Warning: foreach() argument must be of type array|object, bool given in /var/www/html/web/app/themes/studypress-core-theme/template-parts/header/mobile-offcanvas.php on line 20

A water pipe narrows from a radius of \(r_{1}=5.00 \mathrm{~cm}\) to a radius of \(r_{2}=2.00 \mathrm{~cm} .\) If the speed of the water in the wider part of the pipe is \(2.00 \mathrm{~m} / \mathrm{s},\) what is the speed of the water in the narrower part?

Short Answer

Expert verified
Answer: The water flow velocity in the narrower section of the pipe is 25.00 m/s.

Step by step solution

01

Identify the known information

We are given: - Radius of the wider pipe section, \(r_1=5.00\) cm - Radius of the narrower pipe section, \(r_2=2.00\) cm - Water flow velocity in the wider pipe section, \(v_1=2.00\) m/s
02

Understand the principle of continuity

Since the water is incompressible, the principle of continuity states that the mass flow rate is constant at any cross-sectional area of the pipe. The mass flow rate is defined as the product of the cross-sectional area, the velocity, and the density (\(\rho\)) of the fluid: \(m_1 = m_2\) (mass flow rate is conserved) Hence, \(A_1v_1 \rho = A_2v_2 \rho\) As the water's density is constant, the expression reduces to: \(A_1v_1 = A_2v_2\)
03

Calculate the cross-sectional areas of the sections

The cross-sectional area of a pipe is determined by finding the area of the circular section. For a pipe with radius r, this is given by the formula: \(A = \pi r^2\) So, for both sections of the pipe, we find the areas: \(A_1= \pi r_1^2\) and \(A_2= \pi r_2^2\)
04

Apply the principle of continuity to find the water velocity in the narrow section

Now, we need to find the water flow velocity in the narrower section of the pipe (\(v_2\)). We can do this by applying the principle of continuity. Using the expression \(A_1v_1 = A_2v_2\) and knowing the areas computed in step 3, we get: \(A_1v_1 = A_2v_2\) Substitute the known values into the equation: \((\pi (5.00\mathrm{~cm})^2)(2.00 \mathrm{~m/s}) = (\pi (2.00\mathrm{~cm})^2)(v_2)\) Divide both sides of the equation by \(\pi (2.00\mathrm{~cm})^2\) to solve for \(v_2\) and remember to convert cm to m (1 cm = 0.01 m): \(v_2 = \frac{(\pi (0.050\mathrm{~m})^2)(2.00 \mathrm{~m/s})}{(\pi (0.020\mathrm{~m})^2)}\)
05

Calculate the water flow velocity in the narrow section

Perform the calculations: \(v_2 = \frac{(\pi (0.050\mathrm{~m})^2)(2.00 \mathrm{~m/s})}{(\pi (0.020\mathrm{~m})^2)} = 25.00 \mathrm{~m/s}\) The water flow velocity in the narrower part of the pipe is 25.00 m/s.

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 Vaia!

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

A basketball of circumference \(75.5 \mathrm{~cm}\) and mass \(598 \mathrm{~g}\) is forced to the bottom of a swimming pool and then released. After initially accelerating upward, it rises at a constant velocity. a) Calculate the buoyant force on the basketball. b) Calculate the drag force the basketball experiences while it is moving upward at constant velocity.

An open-topped tank completely filled with water has a release valve near its bottom. The valve is \(1.0 \mathrm{~m}\) below the water surface. Water is released from the valve to power a turbine, which generates electricity. The area of the ton of the tank \(A_{1}\) is 10 times the cross sectional area, \(A_{y}\) of the valve opening. Calculate the speed of the water as it exits the valve. Neglect friction and viscosity. In addition, calculate the speed of a drop of water released from rest at \(h=1.0 \mathrm{~m}\) when it reaches the elevation of the valve Compare the two speeds.

Brass weights are used to weigh an aluminum object on an analytical balance. The weighing is done one time in dry air and another time in humid air. What should the mass of the object be to produce a noticeable difference in the balance readings, provided the balance's sensitivity is \(m_{0}=0.100 \mathrm{mg} ?\) (The density of aluminum is \(\rho_{\mathrm{A}}=2.70 \cdot 10^{3} \mathrm{~kg} / \mathrm{m}^{3}\); the density of brass is \(\rho_{11}=8.50 \cdot 10^{3} \mathrm{~kg} / \mathrm{m}^{3}\), The density of the dry air is \(1.2285 \mathrm{~kg} / \mathrm{m}^{3}\), and the density of the humid air is \(1.2273 \mathrm{~kg} / \mathrm{m}^{3}\).).

An approximately round tendon that has an average diameter of \(3.5 \mathrm{~mm}\) and is \(15 \mathrm{~cm}\) long is found to stretch \(0.37 \mathrm{~mm}\) when acted on by a force of \(13.4 \mathrm{~N}\). Calculate Young's modulus for the tendon.

You have two identical silver spheres and two unknown fluids, A and B. You place one sphere in fluid \(A\), and it sinks; you place the other sphere in fluid \(B\), and it floats. What can you conclude about the buoyant force of fluid A versus that of fluid \(B\) ?

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.

Sign-up for free