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Incompressible fluid flows steadily through a plane diverging channel, At the inlet, of height \(H,\) the flow is uniform with magnitude \(V_{1}\). At the outlet, of height \(2 H\), the velocity profile is \\[ V_{2}=V_{m} \cos \left(\frac{\pi y}{2 H}\right) \\] where \(y\) is measured from the channel centerline. Express \(V_{m}\) in terms of \(V_{1}\)

Short Answer

Expert verified
To express \(V_{m}\) in terms of \(V_{1}\), we use the principle of flow conservation for incompressible steady flow, which tells us that the mass flow rate at the inlet equals the mass flow rate at the outlet. By integrating the velocity profile at the outlet and equating it to the flow at the inlet, we solve for \(V_{m}\) in terms of \(V_{1}\).

Step by step solution

01

Identify key principles

Recognize that the flow conservation principle applies in this exercise. For incompressible steady flow, the mass flow rate at the inlet equals the mass flow rate at the outlet.
02

Calculate mass flow rate at the inlet

Calculate the mass flow rate at the inlet. Mass flow rate is given by the equation \(\rho AV\), where \(\rho\) is the fluid density, \(A\) is the cross-sectional area, and \(V\) is the velocity. Here, the velocity is \(V_{1}\) and area of the inlet is \(H\). Since the fluid is incompressible, \(\rho\) remains constant, thus the mass flow rate is proportional to \(HV_{1}\)
03

Determine expression for velocity at the outlet

At the outlet, the velocity profile \(V_{2}\) is given as \(V_{m} \cos \left(\frac{\pi y}{2 H}\right)\). The mass flow rate at the outlet must also be proportional to \(V_{1}\), so we'll integrate the velocity profile over the height of the outlet (0 to \(2H\)) to determine \(V_{m}\) in terms of \(V_{1}\).
04

Set up the integral for the outlet's velocity profile

Set up the integral from 0 to \(2H\) for the velocity profile \(V_{2}\).
05

Solve the integral and equate to the inlet flow

Evaluate the integral and get the result in terms of \(V_{m}\). Next, set up the expression from step 2 equal to the result of the integral to isolate \(V_{m}\) in terms of \(V_{1}\).
06

Solve for \(V_{m}\)

Solve the equation for \(V_{m}\) in terms of \(V_{1}\). This will give us the relationship between the maximum velocity at the outlet and the uniform velocity at the inlet of the channel.

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