Skip to main content
Speclore

Equilibrium

Reference data and engineering information about equilibrium for statics applications.

equilibrium

Overview

Engineering reference data for Equilibrium in statics.

Key Formulas

Equilibrium

F=0,M=0\sum F = 0, \quad \sum M = 0

Sum of forces and moments equals zero for a body in equilibrium.

Stress

σ=FA\sigma = \frac{F}{A}

Force per unit area.

Moment

M=FdM = F \cdot d

Force × perpendicular distance.

Variables

SymbolDescriptionUnit
FFForceN
AAArea
MMMomentN·m
ddDistancem

Comparative Analysis of Equilibrium States

The following table summarizes the defining conditions for common equilibrium states.

5 rows
Comparison of different equilibrium states, their defining conditions, and key quantitative measures.
Equilibrium Type
System Description
Condition for Equilibrium
Key Quantitative Measure
MechanicalRigid bodiesNo relative acceleration$sum ec{F} = 0$, $sum ec{ au} = 0$
ThermalThermodynamic systems in contactNo net heat flow$T_1 = T_2$
ElectrostaticConductorsNo net charge flow (current)$V_1 = V_2$ (electric potential)
PhaseSubstance in multiple phasesNo net phase transformationChemical potential $mu_{alpha} = mu_{eta}$
ChemicalReactive mixtureNo net change in compositionReaction Gibbs energy $Delta_r G = 0$

Source: Engineering Principles

Detailed Equplanations

Mechanical Equilibrium

A system is in mechanical equilibrium when the vector sum of all forces and torques acting on it is zero. This ensures no translational or rotational acceleration. Key Formula:

iFi=0andiτi=0\sum_{i} \vec{F}_i = 0 \quad \text{and} \quad \sum_{i} \vec{\tau}_i = 0

Thermal Equilibrium

Two systems are in thermal equilibrium when they are in diathermal contact (allowing heat exchange) and no net energy flows between them. This is the basis for the Zeroth Law of Thermodynamics and defines temperature. Key Formula:

TA=TBT_A = T_B

where TAT_A and TBT_B are the absolute temperatures of the systems.

Electrostatic Equilibrium

Conductors reach electrostatic equilibrium when their charges have redistributed such that the internal electric field is zero, and no net current flows. Key Conditions:

  1. The electric field E\vec{E} inside the conductor is zero.
  2. Any net charge resides entirely on the surface.
  3. The electric field just outside the surface is perpendicular to the surface.
  4. The conductor is an equipotential volume (V=constantV = \text{constant}).

Phase Equilibrium

For a pure substance, phases (e.g., solid, liquid, gas) coexist in equilibrium when the chemical potential (μ\mu) of the substance is identical in each phase. For a phase transition like vaporization, this leads to the Clausius-Clapeyron equation relating vapor pressure to temperature. Key Formula (Clausius-Clapeyron):

dPdT=ΔtrsSΔtrsV=ΔtrsHTΔtrsV\frac{dP}{dT} = \frac{\Delta_{trs} S}{\Delta_{trs} V} = \frac{\Delta_{trs} H}{T \Delta_{trs} V}

Chemical Equilibrium

A closed system reaches chemical equilibrium when the forward and reverse reaction rates are equal, resulting in no net change in the concentrations of reactants and products. It is characterized by the reaction quotient QQ reaching the equilibrium constant KK. Key Formula (Equilibrium Constant):

ΔrG=ΔrG+RTlnQ\Delta_r G = \Delta_r G^\circ + RT \ln Q

At equilibrium (ΔrG=0\Delta_r G = 0, Q=KQ = K):

ΔrG=RTlnK\Delta_r G^\circ = -RT \ln K

References