Lumped Capacitance Method for Analyzing Transient Conduction Problems: Screencasts
Derives the lumped capacitance method and explores one of its major limitations.
We suggest that after watching this screencast, you list the important points as a way to increase retention.
A second introductory screencast
We suggest that after watching this screencast, you list the important points as a way to increase retention.
Important Equations:
The Biot number, \(Bi\) is a dimensionless quantity defined by this equation:
\[Bi = \frac{hL_c}{k}\]
where \(h\) = heat transfer coefficient \((W/m^2-K)\) or \((W/m^2-^{\circ} C)\),
\(L_c\) = characteristic length \((m)\), and
\(k\) = thermal conductivity \((W/m-K)\) or \((W/m-^{\circ}C)\).
The characteristic length is defined by
\[L_c = \frac{V}{A}\]
where \(V\) = volume of the object \((m^3)\), and
\(A\) = area of the object \((m^2)\).
Conservatively, the characteristic length can be the distance between the temperature extremes, such as the radius in the case of a sphere.
You must confirm that \(Bi\) < 0.1 before using the following equation, which is used to predict temperature as a function of time:
\[T = T_{\infty} + (T_i \,-\, T_{\infty})e^{-\frac{hAt}{\rho Vc}}\]
where \(T\) = temperature at time \(t \, (s)\),
\(T_{\infty}\) = temperature of the surrounding fluid,
\(T_i\) = object’s initial temperature,
\(\rho\) = object’s density \((kg/m^3)\), and
\(c\) = object’s heat capacity \((J/kg-K)\) or \((J/kg-^{\circ}C)\).