Biomedical Engineering Reference
In-Depth Information
It will be clear that, in the context of the discussion above, the following formal
relations hold for the velocity field and the acceleration field:
v = v ( x 0 , t )
and
a = a ( x 0 , t ) .
(9.6)
The configuration change of the material in a certain time interval can be asso-
ciated with deformation. We deal with deformation when the mutual distances
between material points change. The mathematical description of deformation and
deformation velocity is the major theme of Chapter 10 .
9.3 Lagrangian and Eulerian description
In the previous section the velocity and acceleration of the material are formally
written as functions of the material identification
x 0 with material coordinates
0 in V 0 and the time t . Obviously, this can also be done with other physical
properties associated with the material, for example the temperature T .Fora
(time-dependent) temperature field it can be written
T
=
T (
x 0 , t ) .
(9.7)
The temperature field in the current configuration V ( t ) is mapped on the reference
configuration. Such a description is referred to as Lagrangian . Partial differen-
tiation to time t at constant
x 0 results in the material time derivative of the
T :
temperature,
T
t
T
=
.
(9.8)
x 0 constant
This variable T has to be interpreted as the change (per unit time) of the
temperature at a material point (moving through space) identified by x 0 .
Another approach concentrates on a fixed point in three-dimensional space. At
every point in time a different material particle may be arrived at this location. For
the (time-dependent) temperature field it can be written:
T = T ( x , t ) ,
(9.9)
indicating the temperature of the material being present at time t in the spatial
point
x in V ( t ). This alternative field specification is called Eulerian . When the
partial derivative with respect to time t of the temperature field in the Eulerian
description is determined, the spatial time derivative
δ
T
t is obtained:
T
δ T
δ
t =
.
(9.10)
t
x constant
 
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