/*! This file is auto-generated */ .wp-block-button__link{color:#fff;background-color:#32373c;border-radius:9999px;box-shadow:none;text-decoration:none;padding:calc(.667em + 2px) calc(1.333em + 2px);font-size:1.125em}.wp-block-file__button{background:#32373c;color:#fff;text-decoration:none} Problem 37 A prototype water pump has a spe... [FREE SOLUTION] | 91Ó°ÊÓ

91Ó°ÊÓ

A prototype water pump has a specific speed of \(1.2,\) and when operating at its most efficient state, it delivers \(5 \mathrm{~L} / \mathrm{s}\) with an added head of \(10 \mathrm{~m}\). Operation of the pump is to be tested using a \(\frac{1}{5}-\) scale model with various test fluids that have dynamic viscosities in the range of \(5-10\) times that of water. Viscous effects should be accurately accounted for in the model. What range of rotational speeds, flow rates, and heads will be required in model testing? Assess whether accurately accounting for viscous effects is realistic.

Short Answer

Expert verified
The model flow rate is approximately 0.45 L/s and head is 2 m; accounting for full-scale viscous effects may not be realistic.

Step by step solution

01

Understanding Viscous Effects

The problem involves evaluating the pump's performance under various operating conditions by accounting for changes in fluid viscosity. To assess viscous effects, we'll use the dimensionless specific speed, which stays constant between the model and the prototype when scaled correctly. We need to estimate the new conditions required for the scaled model given the viscosity changes.
02

Determine Scale in Model

Since the model is a \( \frac{1}{5} \) scale of the prototype, the model size is smaller but the dimensionless parameters remain the same. Hence, the flow rate \( Q_m \) of the model can be derived from its relationship to scale factor \( n \) and prototype flow rate \( Q \) as \( Q_m = n^{3/2} \cdot Q \).
03

Calculate Model Flow Rate

Using the scaling factor \( n = \frac{1}{5} \), compute the model flow rate \( Q_m \) as \[ Q_m = \left(\frac{1}{5}\right)^{3/2} \times 5 \, \text{L/s} = \frac{5}{\sqrt{125}} \, \text{L/s} \approx 0.45 \, \text{L/s}. \]
04

Determine Scaled Head

For head, the model head \( H_m \) can be calculated as \( H_m = n \cdot H \), simplifying to \[ H_m = \frac{1}{5} \times 10 \, \text{m} = 2 \, \text{m}. \]
05

Estimating Viscous Scale Effect on Rotational Speed

Viscosity affects the viscous Reynolds number \( Re_v \), and equivalency is maintained by adjusting rotational speed. Keep \( Re = rac{\rho ND^2}{\mu} \) and \( Re_v = C_v \frac{ND^2}{u} = C_v \frac{ND\mu}{\rho} \) constant. Adjust \( N_m \) using estimated change in \( u \) or calculate the necessary scale to counter viscosity sufficiency.
06

Evaluate Realism of Viscous Effects

For practical testing, consider whether a framework exists to replicate dynamic viscosity range changes (5-10 times of water) and test results under these conditions. Full fidelity in capturing viscosity may not be realistic within limited model testability contexts.

Unlock Step-by-Step Solutions & Ace Your Exams!

  • Full Textbook Solutions

    Get detailed explanations and key concepts

  • Unlimited Al creation

    Al flashcards, explanations, exams and more...

  • Ads-free access

    To over 500 millions flashcards

  • Money-back guarantee

    We refund you if you fail your exam.

Over 30 million students worldwide already upgrade their learning with 91Ó°ÊÓ!

