Thermal Energy, Specific Heat Capacity & Thermodynamics Study Notes

Fundamental Concepts

  • Thermal / Internal Energy
    • Total microscopic energy stored in a system.
    • Sum of kinetic energy (motion of particles) + potential energy (inter-particle forces).
    • Increase in thermal energy ⇒ increase in internal energy, particle speed or separation.
  • Heat vs. Temperature
    • Heat = energy in transit due to temperature difference; measured in J\text{J}.
    • Temperature = measure of average kinetic energy of particles; unit Kelvin (K).
    • Absolute zero 0K(!!273C)0\,\text{K}\,(!!-273\,^{\circ}\text{C}): particles possess essentially no kinetic energy.
    • Conversion: T<em>(K)=T</em>(C)+273T<em>{\text{(K)}} = T</em>{\,(^{\circ}\text{C})} + 273.

Laws of Thermodynamics

  • Zeroth Law
    • If body A is in thermal equilibrium with body B, and B with C, then A and C are also in thermal equilibrium.
    • Foundation for the definition of temperature.
  • First Law (Energy Conservation for Thermodynamic Systems)
    • ΔU=Q+W\Delta U = Q + W
      ΔU\Delta U: change in internal energy.
      QQ: heat supplied to the system (positive when added).
      WW: work done by the system on surroundings (positive when done by the system in transcript convention).
  • Second Law
    • Heat flows spontaneously from higher to lower temperature objects until equilibrium is reached.
    • Implies real processes have irreversibilities (friction, sound), limiting efficiency.

Specific Heat Capacity (SHC)

  • Definition
    • Energy required to raise the temperature of 1kg1\,\text{kg} of a substance by 1C1\,^{\circ}\text{C} (or 1K1\,\text{K}) without a phase change.
  • Equation
    • Q=mcΔTQ = mc\,\Delta T
      mm: mass (kg)
      cc: specific heat capacity (Jkg1K1)(\text{Jkg}^{-1}\text{K}^{-1})
      ΔT\Delta T: temperature change (K or C^{\circ}\text{C}).
  • Value for water: cwater=4.18×103Jkg1K1c_{\text{water}} = 4.18 \times 10^{3}\,\text{Jkg}^{-1}\text{K}^{-1}.
  • Key ideas
    • Large cc ⇒ substance can ‘hold’ lots of heat with small temperature change (thermal buffering).
    • No change of state occurs during SHC processes.

Specific Latent Heat (SLH)

  • Definition
    • Energy required to change the state of 1kg1\,\text{kg} of a substance at constant temperature.
  • Types & Symbols
    • Fusion (solid ↔ liquid): LfL_f.
    • Vaporisation (liquid ↔ gas): LvL_v.
  • Equation
    • Q=mLQ = mL.
  • Units: Jkg1\text{Jkg}^{-1}.
  • Example: Steam at 100C100^{\circ}\text{C} contains more energy than water at 100C100^{\circ}\text{C} because of the latent heat of vaporisation.

Energy Transfer Mechanisms

  • Conduction: particle-to-particle transfer in solids.
  • Convection: bulk movement of fluids (liquids & gases).
  • Radiation: emission/absorption of electromagnetic waves; no particles required.

Temperature–Time Graphs

  • Flat regions ⇒ latent heat (energy in, temperature constant).
  • Sloped regions ⇒ SHC processes (temperature changes, no phase change).
  • Gradient in sloped region linked to cc; length of plateaus linked to LL.

Internal Energy & Kinetic Model Connections

  • In thermal equilibrium, two bodies share the same temperature ⇒ same average kinetic energy per particle.
  • Microscopic picture explains conduction (vibrations), convection (density changes), radiation (photon emission).

Efficiency of Machines

  • Formula
    • η=useful energyouttotal energyin×100%\eta = \dfrac{\text{useful energy\,out}}{\text{total energy\,in}} \times 100\%.
  • Sources of loss: friction, sound, electrical resistance.
  • Improvement strategies
    • Use lubricants to minimise friction.
    • Employ low-resistance wiring.
    • Reduce vibration of moving parts.
    • Streamline vehicles to cut drag.

Experimental Considerations & Mandatory Practicals

  • Determining SHC in the lab
    1. Measure mass mm of sample.
    2. Supply known electrical energy Q=IVtQ = IVt or Q=PtQ = P t.
    3. Record initial and final temperatures to get ΔT\Delta T with a calibrated probe.
    4. Compute c=QmΔTc = \dfrac{Q}{m\,\Delta T}.
    5. Plot scatter graph of QQ vs ΔT\Delta T; gradient =mc= mc.
    6. Estimate absolute & percentage uncertainties; include error bars, find gradient uncertainty.
    7. Repeat trials to obtain means & reduce random error; comment on systematic errors (heat loss to surroundings).
  • Risk assessment: hot surfaces, electrical hazards, steam burns—implement goggles, heat-resistant gloves, circuit fuses.

Key Equations & Constants (Quick Reference)

  • ΔU=Q+W\Delta U = Q + W (First Law)
  • Q=mcΔTQ = mc\,\Delta T (Specific Heat Capacity)
  • Q=mLQ = mL (Specific Latent Heat)
  • η=useful  E<em>outE</em>in×100%\eta = \dfrac{\text{useful}\;E<em>{\text{out}}}{E</em>{\text{in}}} \times 100\% (Efficiency)
  • T<em>(K)=T</em>(C)+273T<em>{\text{(K)}} = T</em>{\,(^{\circ}\text{C})} + 273 (Kelvin conversion)
  • cwater=4.18×103Jkg1K1c_{\text{water}} = 4.18 \times 10^{3}\,\text{Jkg}^{-1}\text{K}^{-1}
  • Appliances: kettles, engines—design revolves around SHC, SLH, and efficiency constraints.
  • Climate science: water’s high cc moderates Earth’s temperature.
  • Industrial processes: latent heat exploited in distillation, refrigeration.
  • Absolute zero concept underpins cryogenics & quantum research.