← Back to Physics Formulas

Thermodynamics Formulas

Complete collection of thermodynamics formulas with detailed explanations, notation meanings, units, and real-world applications. Master heat, work, and energy.

🔥
🔥

Gas Laws

Ideal Gas Law

PV=nRTPV = nRT

Pressure times volume equals number of moles times gas constant times temperature.

Notation:

PP:Pressure
VV:Volume
nn:Number of moles
RR:Universal gas constant
TT:Temperature (Kelvin)

Units:

PP:Pascal (Pa) or atm
VV:m³ or L
nn:mol
RR:8.314 J/(mol·K)
TT:Kelvin (K)

Applications:

  • •Gas behavior prediction
  • •Chemical reactions
  • •Industrial processes

Limitations:

Ideal gases only, low pressure

Boyle's Law

P1V1=P2V2P_1V_1 = P_2V_2

At constant temperature, pressure and volume are inversely proportional.

Notation:

P1,P2P_1, P_2:Initial and final pressure
V1,V2V_1, V_2:Initial and final volume

Units:

P1,P2P_1, P_2:Pa or atm
V1,V2V_1, V_2:m³ or L

Applications:

  • •Scuba diving
  • •Pneumatic systems
  • •Gas storage

Limitations:

Constant temperature, ideal gas

Charles's Law

V1T1=V2T2\frac{V_1}{T_1} = \frac{V_2}{T_2}

At constant pressure, volume and temperature are directly proportional.

Notation:

V1,V2V_1, V_2:Initial and final volume
T1,T2T_1, T_2:Initial and final temperature

Units:

V1,V2V_1, V_2:m³ or L
T1,T2T_1, T_2:K

Applications:

  • •Hot air balloons
  • •Thermal expansion
  • •Temperature measurement

Limitations:

Constant pressure, ideal gas

⚖️

Laws of Thermodynamics

First Law of Thermodynamics

ΔU=Q−W\Delta U = Q - W

Change in internal energy equals heat added minus work done by the system.

Notation:

ΔU\Delta U:Change in internal energy
QQ:Heat added to system
WW:Work done by system

Units:

ΔU\Delta U:Joule (J)
QQ:J
WW:J

Applications:

  • •Heat engines
  • •Refrigeration
  • •Energy conservation

Limitations:

Closed system

Second Law of Thermodynamics

ΔS≥QT\Delta S \geq \frac{Q}{T}

Change in entropy is greater than or equal to heat divided by temperature.

Notation:

ΔS\Delta S:Change in entropy
QQ:Heat transfer
TT:Temperature

Units:

ΔS\Delta S:J/K
QQ:J
TT:K

Applications:

  • •Heat engine efficiency
  • •Spontaneous processes
  • •Entropy calculations

Limitations:

Reversible processes (equality)

Third Law of Thermodynamics

S→0 as T→0S \rightarrow 0 \text{ as } T \rightarrow 0

Entropy approaches zero as temperature approaches absolute zero.

Notation:

SS:Entropy
TT:Temperature

Units:

SS:J/K
TT:K

Applications:

  • •Absolute zero studies
  • •Perfect crystal entropy
  • •Quantum systems

Limitations:

Perfect crystals only

🌡️

Heat Transfer

Conduction

Q=kAΔTLtQ = kA\frac{\Delta T}{L}t

Heat transferred by conduction equals thermal conductivity times area times temperature difference divided by length times time.

Notation:

QQ:Heat transferred
kk:Thermal conductivity
AA:Cross-sectional area
ΔT\Delta T:Temperature difference
LL:Length
tt:Time

Units:

QQ:J
kk:W/(m·K)
AA:m²
ΔT\Delta T:K
LL:m
tt:s

Applications:

  • •Building insulation
  • •Heat exchangers
  • •Thermal management

Limitations:

Steady state, uniform material

Convection

Q=hA(ΔT)tQ = hA(\Delta T)t

Heat transferred by convection equals convective heat transfer coefficient times area times temperature difference times time.

Notation:

QQ:Heat transferred
hh:Convective heat transfer coefficient
AA:Surface area
ΔT\Delta T:Temperature difference
tt:Time

Units:

QQ:J
hh:W/(m²·K)
AA:m²
ΔT\Delta T:K
tt:s

Applications:

  • •Cooling systems
  • •Heating systems
  • •Natural convection

Limitations:

Constant coefficient

Radiation

Q=σεAT4tQ = \sigma\varepsilon AT^4t

Heat transferred by radiation equals Stefan-Boltzmann constant times emissivity times area times temperature to fourth power times time.

