Session 02 Basic Concepts in Fluid Mechanics - 2 Content 2.1 Types of Fluids 15 2.2 Dimensions 17 2.3 Units 18 2.4 Dimensional Homogeneity 19 2.5 Applications of fluid mechanics in different areas 19 Summary 22 Learning Outcomes 22 2.1 Types of Fluids There are five types of fluids. • • • • • Ideal Fluid Real Fluid Newtonian Fluid Non Newtonian Fluid Ideal Plastic Fluid Ideal Fluid In the preceding sections we have reviewed the principal physical properties of fluids. It is, however, rare for a specific engineering problem to be solved after taking into consideration all the properties of fluids. The mathematics and physical arguments become too complicated if all the properties of fluid is considered. In fact, the numerical accuracy achieved by considering real fluid behavior is often not necessary. An approximate solution obtained by making simplifying assumptions is usually adequate. The simplification often made is to assume the fluid to be ideal. The ideal fluid is assumed, (a) to have zero viscosity and, hence, cannot develop and shear stresses; (b) to be incompressible; 15 (c) to have no surface tension; and (d) not to vaporise. With these assumptions, many problems can now be solved, although there is certain unreality when compared with real fluids. Experimental evidence can be used to convert the predicted result, and the value of empirical coefficients used is an indication of the accuracy of assuming an ideal fluid. Real fluid A fluid which possesses as real fluid. All the fluids in actual practice are real fluids. Newtonian fluid A real fluid, in which the shear stress is directly, proportional to the rate of shear strain (or velocity gradient), is known as Newtonian fluid. The graphs plotting shear stress against rate of shear or velocity gradient is called rheograms. The slope of the straight line in any rheogram of a Newtonian fluid represents the viscosity (or more specifically, the dynamic viscosity) of the fluid. The higher viscosity of a fluid becomes the steeper the slope in the rheogram. Fluids such as air, water, oil, glycerin, and honey are described as Newtonian fluids. Figure 2.1: Rheogram of various Newtonian fluids Non-Newtonian fluid A real fluid, in which the shear stress is not proportional to the rate of shear strain (or velocity gradient), is known as Non-Newtonian fluid. For Non-Newtonian fluids, the line in the rheogram either is curved or does not pass through the origin, or both. Figure (3.2) shows the rheograms of various types of Non16 Newtonian fluids. Note that while the rheogram of a pseudoplastic fluid curves downward (i.e., having decreasing slope with increased shear), for a dilatant fluid the rheogram curves upward (i.e. having increasing slope with increased shear). Otherwise, the two are similar: they both pass through the origin of the rheogram, as is the case with Newtonian fluids. As shown in Fig. (1.6), a Bingham plastic (or simply Bingham) fluid is represented by a straight line in rheograms, but the line does not pass through the origin. It takes a certain minimum shear stress, called the yield stress to cause a Bingham fluid to behave like a fluid. Figure 2.3: Rheogram of various Non-Newtonian fluids Ideal plastic fluid A real fluid, in which the shear stress is more that the yield value and the shear stress is proportional to the rate of shear strain (or velocity gradient), is known as ideal plastic fluid. 2.2 Dimensions A dimension is a category that represents a physical quantity such as mass, length, time, momentum, force, acceleration, and energy. To simplify matters, engineers express dimensions using a limited set that are called primary dimensions. Table 2.1 lists one common set of primary dimensions. Table 2.1: Primary Dimensions Dimension Symbol Unit (SI) 17 Length L meter (m) Mass M kilogram (kg) Time T second (s) Temperature θ kelvin (K) Electric current i ampere (A) Amount of light C candela (cd) Amount of matter N mole (mol) Secondary dimensions such as momentum and energy can be related to primary dimensions by using equations. For example, the secondary dimension “force” is expressed in primary dimensions by using Newton’s second law of motion, 𝐹 = 𝑚𝑎. The primary dimensions of acceleration are 𝐿/𝑇 2 , Therefore 𝐹 = 𝑚𝑎 = 𝑀𝐿 𝑇2 2.3 Units While a dimension expresses a specific type of physical quantity, a unit assigns a number so that the dimension can be measured. For example, measurement of volume (a dimension) can be expressed using units of liters. Similarly, measurement of energy (a dimension) can be expressed using units of joules. Most dimensions have multiple units that are used for measurement. For example, the dimension of “force” can be expressed using units of newtons, pounds-force, or dynes. In practice, there are several unit systems in use. The International System of Units (abbreviated SI from the French “Le Système International d'Unités”) is based on the meter, kilogram, and second. Although the SI system is intended to serve as an international standard, there are other systems in common use in the United States. The U.S. Customary System (USCS), sometimes called English Engineering System, uses the pound-mass (lbm) for mass, the foot (ft) for length, the pound-force (lbf) for force, and the second (s) for time. Table 2.2: Units for different quantities QUANTITY SI UNITS Mass kilogram (kg) Length metre (m) Time second (s) Density kilogrames/metre3 (kg/m3) 18 Force Newton (N) Velocity metre/Sec (m/s) Acceleration metre/Sec2 (m/s2) Pressure Pascal (N/m2) Surface tension Newton/metre (N/m) Work Joules (J) Power kilowatt (kw) Volume metre3 (m3) 2.4 Dimensional Homogeneity When the primary dimensions on each term of an equation are the same, the equation is dimensionally homogeneous. For example, consider the equation for vertical position 𝑠 of an object