8.4 Moving Fluids and Bernoulli's Equation
The motion or flow of a fluid is a complex phenomenon, which
in principle can be analyzed in terms of Newtonian Mechanics, as applied to
a system of particles.
Two types of flow of fluids can be characterized. They are
the streamlined flow and the turbulent flow.
The flow of water in naturally occurring streams is an example
of steadystreamlined flow whereas the flow of water in rapids or waterfalls
is the turbulent flow.
The mechanics of fluid in the turbulent flow is beyond the
scope of this book; only some aspects of the steadystreamlined flow based on
the principles of conservation of mass and energy will be discussed here.
The steadystream lined flow is characterized by stream lines and tubes of
stream lines. When a nonviscous fluid flows through a certain region of space
such that at a given point the velocity of all fluid particles that flow past
that point is same at all times (though at different points the velocity of
fluid may be different but again it will be independent of time), then such
a flow is called the steady  stream lined flow.
The line (curve) connecting such points is called a stream line. Stream lines
have the following properties:
i) Only one stream line can pass through any point.
ii) A tangent at any point to the stream line represents the path of motion
of a fluid particle passing through that point.
The diagram above represents a stream line. Any particle at P will
have the same velocity V and will follow the same path from P to
Q. Also particles that arrive at Q will have same velocity V at
all times.
Tube of Flow
Consider any area of Crosssection A in a fluid in a steady flow. Consider
the stream lines of flow from each point on the boundary of crosssection, these
stream lines enclose a tube; such a tube is called a tube of flow. The properties
of tubes of flow are:
i) Fluid in different tubes cannot mix with each other.
ii) The same fluid particles will keep on moving through a given tube of flow.
Equation of Continuity
The conservation of the mass of fluid in a tube of flow, immediately results
into the equation of continuity.
Consider the steady  Stream lined flow of a non viscous fluid; consider a
tube of flow of such a fluid in motion as shown. Let P and Q be two points and
let A_{1} and A_{2} be areas of crosssections of the tube of flow normal to the velocities
v_{1} and v_{2} respectively at P and Q.
[next page]
