Transient Conduction through a Plane Wall

Requires a Wolfram Notebook System
Interact on desktop, mobile and cloud with the free Wolfram Player or other Wolfram Language products.
A plane wall of thickness is initially at uniform temperature. At time
, its surface is exposed to a liquid at a different temperature. The centerline temperature (at
) is plotted as a function of time on the left, and the temperature distribution as a function of location is plotted on the right; it varies in time.
Contributed by: Rachel Saker and Rachael L. Baumann (February 2017)
Additional contributions by: John L. Falconer
(University of Colorado Boulder, Department of Chemical and Biological Engineering)
Open content licensed under CC BY-NC-SA
Snapshots
Details
Lumped capacitance is a quick method for determining the temperature within an object, such as the plane wall considered here. This method assumes a uniform temperature at any point within the solid (regardless of proximity to the surface) and therefore is only reliable for Biot number . The Biot number is
,
where is the convective heat transfer coefficient (
),
is the thermal conductivity (
) of the material, and
is the cross-sectional length of the wall (m). The lumped capacitance method, which assumes a uniform temperature distribution through the wall, is only a function of the wall thickness
and not a function of position within the wall. The temperature as a function of time is calculated using the lumped capacitance method from the ratio of the temperature differences:
,
,
where is temperature (K), the subscripts
and
denote the initial and ambient temperatures, and
is the Fourier number (dimensionless):
,
,
where is thermal diffusivity (
),
is time (
),
is density (
) and
is heat capacity (
).
When , uniform temperature in the solid is not a valid assumption, and thus the lumped capacitance method is not accurate. Instead, the one-term approximation models the temperature distribution with better accuracy, and is valid for
:
,
,
where is the position within the solid (
),
is dimensionless, and
and
are constants that can be found in Table 5.1 on p. 301 of [1].
Reference
[1] T. L. Bergman, A. S. Lavine, F. P. Incropera and D. P. DeWitt, Introduction to Heat Transfer, 6th ed., Hoboken, NJ: John Wiley and Sons, 2011.
Permanent Citation