moving in a gravitational field: 𝑠= 𝑔𝑡 2 2 + 𝑣0 𝑡 + 𝑠0 In the equation, 𝑔 is the gravitational constant, 𝑡 is time, 𝑣𝑜 is the magnitude of the vertical component of the initial velocity, and 𝑠𝑜 is the vertical component of the initial position. This equation is dimensionally homogeneous because the primary dimension of each term is length 𝐿. 2.5 Applications of fluid mechanics in different areas Hydraulics Hydraulics is the study of the flow of water through pipes, rivers, and openchannels. This includes pumps and turbines and applications such as hydropower. Hydraulics is important for ecology, policymaking, energy production, recreation, fish and game resources, and water supply. Hydrology Hydrology is the study of the movement, distribution, and quality of water throughout the earth. Hydrology involves the hydraulic cycle and water resource issues. Thus, hydrology provides results that are useful for environmental engineering and for policymaking. Hydrology is important nowadays because of global challenges in providing water for human societies. 19 Aerodynamics Aerodynamics is the study of air flow. Topics include lift and drag on objects (e.g., airplanes, automobiles, birds), shock waves associated with flow around a rocket, and the flow through a supersonic or deLaval nozzle. Aerodynamics is important for the design of vehicles, for energy conservation, and for understanding nature. Bio-fluid mechanics Bio-fluid mechanics is an emerging field that includes the study of the lungs and circulatory system, blood flow, micro-circulation, and lymph flow. Bio-fluids also includes development of artificial heart valves, stents, vein and dialysis shunts, and artificial organs. Bio-fluid mechanics is important for advancing health care. Acoustics Acoustics is the study of sound. Topics include production, control, transmission, reception of sound, and physiological effects of sound. Since sound waves are pressure waves in fluids, acoustics is related to fluid mechanics. In addition, water hammer in a piping system, which involves pressure waves in liquids, involves some of the same knowledge that is used in acoustics. Microchannel flow Microchannel flow is an emerging area that involves the study of flow in tiny passages. The typical size of a microchannel is a diameter in the range of 10 to 200 micrometers. Applications that involve microchannels include microelectronics, fuel cell systems, and advanced heat sink designs. Computational fluid dynamics (CFD) CFD is the application of numerical methods implemented on computers to model and solve problems that involve fluid flows. Computers perform millions of calculations per second to simulate fluid flow. Examples of flows that are modeled by CFD include water flow in a river, blood flow in the abdominal aorta, and air flow around an automobile. Petroleum engineering Petroleum engineering is the application of engineering to the exploration and production of petroleum. Movement of oil in the ground involves flow through a porous medium. Petroleum extraction involves flow of oil through passages in wells. Oil pipelines involve pumps and conduit flow. 20 Atmospheric science Atmospheric science is the study of the atmosphere, its processes, and the interaction of the atmosphere with other systems. Fluid mechanics topics include flow of the atmosphere and applications of CFD to atmospheric modeling. Atmospheric science is important for predicting weather and is relevant to current issues including acid rain, photochemical smog, and global warming. Electrical engineering Electrical engineering problems can involve knowledge from fluid mechanics. For example, fluid mechanics is involved in the flow of solder during a manufacturing process, the cooling of a microprocessor by a fan, sizing of motors to operate pumps, and the production of electrical power by wind turbines. Environmental engineering Environmental engineering involves the application of science to protect or improve the environment (air, water, and or land resources) or to remediate polluted sites. Environmental engineers design water supply and wastewater treatment systems for communities. Environmental engineers are concerned with local and worldwide environmental issues such as acid rain, ozone depletion, water pollution, and air pollution. S.A.Q. 1: Show that the Reynolds number (𝑅𝑒) given by 𝑅𝑒 = 𝜌𝑣𝐷 𝜇 , is a dimensionless group, where 𝜌 is the density, 𝑣 is the velocity, 𝐷 is the diameter and 𝜇 is the viscosity. S.A.Q. 2: Derive the units of viscosity in terms of force, time and length in the SI system Answer In the SI system, Force – Newton (N) Time – seconds (s) Length – metres (m) τ = Force/Area = N/m2 𝑑𝑢 = 𝑚⁄𝑠 𝑑𝑦 = 𝑚 21 μ= τ du ( ) dy 𝜇= (𝑁⁄ 2 ) 𝑚 (𝑚⁄𝑠) 𝑚 = 𝑁𝑠/𝑚2 = 𝑃𝑎 Summary Fluid mechanics involves the application of scientific concepts such as position, force, velocity, acceleration, and energy to materials that are in the liquid or gas states. A fluid is defined as a substance that continually deforms (flows) under an applied shear stress. Basically, the fluids are classified into five types and these are; 1. Ideal fluid 2. Real fluid 3. Newtonian fluid 4. Non-Newtonian fluid 5. Ideal plastic fluid. In fluid mechanics, there are four primary dimensions: mass, length, time, and temperature. Primary dimensions are defined as independent dimensions, from which all other dimensions can be obtained. Dimensions have no numbers associated with them. A unit is a way to assign a number or measurement to a dimension. Units must always have numbers associated with them. Learning Outcomes At the end of this lesson the student should be able to • identify different types of fluids, be familiar with some of its basic properties • be able to deal with the systems of units and dimensions used in measuring different fluid quantities. 22 23