For what types of fluids and flows is the viscous dissipation term in the energy equation likely to be significant?

Short Answer

Expert verified
Answer: The viscous dissipation term becomes significant for fluid flow under conditions with high fluid viscosity, high flow velocities, and large gradients in fluid velocity. This is typically observed in highly viscous fluids or flow scenarios with abrupt velocity changes, such as in pumps, turbines, or around obstacles.

Step by step solution

01

Understand the energy equation for fluid flow

The energy equation for fluid flow demonstrates the conservation of energy in fluid systems and is used to describe how the energy changes due to fluid motion, pressure, viscous forces, and external work. The general form of the energy equation is: E_in + E_out + E_stored = 0 where E_in is the energy input, E_out is the energy output, and E_stored is the change in energy stored in the system. For fluid flow, the energy equation can be expressed as: ρ((∂e)/∂t + v∙∇e) = -∇∙(ρve) + (σ:∇)v Here, ρ is the fluid density, e is the specific internal energy, v is the fluid velocity vector, σ is the stress tensor, and the ":" denotes a double dot product.
02

Identify the viscous dissipation term

In the energy equation, the viscous dissipation term is given by the expression (σ:∇)v, which represents the work done by the viscous forces in the fluid. This term is responsible for dissipating energy as heat due to the fluid's internal friction.
03

Analyze the conditions for the significance of viscous dissipation term

The viscous dissipation term will be significant under the following conditions: 1. High fluid viscosity: The viscous dissipation term is directly related to the fluid's viscosity. As the viscosity increases, the energy dissipation due to viscous forces also increases. Therefore, fluids with high viscosity, such as honey and motor oil, are more likely to have significant viscous dissipation. 2. High flow velocities: When the fluid flow velocity is high, it leads to an increased rate of energy dissipation due to the viscous forces. As a result, the viscous dissipation term will be more significant in high-speed flows, such as the flow in a turbine or high-performance pumps. 3. Large gradients in fluid velocity: The viscous dissipation term is also related to the gradient of the fluid velocity. When there are abrupt changes in the fluid velocity (e.g., around obstacles or in the boundary layer), the viscous dissipation term becomes more significant.
04

Conclusion

The viscous dissipation term in the energy equation is likely to be significant for fluids with high viscosity, high flow velocities, and large gradients in fluid velocity. This includes highly viscous fluids or flow scenarios where abrupt velocity changes occur, such as in pumps, turbines, or around obstacles.

Unlock Step-by-Step Solutions & Ace Your Exams!

  • Full Textbook Solutions

    Get detailed explanations and key concepts

  • Unlimited Al creation

    Al flashcards, explanations, exams and more...

  • Ads-free access

    To over 500 millions flashcards

  • Money-back guarantee

    We refund you if you fail your exam.

Over 30 million students worldwide already upgrade their learning with Vaia!

Key Concepts

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

Understanding the Energy Equation in Fluid Flow
The energy equation is a fundamental concept in fluid mechanics, holding key to analyzing energy conservation and transfer within fluid systems. It equates the sum of energy inputs, outputs, and storage changes to zero, implying that energy in a closed system is conserved. For fluids, the equation takes the form

\[\rho\left(\frac{\partial e}{\partial t} + \boldsymbol{v} \cdot abla e\right) = -abla \cdot (\rho\boldsymbol{ve}) + (\boldsymbol{\sigma}:abla)\boldsymbol{v}\]
where \(\rho\) is the fluid density, \(e\) is specific internal energy, \(\boldsymbol{v}\) is the fluid velocity vector, and \(\boldsymbol{\sigma}\) is the stress tensor. The term \((\boldsymbol{\sigma}:abla)\boldsymbol{v}\) is particularly interesting as it represents the viscous dissipation, which can turn kinetic energy into thermal energy, heating the fluid. This is significant especially when dealing with high-velocity flows or fluids with high viscosity, as they lead to greater energy conversion from mechanical to thermal due to friction.
The Role of Fluid Viscosity in Energy Dissipation
Viscosity is the measure of a fluid's resistance to deformation at a given rate, and it plays a critical role in energy dissipation during flow. Highly viscous fluids, like honey or motor oil, experience more friction as they flow, which translates to higher energy loss in the form of heat.

