies of a system, that is with the energy associated with the random motion of the molecules within a system.

More generally, while external energy is energy due to macroscopic motion (of the system as a whole) or to external fields, internal energy is all other forms of energy, including random motion (relative motion of molecules within the system) and dipole moments and stress.

Equations

First Law of Thermodynamics:

dU\,=\,dQ\,+\,dW

Central Equation:

dU\,=\,TdS\,-\,PdV

Internal energy plus pressure times volume equals enthalpy:

H\ =\ U\ +\ P\,V

Extended explanation

Above we define the internal energy as the energy associated with the microscopic energies of a system, that is the energy associated with the random motion of the molecules within a system.

So for a general fluid, the internal energy of a system is the sum of the translational kinetic energies, the rotational kinetic energies, the vibrational kinetic energies and the potential energies of all the molecules in that system.

The internal energy of a system is often erroneously referred to as the heat of a system.

Path independence:

One important point to note here is that dU is an exact differential, which means that the path integral

U = \int_\gamma dU

is path independent. In other words, at each equilibrium point, U is uniquely defined, irrespective of the path taken.

More physically, the change in internal energy between two states is independent of the process through which the change of state was made. Hence, internal energy is a state function.

Specific internal energy (s.i.e):

Specific internal energy (s.i.e) is internal energy per unit mass.

* This entry is from our old Library feature. If you know who wrote it, please let us know so we can attribute a writer. Thanks!
 
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I understand that internal energy is the energy associated with the microscopic motions of molecules in a system. It includes translational kinetic energies, rotational kinetic energies, vibrational kinetic energies and potential energies. Additionally, it is a state function, which means that the change in internal energy between two states is independent of the process through which the change was made. Specific internal energy (s.i.e) is the internal energy per unit mass.
 

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