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It is known from engineering analysis that for a liquid flowing upward in a vertical pipe, the gauge pressure, \(p\), in the a pipe at a height \(z\) above the liquid surface in the source reservoir is given by $$p=-\gamma\left(1+0.24 \frac{Q^{2}}{g D^{5}}\right) z$$ where \(\gamma\) is the specific weight of the liquid, \(Q\) is the volume flow rate \(\left(\mathrm{L}^{3} \mathrm{~T}^{-1}\right),\) and \(D\) is the diameter of the pipe. Show that Equation 6.25 is dimensionally homogeneous.

Short Answer

Expert verified
Equation 6.25 is dimensionally homogeneous; both sides have dimension \( \text{F L}^{-2} \).

Step by step solution

01

Understand Equation 6.25

Look at Equation 6.25: \[ p = -\gamma\left(1+0.24 \frac{Q^{2}}{g D^{5}}\right) z \]. Here \( \gamma \) represents specific weight \( \left( \text{F L}^{-3} \right) \), \( Q \) is the flow rate \( \left( \text{L}^3 \text{T}^{-1} \right) \), \( g \) is the gravitational acceleration \( \left( \text{L T}^{-2} \right) \), and \( D \) is the pipe diameter \( \left( \text{L} \right) \). The primary unit of pressure \( p \) is \( \text{F L}^{-2} \).
02

Analyze Dimensions for Pressure Term

The left side of Equation 6.25 is \( p \) with dimensions \( \text{F L}^{-2} \). Ensure the right side matches these dimensions.
03

Determine Dimensions of Right Side Expression

The expression \(-\gamma z\) has dimensions \( \text{F L}^{-3} \times \text{L} = \text{F L}^{-2} \).
04

Analyze Dimensionless Term

Analyzing \( 0.24 \frac{Q^2}{gD^5} \): \( Q^2 \) has dimensions \( \left( \text{L}^3 \text{T}^{-1} \right)^2 = \text{L}^6 \text{T}^{-2} \), \( g \) has dimensions \( \text{L T}^{-2} \), \( D^5 \) has dimensions \( \text{L}^5 \). Thus, \( \frac{Q^2}{gD^5} = \frac{\text{L}^6 \text{T}^{-2}}{\text{L T}^{-2} \times \text{L}^5} = 1 \), resulting in a dimensionless term.
05

Combine Results

The equation simplifies to having \(-\gamma z\) with dimensions \( \text{F L}^{-2} \), matching the dimensions of \( p \). The term \((1 + 0.24 \frac{Q^{2}}{g D^{5}})\) is dimensionless and does not affect the overall dimensionality.

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Fluid Flow in Pipes
Fluid flow in pipes is a fundamental concept in fluid dynamics, involving the movement of liquid through a conduit. Understanding this process is crucial in engineering applications like water supply, chemical processing, and heating systems. In the context of fluid flow, pipes can be oriented in various directions, such as horizontally, vertically, or at any angle between these two.

When dealing with upward fluid flow in a vertical pipe, as the exercise suggests, we have to consider gravitational effects. The fluid must overcome gravity while being pushed upward, which requires careful pressure management.

Key considerations include:
  • Velocity and Flow Rate: Velocity denotes how fast the fluid particles move along the pipe, while the flow rate is the volume of fluid moving through a section of pipe per unit of time.
  • Pipe Diameter: The diameter significantly affects the flow rate and velocity. A larger diameter allows more fluid to pass through, potentially decreasing resistance and pressure losses.
  • Pressure Drops: As fluid moves up, it tends to lose pressure due to friction and elevation gains, which needs calculation for efficiency and system design.
  • Pressure Loss Calculations: Engineers use mathematical models, like Bernoulli's equation, to estimate the necessary pressure for maintaining flow.
These factors must be balanced to ensure efficient and safe operation of pipe systems.
Pressure Calculation
Calculating pressure in fluid systems, especially vertical pipes, requires understanding the interplay between different forces acting on the fluid.

In our exercise, the pressure calculation formula is given as: \[ p = -\gamma \left(1+0.24 \frac{Q^{2}}{g D^{5}}\right) z \]This demonstrates how the pressure, \( p \), changes with height, \( z \), above a reservoir's surface.
  • Specific Weight, \( \gamma \): This is a measure of the weight per unit volume of a fluid, factoring significantly in the pressure exerted by the fluid column.
  • Height, \( z \): The higher the liquid rises in a pipe, the greater the gravitational potential energy it gains. This increases the pressure required at the base to push the fluid up.
  • Dimensionless Modification Factor: The factor \(1+0.24 \frac{Q^{2}}{g D^{5}}\) accounts for non-gravitational forces, adjusting pressure for flow conditions and pipe geometry.
Calculating the correct pressure is vital for efficient fluid management and safety in systems, avoiding issues like pipe bursts or insufficient supply.
Dimensionless Analysis
Dimensionless analysis helps simplify complex fluid dynamic problems by reducing the number of variables. By concentrating on ratios, engineers can predict how a system will perform under different conditions without needing to replicate the exact scenario.

In the exercise, the term \(0.24 \frac{Q^{2}}{g D^{5}}\) is a dimensionless quantity. Let's explore why dimensionless numbers are powerful:
  • Simplification: By transforming variables into dimensionless quantities, equations and calculations often become more straightforward and interpretable.
  • Comparison Across Systems: Dimensional homogeneity lets engineers compare different systems, or scale models to real life, to predict behaviors without directly measuring every variable.
  • Universal Application: Many dimensionless numbers like Reynolds number apply universally across different contexts in fluid dynamics, aiding in standardized analysis of flow conditions.
Dimensionless analysis is a crucial tool in fluid engineering, allowing for accurate predictions and designs in diverse fluid flow scenarios.

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Most popular questions from this chapter

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