Physical Significance of Stream Funtion
ψ
Figure 10.1 illustrates a two dimensional
flow.
Fig 10.1 Physical
Interpretation of Stream Function
Let A be a fixed point, whereas P be
any point in the plane of the flow. The points A and P are
joined by the arbitrary lines ABP and ACP.
For an incompressible steady flow, the volume flow rate across
ABP into the space ABPCA (considering a unit width in a direction
perpendicular to the plane of the flow) must be equal to that
across ACP. A number of different paths connecting A and P
(ADP, AEP,...) may be imagined but the volume flow rate across
all the paths would be the same. This implies that the
rate of flow across any curve between A and P depends only
on the end points A and P.
Since A is fixed,
the rate of flow across ABP, ACP, ADP, AEP (any path connecting
A and P) is a function only of the position P. This function
is known as the stream
function ψ.
The value of ψ
at P represents the volume flow rate across any line joining
P to A.
The value of ψ at A is made arbitrarily zero. If a point
P’ is considered (Fig. 10.1b),PP’ being along a
streamline, then the rate of flow across the curve joining
A to P’ must be the same as across AP, since, by the
definition of a streamline, there is no flow across PP'
The value of ψ thus
remains same at P’ and P. Since P’ was taken as
any point on the streamline through P, it follows that ψ
is constant along a streamline. Thus the flow may be represented
by a series of streamlines at equal increments of ψ.
In fig (10.1c) moving from A to B net flow
going past the curve AB is
The stream function, in
a polar coordinate system is defined as
The expressions for Vr
and Vθ in terms of the stream function automatically
satisfy the equation of continuity given by
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