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The momentum equation that describes the motion of a nonviscous incompressible fluid in a three-dimensional \((x y z)\) flow field can be expressed in the form $$\rho\left[\frac{\partial \mathbf{V}}{\partial t}+u \frac{\partial \mathbf{V}}{\partial x}+v \frac{\partial \mathbf{V}}{\partial y}+w \frac{\partial \mathbf{V}}{\partial z}\right]=-\nabla p-\rho g \mathbf{k}$$ where \(\rho\) is the density of the fluid, \(\mathbf{V}\) is the velocity vector with components \(u, v,\) and \(w, p\) is the pressure, and \(g\) is the gravity constant. Consider the case in which the only relevant scales are the length scale, \(L,\) and the velocity scale, \(V\). Note that time can be normalized by \(L / V\) and pressure can be normalized by \(\rho V^{2}\). Express Equation 6.29 in normalized form, using the Froude number, Fr, defined as \(\mathrm{Fr}=V / \sqrt{g L},\) in the final expression. What happens to the effect of gravity on the flow as the Froude number becomes large?

Short Answer

Expert verified
As the Froude number increases, gravity's effect on the flow diminishes.

Step by step solution

01

Set Up the Equation

The given momentum equation is \(\rho\left[\frac{\partial \mathbf{V}}{\partial t}+u \frac{\partial \mathbf{V}}{\partial x}+v \frac{\partial \mathbf{V}}{\partial y}+w \frac{\partial \mathbf{V}}{\partial z}\right]=-abla p-\rho g \mathbf{k}\). We'll begin by identifying each term with its physical significance, such as inertia, pressure gradient, and gravitational force.
02

Normalize Time and Pressure

Since time \(t\) is scaled by \(L/V\), we redefine dimensionless time as \(t^* = tV/L\). Pressure is scaled by \(\rho V^2\), so define dimensionless pressure as \(p^* = p/(\rho V^2)\). The velocity components \(u, v, w\) are already in terms of the velocity scale, so they remain as they are.
03

Express in Dimensionless Form

Substituting the scaled variables into the original equation and dividing by \(\rho V^2/L\) gives: \[\frac{\rho V}{L}\left[\frac{\partial \mathbf{V}}{\partial t^*}+u \frac{\partial \mathbf{V}}{\partial x}+v \frac{\partial \mathbf{V}}{\partial y}+w \frac{\partial \mathbf{V}}{\partial z}\right]= -abla p^* - \frac{\rho g}{V^2/L} \mathbf{k}.\]
04

Simplify and Introduce Froude Number

Recognizing that \(\frac{\rho g}{V^2/L} = \rho \frac{gL}{V^2} \approx \rho/\mathrm{Fr}^2\), the dimensionless form becomes: \[\frac{\partial \mathbf{V}}{\partial t^*} + u \frac{\partial \mathbf{V}}{\partial x} + v \frac{\partial \mathbf{V}}{\partial y} + w \frac{\partial \mathbf{V}}{\partial z} = -abla p^* - \frac{1}{\mathrm{Fr}^2} \mathbf{k}.\]
05

Analyze Effect of Froude Number

As the Froude number \(\mathrm{Fr}\) becomes large, \(1/\mathrm{Fr}^2\) becomes very small. This implies that the term representing the gravitational effect, \(-\frac{1}{\mathrm{Fr}^2} \mathbf{k}\), becomes negligible, indicating that gravity has less influence on the flow.

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Key Concepts

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

Dimensionless Analysis
Dimensionless analysis is a useful mathematical tool in fluid mechanics and beyond, as it helps simplify complex physical problems by reducing the number of variables. This technique involves creating dimensionless numbers or parameters that can be used to characterize physical systems, making it easier to identify dominant forces or effects in different scenarios.

A key aspect of dimensionless analysis is identifying relevant scales for quantities like length, time, and velocity, and using these to normalize equations. By doing so, we can better compare different fluid flows and make predictions about their behavior. For instance, instead of dealing with units like meters and seconds, we use symbolic terms like length scales and time scales.

This simplification often leads to equations with dimensionless terms that highlight important relationships between different physical quantities. In fluid mechanics, this is particularly beneficial because it helps in reducing the complexity of the Navier-Stokes equations, enabling us to focus on the significant effects influencing fluid flow, such as inertia, viscous forces, and gravity.
Froude Number
The Froude number (\( \mathrm{Fr} \)) is an important dimensionless parameter in fluid dynamics, particularly when considering the effects of gravity on a given fluid flow. Defined as the ratio of a flow's inertial forces to gravitational forces, it offers critical insights into the flow regime of a fluid system.

Mathematically, the Froude number is expressed as \(\mathrm{Fr}=V / \sqrt{g L} \), where \(V\) is the flow velocity, \(g\) the acceleration due to gravity, and \(L\) a characteristic length. The Froude number helps determine the balance between the flow's inertia and gravitational pull, especially in open channel flows, such as rivers and channels.

