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Heat Capacity

Reference data and engineering information about heat capacity for thermodynamics applications.

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Overview

Engineering reference data for Heat Capacity in thermodynamics.

Key Formulas

First Law

ΔU=QW\Delta U = Q - W

Energy is conserved — heat added minus work done.

Ideal Gas Law

PV=nRTPV = nRT

Relates pressure, volume, and temperature of an ideal gas.

Heat Transfer

Q=mcΔTQ = mc\Delta T

Sensible heat transfer.

Carnot Efficiency

η=1TC/TH\eta = 1 - T_C/T_H

Maximum efficiency between two temperatures.

Variables

SymbolDescriptionUnit
UUInternal energyJ
QQHeatJ
WWWorkJ
PPPressurePa
VVVolume
TTTemperatureK

Specific Heat for Gases

For vapors and gases, there are two distinct definitions of specific heat:

  • Specific heat at constant pressure: cp=(hT)pc_p = \left(\frac{\partial h}{\partial T}\right)_p
  • Specific heat at constant volume: cv=(hT)vc_v = \left(\frac{\partial h}{\partial T}\right)_v

Note: For solids and liquids, cpcvc_p \approx c_v because these substances are nearly incompressible.

Gas Constant and Specific Heat Ratio

The individual gas constant RR relates the two specific heats:

R=cpcvR = c_p - c_v

The ratio of specific heats (also called the adiabatic index or isentropic expansion factor) is:

k=cpcvk = \frac{c_p}{c_v}

This ratio is critical in thermodynamic processes involving ideal gases, particularly in adiabatic expansions and compressions.

Molar Heat Capacity

Molar heat capacity (CpC_p) is the amount of heat required to raise the temperature of one mole of a substance by one degree at constant pressure.

PropertySymbolUnits
Molar heat capacityCpC_pJ/(mol·K)

Example: The molar heat capacity of iron is 25.10 J/(mol·K), meaning it takes 25.10 J of heat to raise 1 mol of iron by 1 K.

Converting Between Specific and Molar Heat Capacity

cp=CpMandCp=cpMc_p = \frac{C_p}{M} \qquad \text{and} \qquad C_p = c_p \cdot M

where MM is the molar mass of the substance (g/mol).

Example — Methanol (CH₃OH):

Given: Cp=81.1C_p = 81.1 J/(mol·K)

Molar mass: M=12.01+4(1.008)+16.00=32.04M = 12.01 + 4(1.008) + 16.00 = 32.04 g/mol

cp=81.132.04=2.53 J/(g⋅K)c_p = \frac{81.1}{32.04} = 2.53 \text{ J/(g·K)}

Unit Conversion Reference

ConversionValue
1 Btu/(lb·°F)4186.8 J/(kg·K)
1 Btu/(lb·°F)1 kcal/(kg·°C)
1 kJ/(kg·°C)0.239 Btu/(lb·°F)

Practical Examples

Heating Aluminum

Calculate the heat required to heat 2 kg of aluminum from 20 °C to 100 °C.

Given:

  • Mass: m=2m = 2 kg
  • Specific heat: c=0.91c = 0.91 kJ/(kg·°C)
  • Temperature change: ΔT=10020=80\Delta T = 100 - 20 = 80 °C

Q=mcΔT=(2)(0.91)(80)=145.6 kJQ = m \cdot c \cdot \Delta T = (2)(0.91)(80) = 145.6 \text{ kJ}

Heating Water

Calculate the energy required to heat 1 liter of water from 0 °C to 100 °C.

Given:

  • Volume: 1 L (mass = 1 kg, since density of water ≈ 1 kg/L)
  • Specific heat: c=4.19c = 4.19 kJ/(kg·°C)
  • Temperature change: ΔT=1000=100\Delta T = 100 - 0 = 100 °C

Q=(1)(4.19)(100)=419 kJQ = (1)(4.19)(100) = 419 \text{ kJ}

Converting to kilowatt-hours:

Q=419 kJ×13600 h/s=0.116 kWhQ = 419 \text{ kJ} \times \frac{1}{3600} \text{ h/s} = 0.116 \text{ kWh}

Engineering Insight: The high specific heat of water (4.19 kJ/kg·°C) compared to most metals makes it an excellent medium for thermal energy storage systems.

References