Whenever a fluid's viscosity is high, the internal layers of fluid move with different speeds, which causes more interaction and friction between these layers. This energy loss, captured in the viscous dissipation term \((\boldsymbol{\sigma}:abla)\boldsymbol{v}\) of the energy equation, is more pronounced in certain scenarios. For example, pumping viscous fluids through a pipeline or the movement of high viscosity substances in manufacturing processes often results in significant energy dissipation, affecting the overall efficiency of fluid flow systems.
Velocity Gradients and their Effect on Fluid Flow
Velocity gradients refer to the changes in speed within different parts of a fluid flow, which are the root of viscous dissipation. In areas with high velocity gradients, such as nearby surfaces of solid objects or within narrow passages, the rate of energy loss due to internal friction is substantial.

Imagine flowing water striking a rock in a stream: right at the rock's edge, the water's flow velocity changes abruptly, creating a significant velocity gradient. This arrangement leads to heightened viscous forces and thus to more intense energy dissipation. In engineering applications like turbines, pumps, or aerodynamic designs of vehicles, understanding and controlling velocity gradients are essential. Poor management of velocity gradients could result in unnecessary energy losses and diminished performance, highlighting the importance of incorporating these gradients into the design and analysis of fluid flow.

One App. One Place for Learning.

All the tools & learning materials you need for study success - in one app.

Get started for free

Most popular questions from this chapter

For steady two-dimensional flow, what are the boundary layer approximations?

An airfoil with a characteristic length of \(0.2 \mathrm{ft}\) is placed in airflow at \(1 \mathrm{~atm}\) and \(60^{\circ} \mathrm{F}\) with free stream velocity of \(150 \mathrm{ft} / \mathrm{s}\) and convection heat transfer coefficient of \(21 \mathrm{Btu} / \mathrm{h} \cdot \mathrm{ft}^{2} \cdot{ }^{\circ} \mathrm{F}\). If a second airfoil with a characteristic length of \(0.4 \mathrm{ft}\) is placed in the airflow at \(1 \mathrm{~atm}\) and \(60^{\circ} \mathrm{F}\) with free stream velocity of \(75 \mathrm{ft} / \mathrm{s}\), determine the heat flux from the second airfoil. Both airfoils are maintained at a constant surface temperature of \(180^{\circ} \mathrm{F}\).

What is the physical mechanism that causes the friction factor to be higher in turbulent flow?

A 5 -mm-thick stainless steel strip \((k=21 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K}, \rho=\) \(8000 \mathrm{~kg} / \mathrm{m}^{3}\), and \(\left.c_{p}=570 \mathrm{~J} / \mathrm{kg} \cdot \mathrm{K}\right)\) is being heat treated as it moves through a furnace at a speed of \(1 \mathrm{~cm} / \mathrm{s}\). The air temperature in the furnace is maintained at \(900^{\circ} \mathrm{C}\) with a convection heat transfer coefficient of \(80 \mathrm{~W} / \mathrm{m}^{2} \cdot \mathrm{K}\). If the furnace length is \(3 \mathrm{~m}\) and the stainless steel strip enters it at \(20^{\circ} \mathrm{C}\), determine the surface temperature gradient of the strip at mid-length of the furnace. Hint: Use the lumped system analysis to calculate the plate surface temperature. Make sure to verify the application of this method to this problem.

The coefficient of friction \(C_{f}\) for a fluid flowing across a surface in terms of the surface shear stress, \(\tau_{s}\), is given by (a) \(2 \rho V^{2} / \tau_{w}\) (b) \(2 \tau_{w} / \rho V^{2}\) (c) \(2 \tau_{w} / \rho V^{2} \Delta T\) (d) \(4 \tau_{w} / \rho V^{2}\) (e) None of them

See all solutions

Recommended explanations on Physics Textbooks

View all explanations

What do you think about this solution?

We value your feedback to improve our textbook solutions.

Study anywhere. Anytime. Across all devices.

Sign-up for free