High Froude numbers, greater than 1, indicate that inertial forces dominate, leading to rapid flows where gravity plays a minor role. Conversely, low Froude numbers, less than 1, suggest that gravity significantly influences the flow behavior.

Understanding the Froude number is essential for designing hydraulic structures, ensuring efficient water transportation, and anticipating how a fluid will behave under various conditions.
Nonviscous Incompressible Flow
Nonviscous and incompressible flow refers to an idealized fluid motion where viscosity and density variations are neglected. While real fluids always exhibit some viscosity, considering a nonviscous (also known as inviscid) nature simplifies analysis significantly by assuming the absence of internal friction.

For such flows, the primary forces considered are inertial and external forces, like pressure gradients and gravity, without the complicating effects of viscous shear forces. In compressible flows, the fluid's density remains constant throughout the motion, eliminating changes in volume and pressure.

These assumptions allow one to focus more on how the velocity and pressure interact in a system, which is crucial for understanding simple flow patterns in applications ranging from aerodynamics to pipelines. Despite being an idealization, this type of analysis forms the foundational layer for more complex investigations where viscous and compressible effects are progressively introduced.
Gravity Effect in Fluid Mechanics
Gravity plays a pivotal role in fluid mechanics as it influences the movement and behavior of fluids. When analyzing fluid flows, the gravitational force is often a fundamental component of the equations governing their motion, like the momentum equation presented in the exercise.

In fluid systems, gravity can drive motion, such as in free-falling liquids or down-slope water flows. Its effects can be quantified through dimensionless numbers like the Froude number, which portrays the relative significance of gravitational forces alongside other factors, such as fluid momentum.

As demonstrated by analyzing the momentum equation, when the gravity term is negligible relative to other forces (e.g., at large Froude numbers), its impact becomes less pronounced. However, when gravity is a dominant factor, as at low Froude numbers, it shapes the velocity and pressure distribution within the fluid. This understanding is vital for designing systems where gravity-driven flow is intended, such as aqueducts, dams, and irrigation channels, ensuring efficiency and stability.

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Most popular questions from this chapter

The power, \(P\), required to drive the propeller on a turboprop aircraft is thought to be a function of the diameter, \(D,\) forward speed, \(V,\) and rate of rotation, \(\omega,\) of the propeller, the density, \(\rho,\) and viscosity, \(\mu,\) of the air, and the sonic speed, \(c\), in the air. Determine a nondimensional functional relationship between the power, \(P\), and its influencing variables. Identify any named conventional dimensionless groups that appear in this relationship.

A fluid of density \(\rho\) and dynamic viscosity \(\mu\) flows with a velocity \(V\) toward a rectangular plate of width \(W\), height \(H\), and thickness \(T\). The approaching fluid flow makes an angle \(\theta\) with the direction normal to the plate. Determine the functional relationship between dimensionless groups that would be appropriate for studying the relationship between the drag force on the plate and the given independent variables.

An orifice in the side of an open storage tank discharges the stored liquid at an average velocity of \(V\) when the depth of liquid above the orifice is \(h\). The liquid has a density and viscosity of \(\rho\) and \(\mu\), respectively, and the acceleration due to gravity is \(g\). (a) Show by dimensional reasoning that if viscous effects are negligible, the density of the fluid does not influence the average discharge velocity. (b) If viscous effects are negligible, use dimensional analysis to determine the functional relationship between \(V\) and the influencing variables.

The length, \(L_{w},\) of the wake behind a particular model aircraft depends on the speed of the aircraft, the size of the aircraft, \(L,\) and the density and viscosity of the ambient air. Develop a nondimensional functional relationship that relates the size of the wake to its influencing variables.

The temperature distribution, \(T(x, y)\), within a two-dimensional flow field of an incompressible and nonviscous fluid is governed by the following (energy) equation: $$\rho c_{p}\left[u \frac{\partial T}{\partial x}+v \frac{\partial T}{\partial y}\right]=k\left(\frac{\partial^{2} T}{\partial x^{2}}+\frac{\partial^{2} T}{\partial y^{2}}\right)$$ where \(\rho\) and \(c_{p}\) are the density and specific heat of the fluid, respectively, \(u\) and \(v\) are the velocity components in the \(x\) - and \(y\) -directions, respectively, and \(k\) is the thermal conductivity of the fluid. The relevant scales are the length scale, \(L ;\) the velocity scale, \(V\); and the temperature scale, \(T_{0}\). Express Equation 6.31 in normalized form, using the Prandtl number, Pr, defined as \(\operatorname{Pr}=\mu c_{p} / k\), and the Reynolds number, Re, defined as \(\mathrm{Re}=\rho V L / \mu,\) where \(\mu\) is the dynamic viscosity of the fluid.

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