Notation:

QQ:Heat transferred
σ\sigma:Stefan-Boltzmann constant
ε\varepsilon:Emissivity
AA:Surface area
TT:Temperature
tt:Time

Units:

QQ:J
σ\sigma:5.67 × 10⁻⁸ W/(m²·K⁴)
ε\varepsilon:dimensionless
AA:m²
TT:K
tt:s

Applications:

  • •Solar radiation
  • •Infrared heating
  • •Thermal imaging

Limitations:

Black body approximation

🌀

Entropy and Disorder

Entropy Change

ΔS=QrevT\Delta S = \frac{Q_{\text{rev}}}{T}

Change in entropy equals reversible heat transfer divided by temperature.

Notation:

ΔS\Delta S:Change in entropy
QrevQ_{\text{rev}}:Reversible heat transfer
TT:Temperature

Units:

ΔS\Delta S:J/K
QrevQ_{\text{rev}}:J
TT:K

Applications:

  • •Phase transitions
  • •Chemical reactions
  • •Thermodynamic cycles

Limitations:

Reversible processes only

Statistical Entropy

S=kBln⁡WS = k_B \ln W

Entropy equals Boltzmann constant times natural logarithm of number of microstates.

Notation:

SS:Entropy
kBk_B:Boltzmann constant
WW:Number of microstates

Units:

SS:J/K
kBk_B:1.381 × 10⁻²³ J/K
WW:dimensionless

Applications:

  • •Statistical mechanics
  • •Quantum systems
  • •Information theory

Limitations:

Equilibrium systems

Entropy of Mixing

ΔSmix=−R(n1ln⁡x1+n2ln⁡x2)\Delta S_{\text{mix}} = -R(n_1\ln x_1 + n_2\ln x_2)

Entropy change of mixing equals negative gas constant times sum of moles times natural log of mole fractions.

Notation:

ΔSmix\Delta S_{\text{mix}}:Entropy change of mixing
RR:Gas constant
n1,n2n_1, n_2:Number of moles
x1,x2x_1, x_2:Mole fractions

Units:

ΔSmix\Delta S_{\text{mix}}:J/K
RR:8.314 J/(mol·K)
n1,n2n_1, n_2:mol
x1,x2x_1, x_2:dimensionless

Applications:

  • •Solution thermodynamics
  • •Chemical mixing
  • •Phase separation

Limitations:

Ideal solutions

⚙️

Heat Engines and Cycles

Carnot Efficiency

η=1−TcTh\eta = 1 - \frac{T_c}{T_h}

Maximum efficiency equals one minus cold temperature divided by hot temperature.

Notation:

η\eta:Efficiency
TcT_c:Cold reservoir temperature
ThT_h:Hot reservoir temperature

Units:

η\eta:dimensionless
Tc,ThT_c, T_h:K

Applications:

  • •Power plants
  • •Refrigeration
  • •Heat pumps

Limitations:

Reversible Carnot cycle

Work Done by Heat Engine

W=Qh−QcW = Q_h - Q_c

Work done equals heat absorbed from hot reservoir minus heat rejected to cold reservoir.

Notation:

WW:Work done
QhQ_h:Heat absorbed from hot reservoir
QcQ_c:Heat rejected to cold reservoir

Units:

WW:J
Qh,QcQ_h, Q_c:J

Applications:

  • •Steam engines
  • •Internal combustion
  • •Thermal power

Limitations:

Cyclic processes

Coefficient of Performance (Heat Pump)

COP=QhW\text{COP} = \frac{Q_h}{W}

Coefficient of performance equals heat delivered divided by work input.

Notation:

COP\text{COP}:Coefficient of performance
QhQ_h:Heat delivered
WW:Work input

Units:

COP\text{COP}:dimensionless
Qh,WQ_h, W:J

Applications:

  • •Heat pumps
  • •Air conditioning
  • •Refrigeration

Limitations:

Reversible processes

Practice Problems

  • 📝Calculate pressure of 2 mol gas at 300K in 5L container
  • 📝Find efficiency of Carnot engine between 500K and 300K
  • 📝Calculate heat transfer through 2m² wall with 10K difference

Study Tips

  • 💡Always use Kelvin for temperature
  • 💡Pay attention to sign conventions
  • 💡Remember entropy always increases