Fluid Mechanics is the branch of science that studies the behavior of fluids when they are in state of motion or rest. Gases are not bonded to neighboring atoms and can have large separations between molecules. At high temperatures, molecules may disassociate into atoms, and atoms disassociate into electrons (with negative charges) and protons (with positive charges), forming a plasma. Viscosity 1. (Shearing forces are forces applied tangentially to a surface, as described in Static Equilibrium and Elasticity.). Density is an important characteristic of substances. These parameters generally include fluid properties (e.g., density, viscosity and surface tension), system geometry (e.g., length, area and volume) or flow conditions (e.g., velocity, pressure change and applied force). Fluid located at deeper levels is subjected to more force than fluid nearer to the surface due to the weight of the fluid above it. The LibreTexts libraries arePowered by NICE CXone Expertand are supported by the Department of Education Open Textbook Pilot Project, the UC Davis Office of the Provost, the UC Davis Library, the California State University Affordable Learning Solutions Program, and Merlot. For fluid mechanics density normally used instead of mass, since mass is dependent on how much fluid is present. Learning Objectives By the end of this section, you will be able to: . Density = mass per unit volume Here, the unit of mass is kg, the unit of volume is m 3. Specific gravity is a particularly useful quantity with regard to buoyancy, which we will discuss later in this chapter. Density is a dimensional property; therefore, when comparing the densities of two substances, the units must be taken into consideration. Density Practice Problems. A U-tube manometer similar to that shown in Figure 3.8 is used to measure the gauge pressure of a fluid P of density = 1000 kg/m3. Atmospheric pressure exerts a large force (equal to the weight of the atmosphere above your bodyabout 10 tons) on the top of your body when you are lying on the beach sunbathing. This behavior of the density of water explains why ice forms at the top of a body of water. }\hfill \end{array}[/latex], [latex]p(y+\Delta y)A-p(y)A-g\Delta m=0(\Delta y \gt 0). Fluid Properties Density ( ) Defined as ratio of mass per unit volume, n i. e. density ( ) = mass (m) / volume (V). Density The density of a fluid, is generally designated by the Greek symbol (rho) is defined as the mass of the fluid over an infinitesimal volume. The gases are displayed for a standard temperature of [latex]0.0^\circ\text{C}[/latex] and a standard pressure of 101.3 kPa, and there is a strong dependence of the densities on temperature and pressure. The presence of the elastic particles in a variable density fluid allows the density of the variable density fluid to vary as a function of pressure. using bernolli's principle, why does a plane lift with increased speed. The density [latex]\rho[/latex] at y, the temperature T in the Kelvin scale (K), and the mass m of a molecule of air are related to the absolute pressure by the ideal gas law, in the form. Specific gravity is defined as the ratio of the density of the material to the density of water at [latex]4.0\,{}^\circ \text{C}[/latex] and one atmosphere of pressure, which is [latex]1000\,{\text{kg/m}}^{3}[/latex]: The comparison uses water because the density of water is [latex]1\,{\text{g/cm}}^{3}[/latex], which was originally used to define the kilogram. (Recall that we introduced the idea of pressure in Static Equilibrium and Elasticity, in the context of bulk stress and strain. P fluid = Pressure at a point taken in fluid . The density of a substance is not necessarily constant throughout the volume of a substance. Air is a gas at room temperature and atmospheric pressure. volume. Specific