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The velocity profile in fully developed laminar flow in a circular pipe of inner radius \(R=10 \mathrm{~cm}\), in \(\mathrm{m} / \mathrm{s}\), is given by \(u(r)=4\left(1-r^{2} / R^{2}\right)\). Determine the mean and maximum velocities in the pipe, and the volume flow rate.

Short Answer

Expert verified
Answer: The maximum velocity is 4 m/s, the mean velocity is 2π m/s, and the volume flow rate is 0.02π² m³/s.

Step by step solution

01

Convert Units

First, we need to convert the radius of the pipe (in cm) to meters: \(R = 10 \mathrm{~cm} \times \frac{1 \mathrm{~m}}{100 \mathrm{~cm}} = 0.1 \mathrm{~m}\).
02

Find the Maximum Velocity

Since the velocity profile contains no variable other than \(r\), we can find the maximum velocity by setting \(r=0\) (at the center of the pipe, where velocity is highest): \(u_{max} = u(0) = 4(1 - \frac{0^2}{0.1^2}) = 4 \mathrm{~m/s}\).
03

Determine the Mean Velocity

We can find the mean velocity by averaging the velocity profile over the cross-sectional area of the pipe. The mean velocity is given by: \(u_{mean} = \frac{1}{A}\int_{0}^{R} u(r)2 \pi r \mathrm{d}r\), where \(A = \pi R^2\) is the cross-sectional area of the pipe.
04

Calculate the Mean Velocity

Now we can plug in the values we know and perform the integration: \(u_{mean} = \frac{1}{\pi (0.1)^2}\int_{0}^{0.1} 4\left(1 - \frac{r^2}{0.1^2}\right)2 \pi r \mathrm{d}r\), \(u_{mean} = \frac{1}{0.01\pi}\int_{0}^{0.1} 8\pi r - \frac{8\pi r^3}{0.01} \mathrm{d}r\), \(u_{mean} = 100 \pi \left[ 4\pi r^2 - \frac{2\pi r^4}{0.01} \right]^0.1_0\), \(u_{mean} = 100 \pi \left( 4\pi (0.1)^2 - \frac{2\pi (0.1)^4}{0.01} \right) = 100 \pi (0.004\pi - 0.002\pi) = 2 \pi \mathrm{~m/s}\).
05

Calculate the Volume Flow Rate

The volume flow rate is the product of the mean velocity and the cross-sectional area of the pipe: \(Q = u_{mean} \times A = 2 \pi \times 0.01\pi = 0.02\pi^2 \mathrm{~m^3/s}\). In summary, the maximum velocity in the pipe is \(u_{max} = 4 \mathrm{~m/s}\), the mean velocity is \(u_{mean} = 2 \pi \mathrm{~m/s}\), and the volume flow rate is \(Q = 0.02\pi^2 \mathrm{~m^3/s}\).

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Velocity Profile
The concept of a velocity profile is fundamental when analyzing fluid flow, especially in the context of laminar flow inside a circular pipe.
The velocity profile describes how the fluid velocity varies across the cross-section of the pipe, from the center to the edge.
In the exercise given, the velocity profile is represented by the equation \(u(r) = 4 \left(1 - \frac{r^2}{R^2}\right)\).
  • Here, \(u(r)\) is the velocity at a distance \(r\) from the center of the pipe.
  • \(R\) is the radius of the pipe, and in the given problem, it is 0.1 meters.
  • The profile illustrates that fluid velocity is highest at the center \((u(0) = u_{max})\) and decreases towards the pipe walls, reaching zero at the surface.
This type of parabolic velocity profile is characteristic of laminar flow, where the streamlined flow causes layers of fluid to slide past one another without mixing.
Mean Velocity
Mean velocity is an average flow velocity across a pipe’s cross-section, providing a single-speed equivalent for varying velocities throughout the pipe.
It considers the velocity variations at different radial positions from the center.
The mean velocity \(u_{mean}\) can be determined using the formula:\[u_{mean} = \frac{1}{A} \int_{0}^{R} u(r) \, 2 \pi r \, dr\]
  • \(A = \pi R^2\) is the cross-sectional area.
  • The integration runs from the center \(r=0\) to the edge of the pipe \(r=R\).
Substituting the problem values, we calculated the mean velocity as \(2 \pi \mathrm{~m/s}\).
It's essential in understanding fluid mechanics because knowing \(u_{mean}\) helps quantify overall flow characteristics and helps in engineering applications such as pipeline design.
Volume Flow Rate
The volume flow rate, often represented by \(Q\), measures how much fluid volume passes a given cross-section of the pipe per unit time.
It's crucial for determining the efficiency and effectiveness of fluid transport systems.
To find the flow rate, multiply the mean velocity by the pipe's cross-sectional area:\[Q = u_{mean} \times A\]
  • In the problem, this calculates to \(Q = 2 \pi \times 0.01 \pi = 0.02 \pi^2 \mathrm{~m^3/s}\).
  • The unit \(\mathrm{m^3/s}\) implies this is a volumetric measure, suitable for various practical applications, from water pipelines to oil shipment.
Understanding volume flow rates helps engineers and designers ensure that pipelines convey the right amount of fluid, balancing efficiency and cost.
Circular Pipe
A circular pipe is a common conduit used in transporting fluids due to its symmetrical shape, which facilitates uniform flow characteristics.
A key focus in fluid dynamics, especially when considering laminar flow, is how this symmetry affects the velocity distribution and hence the flow efficiency.
  • The radius of a circular pipe \(R\) is vital for calculating other parameters, such as flow rate and mean velocity.
  • In our problem, the radius was 0.1 meters after conversion, impacting various calculations.
  • Circular pipes are preferred because they have fewer materials and installation costs and are naturally strong against pressure due to their geometry.
Understanding the role of a circular pipe helps in predicting how fluids behave under different conditions, ensuring optimal design and function in numerous engineering applications.

