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One-dimensional heat conduction equation with constant coefficients

1 ONE-DIMENSIONAL HEAT CONDUCTION EQUATION WITH CONSTANT COEFFICIENTS [Pg.299]

In this section we consider the one-dimensional heat conduction equation with constant coefficients and difference schemes in order to develop various methods for designing the appropriate difference schemes in the case of time-dependent problems. [Pg.299]

Marcel Dekker, Inc. 270 Madison Avenue, New York, New York 10016 [Pg.299]

The original problem. The heat diffusion process on a straight line is described by the heat conduction equation [Pg.300]

Indeed, by introducing x = x/a and denoting once again x by x we obtain (3). Where searching a solution to equation (2) on the segment 0 x I, it is sensible to pass to the dimensionless variables [Pg.300]

We concentrate primarily on the first boundary-value problem associated with equation- (3) in the rectangle D = 0 i l,0 T, in which it is required to find a continuous in D solution u = u(x,t) of the [Pg.300]


One-dimensional heat conduction equation with constant coefficients... [Pg.21]

Small-scale experiments w ere conducted with ambient temperature CO2 [ ], and an experimental run-time coefficient was determined. This coefficient is based on the one-dimensional steady-state heat conduction equation with constant material properties ... [Pg.469]

One-Dimensional Conduction Lumped and Distributed Analysis The one-dimensional transient conduction equations in rectangular (b = 1), cylindrical (b = 2), and spherical (b = 3) coordinates, with constant k, initial uniform temperature 7), S = 0, and convection at the surface with heat-transfer coefficient h and fluid temperature 77, are... [Pg.6]

Transient heat conduction or mass transfer in solids with constant physical properties (diffusion coefficient, thermal diffusivity, thermal conductivity, etc.) is usually represented by a linear parabolic partial differential equation. Steady state heat or mass transfer in solids, potential distribution in electrochemical cells is usually represented by elliptic partial differential equations. In this chapter, we describe how one can arrive at the analytical solutions for linear parabolic partial differential equations and elliptic partial differential equations in finite domains using a separation of variables method. The methodology is illustrated using a transient one dimensional heat conduction in a rectangle. [Pg.587]

Starting with an energy balance on a disk volume ele -ment, derive the one-dimensional transient implicit finite difference equation for a general interior node for r(z, /) in a cylinder whose side surface is subjected (o convection with a conveclioD coefficient of h and an ambient temperature of for the case of constant thermal conductivity with uniform heat generation. [Pg.368]


See other pages where One-dimensional heat conduction equation with constant coefficients is mentioned: [Pg.138]    [Pg.144]    [Pg.265]    [Pg.356]    [Pg.144]   


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