Problem 5: Dimensional Analysis Use the Buckingham Pi Theorem (Song, 2018, pages 219-221) to derive an equation for friction head loss, hr, as a function of gravitational acceleration, g, pipe diameter, D, pipe length, L, and average velocity, V=Q/A. Step 1-List the dimensional parameters (N, n₁, n₂, ...). Step 2-List the dimensions of all parameters in terms of primary dimensions. Step 3-Select a set of primary dimensions (MLT or FLT). Step 4-Select a set of repeating parameters. Step 5-Set up one or more dimensional equations in the form N= n*n2n3², then solve for the unknown exponents.

Structural Analysis
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ISBN:9781337630931
Author:KASSIMALI, Aslam.
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**Problem 5: Dimensional Analysis**

Use the Buckingham Pi Theorem (Song, 2018, pages 219-221) to derive an equation for friction head loss, \( h_r \), as a function of gravitational acceleration, \( g \), pipe diameter, \( D \), pipe length, \( L \), and average velocity, \( V = Q/A \).

**Step 1**—List the dimensional parameters \((N, n_1, n_2, \ldots)\).

**Step 2**—List the dimensions of all parameters in terms of primary dimensions.

**Step 3**—Select a set of primary dimensions (MLT or FLT).

**Step 4**—Select a set of repeating parameters.

**Step 5**—Set up one or more dimensional equations in the form \( N = \Pi n_1^{x_1}n_2^{x_2}n_3^{x_3} \), then solve for the unknown exponents.
Transcribed Image Text:**Problem 5: Dimensional Analysis** Use the Buckingham Pi Theorem (Song, 2018, pages 219-221) to derive an equation for friction head loss, \( h_r \), as a function of gravitational acceleration, \( g \), pipe diameter, \( D \), pipe length, \( L \), and average velocity, \( V = Q/A \). **Step 1**—List the dimensional parameters \((N, n_1, n_2, \ldots)\). **Step 2**—List the dimensions of all parameters in terms of primary dimensions. **Step 3**—Select a set of primary dimensions (MLT or FLT). **Step 4**—Select a set of repeating parameters. **Step 5**—Set up one or more dimensional equations in the form \( N = \Pi n_1^{x_1}n_2^{x_2}n_3^{x_3} \), then solve for the unknown exponents.
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