The pressure drop in a long, uniform length of pipe is a function of fluid density, mean velocity in the pipe, the diameter of the pipe, viscosity, the length of the pipe, and the equivalent sand grain roughness (units of length) of the pipe. The equation is shown below. Develop the dimensional matrix using M (mass), L (length), and T (time) for this phenomenon, and determine its rank. Ap = f(p.V.D.µ.L.ɛ)

Structural Analysis
6th Edition
ISBN:9781337630931
Author:KASSIMALI, Aslam.
Publisher:KASSIMALI, Aslam.
Chapter2: Loads On Structures
Section: Chapter Questions
Problem 1P
icon
Related questions
Question
The pressure drop in a long, uniform length of pipe is a function of fluid density, mean velocity in the pipe, the diameter of the pipe, viscosity, the length of the pipe, and the equivalent sand grain roughness (units of length) of the pipe. The equation is shown below. Develop the dimensional matrix using M (mass), L (length), and T (time) for this phenomenon, and determine its rank.

\[ \Delta p = f \left( \rho, \overrightarrow{V}, D, \mu, L, \varepsilon \right) \] 

Here, \(\Delta p\) represents the pressure drop, \(\rho\) is the fluid density, \(\overrightarrow{V}\) is the mean velocity in the pipe, \(D\) is the diameter of the pipe, \(\mu\) is the viscosity, \(L\) is the length of the pipe, and \(\varepsilon\) is the equivalent sand grain roughness.
Transcribed Image Text:The pressure drop in a long, uniform length of pipe is a function of fluid density, mean velocity in the pipe, the diameter of the pipe, viscosity, the length of the pipe, and the equivalent sand grain roughness (units of length) of the pipe. The equation is shown below. Develop the dimensional matrix using M (mass), L (length), and T (time) for this phenomenon, and determine its rank. \[ \Delta p = f \left( \rho, \overrightarrow{V}, D, \mu, L, \varepsilon \right) \] Here, \(\Delta p\) represents the pressure drop, \(\rho\) is the fluid density, \(\overrightarrow{V}\) is the mean velocity in the pipe, \(D\) is the diameter of the pipe, \(\mu\) is the viscosity, \(L\) is the length of the pipe, and \(\varepsilon\) is the equivalent sand grain roughness.
Expert Solution
Step 1: Introduction:

To develop the dimensional matrix for the given phenomenon, we can use the Buckingham π theorem, which states that if you have

  • 'n' variables and
  • 'k' fundamental dimensions
  • 'n - k' dimensionless π (Pi) groups.

 In this case,

  • 6 variables (Δp, ρ, V, D, μ, L, ε) 
  • 3 fundamental dimensions (M, L, T).

So, we have:

  • n = 6 variables (Δp, ρ, V, D, μ, L, ε)
  • k = 3 fundamental dimensions (M, L, T)
steps

Step by step

Solved in 3 steps

Blurred answer
Knowledge Booster
Pressurized pipe flow
Learn more about
Need a deep-dive on the concept behind this application? Look no further. Learn more about this topic, civil-engineering and related others by exploring similar questions and additional content below.
Recommended textbooks for you
Structural Analysis
Structural Analysis
Civil Engineering
ISBN:
9781337630931
Author:
KASSIMALI, Aslam.
Publisher:
Cengage,
Structural Analysis (10th Edition)
Structural Analysis (10th Edition)
Civil Engineering
ISBN:
9780134610672
Author:
Russell C. Hibbeler
Publisher:
PEARSON
Principles of Foundation Engineering (MindTap Cou…
Principles of Foundation Engineering (MindTap Cou…
Civil Engineering
ISBN:
9781337705028
Author:
Braja M. Das, Nagaratnam Sivakugan
Publisher:
Cengage Learning
Fundamentals of Structural Analysis
Fundamentals of Structural Analysis
Civil Engineering
ISBN:
9780073398006
Author:
Kenneth M. Leet Emeritus, Chia-Ming Uang, Joel Lanning
Publisher:
McGraw-Hill Education
Sustainable Energy
Sustainable Energy
Civil Engineering
ISBN:
9781337551663
Author:
DUNLAP, Richard A.
Publisher:
Cengage,
Traffic and Highway Engineering
Traffic and Highway Engineering
Civil Engineering
ISBN:
9781305156241
Author:
Garber, Nicholas J.
Publisher:
Cengage Learning