FLUID MECHANICS FUNDAMENTALS+APPS
FLUID MECHANICS FUNDAMENTALS+APPS
4th Edition
ISBN: 9781259877766
Author: CENGEL
Publisher: MCG
bartleby

Concept explainers

bartleby

Videos

Question
Book Icon
Chapter 10, Problem 19P
To determine

The velocities with actual form of stocks theorem and compare with actual determined value.

Expert Solution & Answer
Check Mark

Answer to Problem 19P

The theoretical velocities for all different cases are 3.121mm/s, 12.12mm/s and 55.56mm/s. The difference between experimental and theoretical velocities for all three cases are 0.079mm/s, 0.68mm/s and 4.84mm/s.

Explanation of Solution

Given information:

Actual stokes law is FD=3πμDV+(9π/16)ρV2D2. Three aluminum balls of diameters 2mm, 4mm and 10mm.

Concept used:

For constant velocity of ball under glycerin, the relation for summation of forces on the ball is expressed as follows:

  FD+FB=W...... (1)

Here, drag force is FD, Buoyant force is FB, Weight of the ball is W.

Calculation:

Substitute 3πμDV+(9π/16)ρV2D2 for FD, ρalg×πD36 for W and ρglg×πD36 for FB in equation (1).

  3πμDV+(9π/16)ρV2D2+ρglg×πD36=ρalg×πD36( 9π 16ρ glD)V2+3μV+D2g6(ρ glρ al)=0

For first case:

Substitute 2mm for D, 1260Kg/m3 for ρgl, 2700Kg/m3 for ρal and 1Kg-m/s for μ in above equation.

  ( 9π 16×1260×( 2mm)( 1m 1000mm ))V2+3×1×V+ ( ( 2mm )( 1m 1000mm ) )2×9.816(12602700)=04.4532V2+3V0.0094176=0

On solving quadratic equation, the value of V are 0.003121m/s and 0.6768m/s. Velocity cannot negative for this case. So, the theoretical velocity for 2mm diameter ball is 0.003121m/s or 3.121mm/s.

Difference between actual and theoretical velocity is calculated as follows:

  ΔV=VexperimentalVtheoreticalΔV=3.2mm/s3.121mm/sΔV=0.079mm/s

For second case:

Substitute 4mm for D, 1260Kg/m3 for ρgl, 2700Kg/m3 for ρal and 1Kg-m/s for μ in above equation.

  ( 9π 16×1260×( 4mm)( 1m 1000mm ))V2+3×1×V+ ( ( 4mm )( 1m 1000mm ) )2×9.816(12602700)=08.9064V2+3V0.03767=0

On solving quadratic equation, the value of V are 0.01212m/s and 0.3489m/s. Velocity cannot negative for this case. So, the theoretical velocity for 4mm diameter ball is 0.01212m/s or 12.12mm/s.

Difference between actual and theoretical velocity is calculated as follows:

  ΔV=VexperimentalVtheoreticalΔV=12.8mm/s12.12mm/sΔV=0.68mm/s

For Third case:

Substitute 10mm for D, 1260Kg/m3 for ρgl, 2700Kg/m3 for ρal and 1Kg-m/s for μ in above equation.

  ( 9π 16×1260×( 10mm)( 1m 1000mm ))V2+3×1×V+ ( ( 10mm )( 1m 1000mm ) )2×9.816(12602700)=022.26V2+3V0.23544=0

On solving quadratic equation, the value of V are 0.05556m/s and 0.190339m/s. Velocity cannot negative for this case. So, the theoretical velocity for 10mm diameter ball is 0.05556m/s or 55.56mm/s.

Difference between actual and theoretical velocity is calculated as follows:

  ΔV=VexperimentalVtheoreticalΔV=60.4mm/s55.56mm/sΔV=4.84mm/s

Thus, the theoretical velocities for all different cases are 3.121mm/s, 12.12mm/s and 55.56mm/s. The difference between experimental and theoretical velocities for all three cases are 0.079mm/s, 0.68mm/s and 4.84mm/s.

Conclusion:

The theoretical velocities for all different cases are 3.121mm/s, 12.12mm/s and 55.56mm/s. The difference between experimental and theoretical velocities for all three cases are 0.079mm/s, 0.68mm/s and 4.84mm/s.

Want to see more full solutions like this?

Subscribe now to access step-by-step solutions to millions of textbook problems written by subject matter experts!
Students have asked these similar questions
In the derivationof Naurer-stokes equation, ene of the forces considered was shear stress Gnd thus the rchtion: Txy=Tyse Tyz=Tzy てx=え Prove that, Toz =
FLUID MECHANICS
. Determine the displacement gradient tensor, right Cauchy-Green deformation tensor, small deformations strain tensor, rotation tensor, and small deformations and rotations strain tensor for the following displacement fields: u={A X₁² X3, B X1 X2 X3,, C (X2 + X32)} where A, B, and C are constants.

