concept

internal energy

Internal energy is the total energy contained within a system due to its microscopic motions and interactions.
3 related articles · 6 formulas · 2 who worked here

Description

Internal energy U is the total energy of chaotic (thermal) motion of microparticles of a system and the potential energy of their interaction. Unlike the mechanical energy of a body as a whole, internal energy does not depend on the body's speed or position in space, but is determined by its temperature, volume, and chemical composition. The first law of thermodynamics relates the change in internal energy (ΔU) to the amount of heat transferred (Q) and work done on the system (W): ΔU = Q - W.

History

The idea that heat is related to particle motion dates back to the work of Benjamin Thompson (Count Rumford) at the end of the 18th century, but quantitative description began in the 19th century. James Joule in 1843 experimentally proved the equivalence of mechanical work and heat. Rudolf Clausius introduced the concept of internal energy in 1850, formulating the first law of thermodynamics. Ludwig Boltzmann developed a statistical interpretation, linking internal energy to the microscopic motion of particles. James Clerk Maxwell and others developed the kinetic theory of gases, which gave an explicit form of the dependence of internal energy on temperature.

How it works

The change in internal energy of a system occurs according to the first law of thermodynamics: ΔU = Q - W, where Q is heat transferred to the system, W is work done by the system on the external environment. For an ideal gas, internal energy increases with temperature: faster-moving molecules have greater kinetic energy. During phase transitions (melting, vaporization), energy is spent on overcoming intermolecular forces, not on increasing temperature — this is how latent heat arises. In the thermodynamics of non-equilibrium processes, the local change in internal energy is described by the heat conduction equation. Closely related concepts: entropy (measure of disorder), enthalpy (U + pV), free energy. Laws: first law of thermodynamics, second law of thermodynamics (establishing the direction of processes).

In practice

Understanding internal energy makes it possible to efficiently convert heat into work in engines and refrigeration units, as well as to predict chemical reactions and phase transitions.

Fun fact

Even ice at subzero temperature has internal energy: water molecules in the crystal lattice continue to vibrate, and only at absolute zero (−273.15 °C) does this motion theoretically cease.

Concept graph →

Formulas

$$Q = \frac{E_{\text{out}}}{E_{\text{in}}}$$
Energy efficiency is the ratio of useful energy output to energy input.
What is in the formula
Qvariableenergy efficiency (dimensionless ratio) — energy efficiency
E_outvariableuseful energy output — energy joule
E_invariableenergy input — energy joule
q=\frac{e_{{out}}}{e_{{in}}} · 2605.26432
$$E_k = \frac{1}{2} m v^2$$
Kinetic energy equals one-half mass times velocity squared.
What is in the formula
E_kvariablekinetic energy — energy joule
mvariablemass — mass kilogram
vvariablevelocity — velocity metre per second
δ_{\max,a}=\frac{1}{2}μ_av_{\max}^2 · 2606.05299v1
e_{{specific}}=\frac{1}{2}v^2 · 2607.00202
$$f( ext{mix}) = rac{ ext{component A}}{N_A} ext{ln} ext{component A} + rac{ ext{component B}}{N_B} ext{ln} ext{component B} + ext{interaction term}$$
Describes the free energy of mixing for polymer solutions.
What is in the formula
f(mix)variableFree energy of mixing per lattice site — free energy density joule per cubic metre
component AvariableVolume fraction of component A — volume fraction
component BvariableVolume fraction of component B — volume fraction
N_AvariableDegree of polymerization of component A — degree of polymerization
N_BvariableDegree of polymerization of component B — degree of polymerization
interaction termvariableInteraction contribution (typically χ φ_A φ_B)
lnoperatorComputes the natural logarithm of the argument — natural logarithm
f(φ)=\frac{φ}{n_a}\logφ+\frac{1-φ}{n_b}\log(1-φ)+χφ(1-φ) · 2606.31786
$$E_{\text{ads}} = E_{\text{system}} - (E_{\text{surface}} + E_{\text{adsorbate}})$$
Energy released when a molecule adsorbs on a surface.
What is in the formula
E_{\text{ads}}variableAdsorption energy — energy joule
E_{\text{system}}variableTotal energy of the system with adsorbate — energy joule
E_{\text{surface}}variableEnergy of the clean surface — energy joule
E_{\text{adsorbate}}variableEnergy of the isolated adsorbate — energy joule
e_{{ads}}=e_{{system}}-(e_{{surface}}+e_{{molecule}}) · 2607.05321
$$E_{\text{rot}} = \frac{1}{2} I \Omega^2$$
Energy due to rotation depends on moment of inertia and angular velocity.
What is in the formula
E_rotvariablerotational kinetic energy — energy joule
Ivariablemoment of inertia — moment of inertia kilogram metre squared
Ωvariableangular velocity — angular velocity radian per second
e_{{rot}}=\frac{1}{2}km_{\star}r_{\star}^2ω_{\star}^2 · 2607.07781
$$dU = \delta Q - \delta W$$
Change in internal energy equals heat added minus work done.
What is in the formula
dUvariableInfinitesimal change in internal energy — internal energy joule
δQvariableInfinitesimal heat added to the system — heat joule
δWvariableInfinitesimal work done by the system — work joule
doperatorExact differential of a state function — exact differential
δoperatorInexact differential for path-dependent quantities — inexact differential

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