mechanical

Thermal Management: Conduction, Convection, and Heat Exchanger Design

From Fourier's conduction law to convective heat transfer coefficients and heat exchanger sizing, this guide covers practical thermal engineering for machines and electronics.

12 min read · Systems: Thermal Systems · Electronics Cooling · Heat Exchangers
Thermal bridge thermal image showing heat conduction paths
Infrared thermography reveals heat conduction paths — understanding thermal resistance networks is key to managing heat flow.Wikimedia Commons, public domain

Conduction and thermal resistance

Fourier's law: q = −kA(dT/dx). Thermal resistance R = L/(kA) lets engineers treat heat flow like electrical current through a circuit.

  • Series resistances add; parallel resistances reduce (like electrical circuits).
  • High-conductivity materials (copper 400 W/m·K, aluminium 200 W/m·K) minimize resistance.
  • Thermal interface materials reduce contact resistance at joint surfaces.

Convection and heat transfer coefficients

Newton's law of cooling: Q = hA(Ts − T∞). The convective coefficient h depends on geometry, fluid, and flow regime.

  • Natural convection: h = 5–25 W/m²·K (air); forced convection: h = 25–250 W/m²·K.
  • Use dimensionless Nusselt, Reynolds, and Prandtl numbers for correlation-based design.
  • Fins increase effective area; optimize fin pitch with the efficiency ηf.

Heat exchanger sizing with LMTD

The log mean temperature difference method relates exchanger area to heat duty and overall transfer coefficient: Q = U·A·LMTD.

  • Counterflow configuration gives higher LMTD than parallel flow for the same terminal temperatures.
  • Overall U combines wall conduction and both convective resistances.
  • Add 20–30% area margin for fouling allowance in process industry applications.

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