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Homework 7 – Problem 1 Solution 
Part (a) 
Dimensionless Group 
Definition Symbols 
Reynolds Ratio of the inertia and viscous forces 
Nusselt Ratio of convection to pure conduction 
heat transfer (f=fluid) 
Prandtl Ratio of the momentum and thermal 
diffusivities 
Part (b) 
Laminar flow is typically characterized as a visually even flow profile, similar to a slow-moving 
stream and has a parabolic velocity profile for the case of a pipe. Turbulent flow is characterized 
as a more violent flow regime with more dimensions being considered than with laminar flow; 
think of white-water rapids and the like versus the slow-moving stream. For plate flow, laminar 
flow exists from a Reynolds number of 0 to ~500,000. The value 500,000 is called the critical 
Reynolds number and anything above this is termed as turbulent and have already gone through 
the transition flow regime. For pipe flow, laminar flow exists for Reynolds numbers from 0 to 
~2,000, the transition phase is in the range of 2,000 to 4,000, and turbulent flow is deemed 
anything above 4,000. 
Part (c) 
Case Temperature 
i Flow over a flat plate Film Temp: 
ii Flow around a cylinder (Hilpert relation) Film Temp: 
iii Flow around a cylinder (Zukauskas relation) 
iv Flow around a cylinder (Churchill and Bernstein relation) Film Temp: 
v Flow around a sphere (Whitaker relation) 
vi Flow through a bank of tubes (Grimison relation) Film Temp: 
vii Flow through a bank of tubes (Zukauskas relation) Arithmetic mean of fluid 
inlet and outlet temperatures
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CH EN 3453 Heat Transfer 2014 Fall Utah Homework HW 07 Solutions
CH EN 3453 Heat Transfer 2014 Fall Utah Homework HW 07 Solutions
CH EN 3453 Heat Transfer 2014 Fall Utah Homework HW 07 Solutions
CH EN 3453 Heat Transfer 2014 Fall Utah Homework HW 07 Solutions

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CH EN 3453 Heat Transfer 2014 Fall Utah Homework HW 07 Solutions

  • 1. Homework 7 – Problem 1 Solution Part (a) Dimensionless Group Definition Symbols Reynolds Ratio of the inertia and viscous forces Nusselt Ratio of convection to pure conduction heat transfer (f=fluid) Prandtl Ratio of the momentum and thermal diffusivities Part (b) Laminar flow is typically characterized as a visually even flow profile, similar to a slow-moving stream and has a parabolic velocity profile for the case of a pipe. Turbulent flow is characterized as a more violent flow regime with more dimensions being considered than with laminar flow; think of white-water rapids and the like versus the slow-moving stream. For plate flow, laminar flow exists from a Reynolds number of 0 to ~500,000. The value 500,000 is called the critical Reynolds number and anything above this is termed as turbulent and have already gone through the transition flow regime. For pipe flow, laminar flow exists for Reynolds numbers from 0 to ~2,000, the transition phase is in the range of 2,000 to 4,000, and turbulent flow is deemed anything above 4,000. Part (c) Case Temperature i Flow over a flat plate Film Temp: ii Flow around a cylinder (Hilpert relation) Film Temp: iii Flow around a cylinder (Zukauskas relation) iv Flow around a cylinder (Churchill and Bernstein relation) Film Temp: v Flow around a sphere (Whitaker relation) vi Flow through a bank of tubes (Grimison relation) Film Temp: vii Flow through a bank of tubes (Zukauskas relation) Arithmetic mean of fluid inlet and outlet temperatures
  • 2. Excerpts from this work may be reproduced by instructors for distribution on a not-for-profit basis for testing or instructional purposes only to students enrolled in courses for which the textbook has been adopted. Any other reproduction or translation of this work beyond that permitted by Sections 107 or 108 of the 1976 United States Copyright Act without the permission of the copyright owner is unlawful.
  • 3. Excerpts from this work may be reproduced by instructors for distribution on a not-for-profit basis for testing or instructional purposes only to students enrolled in courses for which the textbook has been adopted. Any other reproduction or translation of this work beyond that permitted by Sections 107 or 108 of the 1976 United States Copyright Act without the permission of the copyright owner is unlawful.
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