Gravity 5. Therefore, the densities of liquids are often treated as constant, with the density equal to the average density. where the Greek letter [latex]\rho[/latex] (rho) is the symbol for density, m is the mass, and V is the volume. x 6.4 cm long (plastic is less dense than water) The pressure at any point in a static fluid depends only on the depth at that point. If the density is constant throughout a substance, the substance is said to be a homogeneous substance. A chunk of Swiss cheese is an example of a heterogeneous material containing both the solid cheese and gas-filled voids. In a swimming pool, for example, the density is approximately constant, and the water at the bottom is compressed very little by the weight of the water on top. The pressure due to the fluid is equal to the weight of the fluid divided by the area. This manometer consists of a U-Tube as shown in figure-2. As you can see by examining Figure, the density of an object may help identify its composition. [/latex], [latex]\alpha =-\frac{mg}{{k}_{\text{B}}T}=\frac{4.8\times {10}^{-26}\,\text{kg}\,\times 9.81\,{\text{m/s}}^{2}}{1.38\times {10}^{-23}\,\text{J/K}\times \text{300 K}}=\frac{1}{8800\,\text{m}}. Where, m = mass of the fluid Upthrust is the force exerted on a body by the fluid it is submerged into. 2. The speed of sound in an incompressible fluid is also constant. [/latex], [latex]\frac{p(y+\Delta y)-p(y)}{\Delta y}=\text{}\rho g.[/latex], [latex]\frac{dp}{dy}=\text{}\rho g.[/latex], [latex]\begin{array}{ccc}\hfill {\int }_{{p}_{0}}^{p}dp& =\hfill & \text{}{\int }_{0}^{\text{}h}\rho gdy\hfill \\ \hfill p-{p}_{0}& =\hfill & \rho gh\hfill \\ \hfill p& =\hfill & {p}_{0}+\rho gh.\hfill \end{array}[/latex], [latex]p=\rho \frac{{k}_{\text{B}}T}{m}\,\text{(atmosphere),}[/latex], [latex]\frac{dp}{dy}=\text{}p(\frac{mg}{{k}_{\text{B}}T}),[/latex], [latex]\begin{array}{ccc}\hfill \frac{dp}{dy}& =\hfill & \text{}\alpha p\hfill \\ \hfill \frac{dp}{p}& =\hfill & \text{}\alpha dy\hfill \\ \hfill \underset{{p}_{0}}{\overset{p(y)}{\int }}\frac{dp}{p}& =\hfill & \underset{0}{\overset{y}{\int }}\text{}\alpha dy\hfill \\ \hfill {[\text{ln}(p)]}_{{p}_{0}}^{p(y)}& =\hfill & {[\text{}\alpha y]}_{0}^{y}\hfill \\ \hfill \text{ln}(p)-\text{ln}({p}_{0})& =\hfill & \text{}\alpha y\hfill \\ \hfill \text{ln}(\frac{p}{{p}_{0}})& =\hfill & \text{}\alpha y\hfill \end{array}[/latex], [latex]p(y)={p}_{0}\text{exp}(\text{}\alpha y). A solid iron bar is an example of a homogeneous substance. Likewise, pressure is exerted perpendicular to the surfaces of any object within the fluid. The density of water is 1 kg/L (or 1 g/mL or 1 g/cm 3 ). That is why a sharp needle is able to poke through skin when a small force is exerted, but applying the same force with a finger does not puncture the skin (Figure \(\PageIndex{4}\)). }[/latex] Assume that the density of the water is [latex]\rho =1000\,{\text{kg/m}}^{3}. This occurs because the brass has a greater density than water, whereas the wood has a lower density than water. Fluids include liquids. Image: Density column containing some common liquids and solids. Like solids, the molecules in a liquid are bonded to neighboring molecules, but possess many fewer of these bonds. [/latex], [latex]\begin{array}{cc}\hfill p& =(40.0\,\text{m})({10}^{3}\,\frac{\text{kg}}{{\text{m}}^{3}})(9.80\frac{\text{m}}{{\text{s}}^{2}})\hfill \\ & =3.92\times {10}^{5}\,\frac{\text{N}}{{\text{m}}^{2}}=392\,\text{kPa}\text{. Pressure is a scalar quantity because it is defined to be proportional to the magnitude of the force acting perpendicular to the surface area. [/latex], Entering the density of water from Figure and taking h to be the average depth of 40.0 m, we obtain. Generally, these are either a gas or a liquid. \(h\) is the height of the fluid. Assuming the temperature of air to be constant, and that the ideal gas law of thermodynamics describes the atmosphere to a good approximation, we can find the variation of atmospheric pressure with height, when the temperature is constant. The density of a fluid is defined as the ratio of the mass of the fluid to its volume. Density The average density of a substance or object is defined as its mass per unit volume, = m V 14.1 where the Greek letter (rho) is the symbol for density, m is the mass, and V is the volume. 