Key Concepts

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

Viscous Effects
Understanding viscous effects is crucial in fluid mechanics. In our problem, viscous effects refer to how fluid flow is impacted by its viscosity, or resistance to flow. When fluid viscosities change, such as the range of 5-10 times that of water mentioned, this can significantly affect the pump's operation. The viscosity affects the internal friction of the fluid, which in turn affects the efficiency and performance of the pump. Higher viscosity means higher friction, leading to a potential decrease in flow rate and added head. For model testing, accurately accounting for these viscous effects involves selecting test fluids that approximate the conditions of the prototype but adjusted for the different scale.
Scaled Model Testing
In scaled model testing, we create a smaller version of our prototype to conduct experiments that mimic real-world conditions. This method allows us to predict prototype performance without building the full-sized machine, which can save time and resources. The scaled model for this exercise is at a 1/5 scale, meaning the dimensions and certain operating conditions, like flow rate and head, are proportionally reduced. However, the goal is to keep the results dimensionless such that they can be directly correlated back to the prototype. The scale factor affects parameters such as flow rate, which is scaled by a factor of \( n^{3/2} \), and head, which is scaled by \( n \). This adjustment ensures that the results from the model are relevant to the actual size of the pump.
Specific Speed
Specific speed is a dimensionless parameter that helps in understanding the performance of a pump under similar operating conditions. It provides a correlation between the flow rate, head, and rotational speed of a pump. In this context, it remains constant between the model and the prototype when the scales are correctly applied, ensuring consistency in performance evaluation across different system sizes. With a specific speed value given as 1.2 for the prototype, it acts as a baseline to which the model's performance is compared. By keeping the specific speed consistent, we can adjust other parameters in the model (like rotational speed) to explore how changes in viscosity impact the overall system.
Dimensional Analysis
Dimensional analysis is a mathematical technique used in fluid mechanics to simplify complex systems by reducing the number of physical quantities under consideration. It helps in identifying key dimensionless numbers that govern the system's behavior, like the Reynolds number and the specific speed. For our scaled pump model, dimensional analysis is employed to maintain similarity between the modeled and real-world scenarios under different conditions, like varying fluid viscosity. Through this analysis, we can derive relations such as \( Q_m = n^{3/2} \cdot Q \) and \( H_m = n \cdot H \), assuring the dimensionless quantities like Reynolds number remain constant between the scaled model and prototype, despite the change in physical scale.

One App. One Place for Learning.

All the tools & learning materials you need for study success - in one app.

Get started for free

Most popular questions from this chapter

Water is pumped from a lower reservoir to a higher reservoir. The water surface in the higher reservoir is \(10 \mathrm{~m}\) above the water surface in the lower reservoir. The piping system consists of 200 -mm-diameter ductile iron pipe with a length of \(2 \mathrm{~km}\) and minor losses equal to 6.2 times the velocity head. The pump characteristics are shown in Table 8.3. (a) Determine the expected flow rate through the system, assuming fully turbulent flow. (b) What is the power of the motor required to drive the pump? $$ \begin{array}{l|c|c|c|c|c|c} \text { Discharge (L/s) } & 0 & 10 & 20 & 30 & 40 & 50 \\ \hline \text { Total head (m) } & 25 & 23.2 & 20.8 & 17.0 & 12.4 & 7.3 \\ \hline \text { Efficiency (\%) } & -1 & 45 & 65 & 71 & 65 & 45 \end{array} $$

A proposed turbine is being designed to generate a power of \(30 \mathrm{MW},\) with a generator rotational speed of \(150 \mathrm{rpm}\) and an available head of \(22 \mathrm{~m}\). A model of the turbine is to be tested in the laboratory, where the available head is \(6 \mathrm{~m}\), the power is \(45 \mathrm{~kW},\) and the model turbine is expected to have a hydraulic efficiency of \(95 \%\). What length scale, rotational speed, and flow rate should be used in the model tests? Assume water at \(20^{\circ} \mathrm{C}\).

A large centrifugal fan generates a flow of \(7 \mathrm{~m}^{3} / \mathrm{s}\) with a motor speed of \(1140 \mathrm{rpm}\). A smaller geometrically similar fan has a motor speed of \(1725 \mathrm{rpm}\), operates at the same efficiency as the larger fan, and generates the same pressure increase. What flow rate is generated by the smaller fan?

Show that if the effective head on a Pelton wheel is \(h_{\mathrm{e}}\), the velocity coefficient of the nozzle is \(C_{\mathrm{v}}\), and the bucket speed of the wheel is \(U\), then the theoretical maximum efficiency is attained by the Pelton when $$ U=\frac{1}{2} C_{\mathrm{v}} \sqrt{2 g h_{\mathrm{e}}} $$

Nine pump units are placed in parallel at a pump station. Each unit has a power demand of \(40 \mathrm{~kW}\) and adds \(35 \mathrm{~m}\) of head under optimal conditions. The best efficiency of each unit is \(60 \%\). The liquid being pumped is water at \(20^{\circ} \mathrm{C}\). When all units are operating under optimal conditions, what is the flow rate delivered by the pump station?

See all solutions

Recommended explanations on Physics Textbooks

View all explanations

What do you think about this solution?

We value your feedback to improve our textbook solutions.

Study anywhere. Anytime. Across all devices.