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Suppose that
is the density of some bulk fluid property (e.g., mass, momentum,
or energy) at position
and time
. In other words, suppose that, at time
, an infinitesimal fluid element of volume
, located
at position
, contains an amount
of the property in question. Note, incidentally,
that
can be either a scalar, a component of a vector, or even a component of a tensor.
The total
amount of the property contained within some fixed volume
is
|
(1.28) |
where the integral is taken over all elements of
. Let
be an outward directed
element of the bounding surface of
. Suppose that this element is located at point
. The volume of fluid that
flows per second across the element, and so out of
, is
. Thus, the
amount of the fluid property under consideration that is convected across the element per second is
. It follows that the net amount of the property that
is convected out of volume
by fluid flow across its bounding surface
is
|
(1.29) |
where the integral is taken over all outward directed elements of
. Suppose, finally, that
the property in question is created within the volume
at the rate
per second.
The conservation equation for the fluid property takes the form
|
(1.30) |
In other words, the rate of increase in the amount of the property contained within
is the
difference between the creation rate of the property inside
, and the rate at
which the property is convected out of
by fluid flow.
The previous conservation law can also be written
|
(1.31) |
Here,
is termed the flux of the property out of
, whereas
is called the net generation rate of the property within
.
Next: Mass Conservation
Up: Mathematical Models of Fluid
Previous: Viscosity
Richard Fitzpatrick
2016-03-31