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https://phys.libretexts.org/@app/auth/3/login?returnto=https%3A%2F%2Fphys.libretexts.org%2FBookshelves%2FUniversity_Physics%2FBook%253A_University_Physics_(OpenStax)%2FBook%253A_University_Physics_I_-_Mechanics_Sound_Oscillations_and_Waves_(OpenStax)%2F14%253A_Fluid_Mechanics%2F14.02%253A_Fluids_Density_and_Pressure_(Part_1), \( \newcommand{\vecs}[1]{\overset { \scriptstyle \rightharpoonup} {\mathbf{#1}}}\) \( \newcommand{\vecd}[1]{\overset{-\!-\!\rightharpoonup}{\vphantom{a}\smash{#1}}} \)\(\newcommand{\id}{\mathrm{id}}\) \( \newcommand{\Span}{\mathrm{span}}\) \( \newcommand{\kernel}{\mathrm{null}\,}\) \( \newcommand{\range}{\mathrm{range}\,}\) \( \newcommand{\RealPart}{\mathrm{Re}}\) \( \newcommand{\ImaginaryPart}{\mathrm{Im}}\) \( \newcommand{\Argument}{\mathrm{Arg}}\) \( \newcommand{\norm}[1]{\| #1 \|}\) \( \newcommand{\inner}[2]{\langle #1, #2 \rangle}\) \( \newcommand{\Span}{\mathrm{span}}\) \(\newcommand{\id}{\mathrm{id}}\) \( \newcommand{\Span}{\mathrm{span}}\) \( \newcommand{\kernel}{\mathrm{null}\,}\) \( \newcommand{\range}{\mathrm{range}\,}\) \( \newcommand{\RealPart}{\mathrm{Re}}\) \( \newcommand{\ImaginaryPart}{\mathrm{Im}}\) \( \newcommand{\Argument}{\mathrm{Arg}}\) \( \newcommand{\norm}[1]{\| #1 \|}\) \( \newcommand{\inner}[2]{\langle #1, #2 \rangle}\) \( \newcommand{\Span}{\mathrm{span}}\)\(\newcommand{\AA}{\unicode[.8,0]{x212B}}\), 14.3: Fluids, Density, and Pressure (Part 2), Table 14.1 - Densities of Some Common Substances, source@https://openstax.org/details/books/university-physics-volume-1, status page at https://status.libretexts.org, Describe the characteristics of the phases of matter at the molecular or atomic level, Distinguish between compressible and incompressible materials, Compare and contrast the densities of various substances, Explain the relationship between pressure and force. Figure lists some representative values. volume displaced = objects volume. The upthrust determines whether an object will float or sink. The density of an object or substance can be calculated from this equation: density in kilograms per . The image shows how sandbags placed around a leak outside a river levee can effectively stop the flow of water under the levee. The fuel tank has a total volume of 55 liters. Pressure is the force per unit perpendicular area over which the force is applied, [latex]p=F\text{/}A. In contrast, atoms in gases are separated by large distances, and the forces between atoms in a gas are therefore very weak, except when the atoms collide with one another. That is, liquids flow (so they are a type of fluid), with the molecules held together by mutual attraction. If the density of a substance were not constant, the substance is said to be a heterogeneous substance. Whatis the density of water at 80C ? Since the density is constant, the weight can be calculated using the density: The pressure at the bottom of the container is therefore equal to atmospheric pressure added to the weight of the fluid divided by the area: This equation is only good for pressure at a depth for a fluid of constant density. It is a condition specific to certain substances or it is a subset of matter. Next to the lake, a glacier with the same volume as the floating ice sits on land.

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