Chapter 10 Solutions

FLUID MECHANICS FUNDAMENTALS+APPS

Ch. 10 - Prob. 11PCh. 10 - In Example 9-18 we solved the Navier-Stekes...Ch. 10 - Prob. 13PCh. 10 - A flow field is simulated by a computational fluid...Ch. 10 - In Chap. 9(Example 9-15), we generated an “exact”...Ch. 10 - Prob. 16CPCh. 10 - Prob. 17CPCh. 10 - A person drops 3 aluminum balls of diameters 2 mm,...Ch. 10 - Prob. 19PCh. 10 - Prob. 20PCh. 10 - Prob. 21PCh. 10 - Prob. 22PCh. 10 - Prob. 23PCh. 10 - Prob. 24PCh. 10 - Prob. 25PCh. 10 - Prob. 26PCh. 10 - Prob. 27PCh. 10 - Consider again the slipper-pad bearing of Prob....Ch. 10 - Consider again the slipper the slipper-pad bearing...Ch. 10 - Prob. 30PCh. 10 - Prob. 31PCh. 10 - Prob. 32PCh. 10 - Prob. 33PCh. 10 - Prob. 34EPCh. 10 - Discuss what happens when oil temperature...Ch. 10 - Prob. 36PCh. 10 - Prob. 38PCh. 10 - Prob. 39CPCh. 10 - Prob. 40CPCh. 10 - Prob. 41PCh. 10 - Prob. 42PCh. 10 - Prob. 43PCh. 10 - Prob. 44PCh. 10 - Prob. 45PCh. 10 - Prob. 46PCh. 10 - Prob. 47PCh. 10 - Prob. 48PCh. 10 - Ch. 10 - Prob. 50CPCh. 10 - Consider the flow field produced by a hair dayer...Ch. 10 - In an irrotational region of flow, the velocity...Ch. 10 - Ch. 10 - Prob. 54CPCh. 10 - Prob. 55PCh. 10 - Prob. 56PCh. 10 - Consider the following steady, two-dimensional,...Ch. 10 - Prob. 58PCh. 10 - Consider the following steady, two-dimensional,...Ch. 10 - Prob. 60PCh. 10 - Consider a steady, two-dimensional,...Ch. 10 - Ch. 10 - Prob. 63PCh. 10 - Prob. 64PCh. 10 - Prob. 65PCh. 10 - In an irrotational region of flow, we wtite the...Ch. 10 - Prob. 67PCh. 10 - Prob. 68PCh. 10 - Water at atmospheric pressure and temperature...Ch. 10 - The stream function for steady, incompressible,...Ch. 10 - Ch. 10 - We usually think of boundary layers as occurring...Ch. 10 - Prob. 73CPCh. 10 - Prob. 74CPCh. 10 - Prob. 75CPCh. 10 - Prob. 76CPCh. 10 - Prob. 77CPCh. 10 - Prob. 78CPCh. 10 - Prob. 79CPCh. 10 - Prob. 80CPCh. 10 - Prob. 81CPCh. 10 - Ch. 10 - On a hot day (T=30C) , a truck moves along the...Ch. 10 - A boat moves through water (T=40F) .18.0 mi/h. A...Ch. 10 - Air flows parallel to a speed limit sign along the...Ch. 10 - Air flows through the test section of a small wind...Ch. 10 - Prob. 87EPCh. 10 - Consider the Blasius solution for a laminar flat...Ch. 10 - Prob. 89PCh. 10 - A laminar flow wind tunnel has a test is 30cm in...Ch. 10 - Repeat the calculation of Prob. 10-90, except for...Ch. 10 - Prob. 92PCh. 10 - Prob. 93EPCh. 10 - Prob. 94EPCh. 10 - In order to avoid boundary laver interference,...Ch. 10 - The stramwise velocity component of steady,...Ch. 10 - For the linear approximation of Prob. 10-97, use...Ch. 10 - Prob. 99PCh. 10 - One dimension of a rectangular fiat place is twice...Ch. 10 - Prob. 101PCh. 10 - Prob. 102PCh. 10 - Prob. 103PCh. 10 - Static pressure P is measured at two locations...Ch. 10 - Prob. 105PCh. 10 - For each statement, choose whether the statement...Ch. 10 - Prob. 107PCh. 10 - Calculate the nine components of the viscous...Ch. 10 - In this chapter, we discuss the line vortex (Fig....Ch. 10 - Calculate the nine components of the viscous...Ch. 10 - Prob. 111PCh. 10 - The streamwise velocity component of a steady...Ch. 10 - For the sine wave approximation of Prob. 10-112,...Ch. 10 - Prob. 115PCh. 10 - Suppose the vertical pipe of prob. 10-115 is now...Ch. 10 - Which choice is not a scaling parameter used to o...Ch. 10 - Prob. 118PCh. 10 - Which dimensionless parameter does not appear m...Ch. 10 - Prob. 120PCh. 10 - Prob. 121PCh. 10 - Prob. 122PCh. 10 - Prob. 123PCh. 10 - Prob. 124PCh. 10 - Prob. 125PCh. 10 - Prob. 126PCh. 10 - Prob. 127PCh. 10 - Prob. 128PCh. 10 - Prob. 129PCh. 10 - Prob. 130PCh. 10 - Prob. 131PCh. 10 - Prob. 132PCh. 10 - Prob. 133PCh. 10 - Prob. 134PCh. 10 - Prob. 135PCh. 10 - Prob. 136PCh. 10 - Prob. 137PCh. 10 - Prob. 138P
Knowledge Booster
Background pattern image
Mechanical Engineering
Learn more about
Need a deep-dive on the concept behind this application? Look no further. Learn more about this topic, mechanical-engineering and related others by exploring similar questions and additional content below.
Similar questions
SEE MORE QUESTIONS
Recommended textbooks for you
Text book image
International Edition---engineering Mechanics: St...
Mechanical Engineering
ISBN:9781305501607
Author:Andrew Pytel And Jaan Kiusalaas
Publisher:CENGAGE L
8.01x - Lect 27 - Fluid Mechanics, Hydrostatics, Pascal's Principle, Atmosph. Pressure; Author: Lectures by Walter Lewin. They will make you ♥ Physics.;https://www.youtube.com/watch?v=O_HQklhIlwQ;License: Standard YouTube License, CC-BY
Dynamics of Fluid Flow - Introduction; Author: Tutorials Point (India) Ltd.;https://www.youtube.com/watch?v=djx9jlkYAt4;License: Standard Youtube License