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Heat Diffusion and Boundary Conditions

Jun 11, 2025

Overview

This lecture focused on the heat diffusion equation for conduction, methods to simplify it under different conditions, types of boundary conditions, and a sample problem applying energy conservation and heat transfer concepts.

Heat Diffusion Equation & Its Simplification

  • The heat diffusion equation governs conduction heat transfer in solids and accounts for heat generation, spatial variation, and temporal change.
  • In Cartesian coordinates: α(∂²T/∂x² + ∂²T/∂y² + ∂²T/∂z²) + q̇/k = ∂T/∂t, where α is thermal diffusivity.
  • For steady-state with no heat generation, the equation reduces to ∂²T/∂x² = 0.
  • The equation also applies to cylindrical and spherical coordinates with adjustments for geometry.

Boundary and Initial Conditions

  • Solving the equation requires boundary conditions (two each for x, y, z) and one initial condition for time-dependent problems.
  • Four main types of boundary conditions:
    • Known surface temperature (Dirichlet condition): T at surface is specified.
    • Known surface heat flux (Neumann condition): q'' = -k ∂T/∂x at surface.
    • Adiabatic or insulated boundary: ∂T/∂x = 0, as no heat crosses the surface.
    • Convective/mixed boundary: -k ∂T/∂x at surface = h(T_s - T_∞)._

Newton’s Law of Cooling and Convective Boundaries

  • Convective heat transfer is described by Newton’s law of cooling: q_conv = hA(T_s - T_∞).
  • The convective heat transfer coefficient (h) depends on fluid velocity, properties, and surface geometry.
  • h is often a function of Reynolds and Prandtl numbers._

Problem-Solving Approach

  • Identify coordinate system and governing equation based on geometry and physics.
  • Simplify the equation according to the scenario (steady/unsteady, with/without generation).
  • Select appropriate boundary/initial conditions (Dirichlet, Neumann, Adiabatic, Mixed).
  • Solve for temperature profile and heat flux; use conservation of energy for storage calculations.

Example Problem Recap

  • Wall with internal heat generation, known polynomial temperature profile, and material properties provided.
  • Tasks: Find heat entering/exiting at boundaries, rate of energy stored, and time rate of temperature change at specific locations.
  • Solutions used the derivative of the temperature profile, Fourier’s law, and energy balance.

Key Terms & Definitions

  • Heat Diffusion Equation — Governing PDE describing conduction with possible heat generation and time dependence.
  • Thermal Diffusivity (α) — k/(ρc_p), measures rate of temperature spread.
  • Boundary Condition — Constraint applied at the edge of the domain (e.g., specified T, heat flux, insulation).
  • Newton’s Law of Cooling — q = hA(T_s - T_∞), empirical law for convective heat transfer.
  • Convective Heat Transfer Coefficient (h) — Parameter quantifying convective heat transfer efficiency._

Action Items / Next Steps

  • Practice solving the given example problem on boundary conditions and energy conservation.
  • Review textbook sections on boundary/initial conditions for conduction problems.
  • Prepare to discuss modifications of the heat diffusion equation for various coordinate systems in next class.