Pressure distribution in a fluid Pressure and pressure gradient Lecture 4 Mecânica de Fluidos Ambiental 2015/2016.

Slides:



Advertisements
Similar presentations
Chapter 3: Pressure and Fluid Statics
Advertisements

Aula 5 Mecânica dos Fluidos 2-Estática do fluido.
Hydrostatic forces on curved surfaces. Buoyancy and stability.
Lecture 2 Properties of Fluids Units and Dimensions.
Center of gravity and Centroids MET 2214
1 LECTURE 2: DIVERGENCE THEOREM, PRESSURE, ARCHIMEDES PRINCIPLE Outward normal vector: consider an arbitrarily shaped simply- connected volume. I have.
Hydrostatic Forces on Curved, Submerged Surfaces
Chapter 23 Gauss’ Law.
Lec 4: Fluid statics, buoyancy and stability, pressure
Forces on Submerged Surfaces in Static Fluids
Fluid Statics Pascal’s Law tells us that “Pressure at any point in a fluid is the same in all directions”. This means that any object submerged in a fluid.
Static Surface Forces hinge water ? 8 m 4 m . Static Surface Forces ä Forces on plane areas ä Forces on curved surfaces ä Buoyant force ä Stability of.
Forces on Submerged surfaces—plane surfaces Problem consider a plane surface of area A Draw an y and x axis passing through the centroid x y Place surface.
Water Pressure and Pressure Forces
Water Pressure and Pressure Force (Revision)
Hinge Statics ? Surface Forces.
Static Equilibrium And Elasticity (Keseimbangan Statik dan Kekenyalan)
Static Surface Forces hinge water ? 8 m 4 m . Static Surface Forces ä Forces on plane areas ä Forces on curved surfaces ä Buoyant force ä Stability submerged.
Static Surface Forces hinge 8 m water ? 4 m.
Monroe L. Weber-Shirk S chool of Civil and Environmental Engineeringhinge ? Statics Surface Forces 
It is represented by CG. or simply G or C.
Chapter 14 Fluids Key contents Description of fluids
1 MECH 221 FLUID MECHANICS (Fall 06/07) Chapter 2: FLUID STATICS Instructor: Professor C. T. HSU.
Hinge Statics ? Surface Forces.
Fluid mechanics 3.1 – key points
Ch2 Fluid Statics Fluid either at rest or moving in a manner that there is no relative motion between adjacent particles. No shearing stress in the fluid.
Hydrostatic Pressure distribution in a static fluid and its effects on solid surfaces and on floating and submerged bodies. Fluid Statics M. Bahrami ENSC.
Forces Due to Static Fluid
Fluid Statics Lecture -3.
Engineering Mechanics: Statics
Engineering Mechanics: Statics
Force on Floating bodies:
Motivation for Studying Fluid Mechanics
E Construction Surveying HYDRAULICS. Introduction surveyors –usually not be directly involved in the design of hydraulics systems –most certainly.
Engineering Mechanics: Statics
Pressure at a Point: Pascal’s Law
Chapter 3: Pressure and Fluid Statics
CE 1501 CE 150 Fluid Mechanics G.A. Kallio Dept. of Mechanical Engineering, Mechatronic Engineering & Manufacturing Technology California State University,
The center of gravity of a rigid body is the point G where a single force W, called the weight of the body, can be applied to represent the effect of the.
10.7 Moments of Inertia for an Area about Inclined Axes
Chapter 12 Static Equilibrium and Elasticity. Static Equilibrium Equilibrium implies that the object moves with both constant velocity and constant angular.
FLUID STATICS: Hydrostatic Force on Plane Surfaces slide 18.
Fluid Mechanics and Applications MECN 3110
Water Pressure and Pressure Force (Revision) The Islamic University of Gaza Faculty of Engineering Civil Engineering Department Hydraulics - ECIV 3322.
Chapter 14 Fluids What is a Fluid? A fluid, in contrast to a solid, is a substance that can flow. Fluids conform to the boundaries of any container.
FLUID STATICS HYDROSTATIC FORCES AND BUOYANCY
FLUID STATICS: Hydrostatic Force on Plane Surfaces slide 18.
Chapter 15FLUIDS 15.1 Fluid and the World Around Us 1.A fluid is a substance that cannot support a shearing stress. 2.Both gases and liquids are fluids.
9.6 Fluid Pressure According to Pascal’s law, a fluid at rest creates a pressure ρ at a point that is the same in all directions Magnitude of ρ measured.
MOMENT OF INERTIA Today’s Objectives: Students will be able to: 1.Determine the mass moment of inertia of a rigid body or a system of rigid bodies. In-Class.
Dr. Kamel Mohamed Guedri Umm Al-Qura University, Room H1091
Static Equilibrium and Elasticity
Abj : Pressure, Pressure Force, and Fluid Motion Without Flow [Q1] 1.Area as A Vector  Component of Area Vector – Projected Area  Net Area Vector.
Chapter 14 Fluids.
§2.9 Pressure Prism Area of the plane is rectangular
Ship Computer Aided Design Displacement and Weight.
Theoretical Mechanics STATICS KINEMATICS
Copyright © Cengage Learning. All rights reserved. 8 Further Applications of Integration.
Mecânica de Fluídos Ambiental 2015/2016
Objectives  Introduce the concept of pressure;  Prove it has a unique value at any particular elevation;  Show how it varies with depth according.
Chapter 12 Lecture 21: Static Equilibrium and Elasticity: I HW8 (problems):11.7, 11.25, 11.39, 11.58, 12.5, 12.24, 12.35, Due on Friday, April 1.
SHREE SA’D VIDYA MANDAL INSTITUTE OF TECHNOLOGY DEPARTMENT OF CIVIL ENGINEERING.
Water Pressure and Pressure Force (Revision)
Introduction to Fluid Mechanics
STATICS (ENGINEERING MECHANICS-I)
FLUID MECHANICS 1.1 HYDROSTATIC FORCES.
Chapter Objectives Chapter Outline
ENGINEERING MECHANICS
Statics Course Code: CIVL211 FRICTION Dr. Aeid A. Abdulrazeg.
FLUID STATICS Yosua Heru Irawan Lecture slides by
Presentation transcript:

Pressure distribution in a fluid Pressure and pressure gradient Lecture 4 Mecânica de Fluidos Ambiental 2015/2016

Chapter 2 Concept of pressure and pressure gradient Hydrostatic pressure distribution Hydrostatic forces Buoyance and stability Mecânica de Fluidos Ambiental 2015/2016

Forces in fluids Surface or volumetric (or mass) Surface forces can be normal (pressure) or tangential (friction) Friction Forces are always parallel to velocity. This is why they are often called “tangential forces”. Their equation can be complex if velocity is not parallel to any reference axis. Mecânica de Fluidos Ambiental 2015/2016

Pressure Many fluid problems do not involve motion. They concern the pressure distribution in a static fluid and its effect on solid surfaces and on floating and submerged bodies. Fluids at rest cannot support shear stress. Pressure is used to indicate the normal force per unit of area at a given point acting on a given plane within the fluid mass of interest. How the pressure at a point varies with the orientation of the plane passing through the point? Mecânica de Fluidos Ambiental 2015/2016

Pressure at a point Small wedge (“pequena cunha”) of fluid at rest of size  x by  z by  s and depth b into the paper. There is no shear by definition, but we postulate that the pressures p x, p z, and p n may be different on each face The weight of the element also may be important. The element is assumed small, so the pressure is constant on each face. Summation of forces must equal zero (no acceleration) in both the x and z directions. Mecânica de Fluidos Ambiental 2015/2016

Pressure at a point Mecânica de Fluidos Ambiental 2015/2016

Pressure force in fluid element Mecânica de Fluidos Ambiental 2015/2016

Equilibrium of fluid element Mecânica de Fluidos Ambiental 2015/2016 Weight=  g(dxdydz)

Equilibrium of fluid element Mecânica de Fluidos Ambiental 2015/2016

General equation Mecânica de Fluidos Ambiental 2015/2016

Hydrostatic pressure Mecânica de Fluidos Ambiental 2015/2016

Hydrostatic pressure Mecânica de Fluidos Ambiental 2015/2016

Efect of variable gravity Mecânica de Fluidos Ambiental 2015/2016

Hydrostatic pressure in liquids Mecânica de Fluidos Ambiental 2015/2016

Hidrostatic pressure distribution Mecânica de Fluidos Ambiental 2015/2016

Hydrostatic pressure in gases Mecânica de Fluidos Ambiental 2015/2016

Hydrostatic forces on plane surfaces Objective: compute the hydrostatic force over flat and curve surfaces and the application point (center of pressure). When a surface is submerged in a fluid, forces develop on the surface due to the fluid. The determination of these forces is important in the design of storage tanks, ships, dams, and other hydraulic structures. Mecânica de Fluidos Ambiental 2015/2016

Hydrostatic forces on plane surfaces Plane panel of arbitrary shape completely submerged in a liquid Panel plane makes an arbitrary angle  with the horizontal free surface, so that the depth varies over the panel surface. If h is the depth to any element area dA of the plate, from hydrostatic pressure equation in liquids the pressure there is p=p a +  h. Mecânica de Fluidos Ambiental 2015/2016

Hydrostatic forces on plane surfaces Mecânica de Fluidos Ambiental 2015/2016

Therefore, since  is constant along the plate, becomes Finally, unravel this by noticing that, the depth straight down from the surface to the plate centroid. Thus The force on one side of any plane submerged surface in a uniform fluid equals the pressure at the plate centroid times the plate area, independent of the shape of the plate or the angle  at which it is slanted. Mecânica de Fluidos Ambiental 2015/2016

Center of pressure However, to balance the bending-moment portion of the stress, the resultant force F acts not through the centroid but below it toward the high-pressure side. Its line of action passes through the center of pressure CP of the plate (see figure). To find the coordinates (x CP, y CP ), we sum moments of the elemental force p dA about the centroid and equate to the moment of the resultant F. To compute y CP, we equate I xx is the area moment of inertia of the plate area about its centroidal x axis Mecânica de Fluidos Ambiental 2015/2016 Vanishes by def. of centroidal axes

Center of pressure The negative sign shows that y CP is below the centroid at a deeper level (below the gravity center) and, unlike F, depends on angle . The determination of x CP is exactly similar: I xy the product of inertia of the plate, again computed in the plane of the plate If I xy = 0, usually implying symmetry, x CP = 0 and the center of pressure lies directly below the centroid on the y axis. Mecânica de Fluidos Ambiental 2015/2016

In most cases the ambient pressure p a is neglected because it acts on both sides of the plate; for example, the other side of the plate is inside a ship or on the dry side of a gate or dam. In this case p CG =  h CG, and the center of pressure becomes independent of specific weight: Mecânica de Fluidos Ambiental 2015/2016

Resume Mecânica de Fluidos Ambiental 2015/2016