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Most popular questions from this chapter

Water \(\left(\mu=9.0 \times 10^{-4} \mathrm{~kg} / \mathrm{m} \cdot \mathrm{s}, \rho=1000 \mathrm{~kg} / \mathrm{m}^{3}\right)\) enters a 2-cm- diameter and 3-m-long tube whose walls are maintained at \(100^{\circ} \mathrm{C}\). The water enters this tube with a bulk temperature of \(25^{\circ} \mathrm{C}\) and a volume flow rate of \(3 \mathrm{~m}^{3} / \mathrm{h}\). The Reynolds number for this internal flow is (a) 59,000 (b) 105,000 (d) 236,000 (e) 342,000 (c) 178,000

Cooling water available at \(10^{\circ} \mathrm{C}\) is used to condense steam at \(30^{\circ} \mathrm{C}\) in the condenser of a power plant at a rate of \(0.15 \mathrm{~kg} / \mathrm{s}\) by circulating the cooling water through a bank of 5 -m-long \(1.2-\mathrm{cm}\)-internal-diameter thin copper tubes. Water enters the tubes at a mean velocity of \(4 \mathrm{~m} / \mathrm{s}\) and leaves at a temperature of \(24^{\circ} \mathrm{C}\). The tubes are nearly isothermal at \(30^{\circ} \mathrm{C}\). Determine the average heat transfer coefficient between the water, the tubes, and the number of tubes needed to achieve the indicated heat transfer rate in the condenser.

Water enter a 5-mm-diameter and 13-m-long tube at \(45^{\circ} \mathrm{C}\) with a velocity of \(0.3 \mathrm{~m} / \mathrm{s}\). The tube is maintained at a constant temperature of \(5^{\circ} \mathrm{C}\). The required length of the tube in order for the water to exit the tube at \(25^{\circ} \mathrm{C}\) is (a) \(1.55 \mathrm{~m}\) (b) \(1.72 \mathrm{~m}\) (c) \(1.99 \mathrm{~m}\) (d) \(2.37 \mathrm{~m}\) (e) \(2.96 \mathrm{~m}\) (For water, use \(k=0.623 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K}, \operatorname{Pr}=4.83, v=0.724 \times\) \(10^{-6} \mathrm{~m}^{2} / \mathrm{s}, c_{p}=4178 \mathrm{~J} / \mathrm{kg} \cdot \mathrm{K}, \rho=994 \mathrm{~kg} / \mathrm{m}^{3}\).)

A computer cooled by a fan contains eight printed circuit boards (PCBs), each dissipating \(10 \mathrm{~W}\) of power. The height of the PCBs is \(12 \mathrm{~cm}\) and the length is \(18 \mathrm{~cm}\). The clearance between the tips of the components on the \(P C B\) and the back surface of the adjacent \(P C B\) is \(0.3 \mathrm{~cm}\). The cooling air is supplied by a 10 -W fan mounted at the inlet. If the temperature rise of air as it flows through the case of the computer is not to exceed \(10^{\circ} \mathrm{C}\), determine (a) the flow rate of the air that the fan needs to deliver, \((b)\) the fraction of the temperature rise of air that is due to the heat generated by the fan and its motor, and ( \(c\) ) the highest allowable inlet air temperature if the surface temperature of the components is not to exceed \(70^{\circ} \mathrm{C}\) anywhere in the system. As a first approximation, assume flow is fully developed in the channel. Evaluate properties of air at a bulk mean temperature of \(25^{\circ} \mathrm{C}\). Is this a good assumption?

Air is flowing through a smooth thin-walled 4-indiameter copper tube that is submerged in water. The water maintains a constant temperature of \(60^{\circ} \mathrm{F}\) and a convection heat transfer coefficient of \(176 \mathrm{Btu} / \mathrm{h}-\mathrm{ft}^{2} \cdot \mathrm{R}\). If air (1 atm) enters the copper tube at a mean temperature of \(90^{\circ} \mathrm{F}\) with an average velocity of \(8 \mathrm{ft} / \mathrm{s}\), determine the necessary copper tube length so that the outlet mean temperature of the air is \(70^{\circ} \mathrm{F}\).

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