Problem 65
Question
A venturi meter is used to measure the flow speed of a fluid in a pipe. The meter is connected between two sections of the pipc (Fig. \(14-50) ;\) the cross-scetional arca \(A\) of the entrance and exit of the meter matches the pipe's cross-sectional arca. Between the cntrance and exit, the fluid flows from the pipe with speed \(V\) and then through a narrow "throat" of cross- scetional area \(a\) with speed \(v\). A manometer connects the wider portion of the meter to the narrower portion. The change in the fluid's specd is accompanied by a change \(\Delta p\) in the fluid's pressure, which causes a height difference \(h\) of the liquid in the two arms of the manomcter. (Here \(\Delta p\) means pressure in the throat minus pressurc in the pipe.) (a) By applying Bernoulli's equation and the equation of continuity to points 1 and 2 in Fig. \(14-50,\) show that $$ V=\sqrt{\frac{2 a^{2} \Delta p}{\rho\left(a^{2}-A^{2}\right)}} $$ where \(\rho\) is the density of the fluid. (b) Suppose that the fluid is fresh water, that the cross-scctional arcas are \(64 \mathrm{~cm}^{2}\) in the pipe and \(32 \mathrm{~cm}^{2}\) in the throat, and that the pressure is \(55 \mathrm{kPa}\) in the pipe and \(41 \mathrm{kPa}\) in the throat. What is the rate of water flow in cubic meters per second?
Step-by-Step Solution
VerifiedKey Concepts
Venturi Meter
The meter is designed with a gradually narrowing section called the throat. As fluid enters the Venturi meter, it first moves through a wider section. Then, it passes through the throat where the cross-sectional area is much smaller. Because of this difference in area:
- Fluid speed increases at the throat.
- Pressure decreases at the throat compared to the wider section.
Overall, Venturi meters are crucial in industries where accurate fluid measurements are necessary, such as in water supply systems and various industrial processes.
Equation of Continuity
Mathematically, this is expressed as:\[ AV = av \]where:
- \( A \) is the cross-sectional area of the entrance or exit.
- \( V \) is the fluid speed at these points.
- \( a \) is the cross-sectional area at the narrower throat of the Venturi meter.
- \( v \) is the fluid speed at the throat.
The equation of continuity thus helps us relate the area and velocity, enabling calculations around flow dynamics in more complex systems.
Fluid Dynamics
In essence, Bernoulli's equation relates the velocity, pressure, and potential energy per unit volume of a fluid at two points along a streamline. The equation can be written as:\[ p_1 + \frac{1}{2} \rho V^2 + \rho gh_1 = p_2 + \frac{1}{2} \rho v^2 + \rho gh_2 \]Here:
- \( p \) represents the pressure at a point.
- \( V \) and \( v \) are fluid velocities at two points.
- \( \rho \) is the fluid density.
- \( gh \) refers to the gravitational potential energy term, which can be cancelled out for horizontal flow.
Fluid dynamics enables us to understand phenomena like lift in aircraft wings, ocean currents, and blood flow in arteries, making it indispensable in both theoretical research and practical applications.