MEE2026 FLUID MECHANICS − Chapter III − Fluid Statics Dokuz Eylül University MA Ezan, A Erek, E Alptekin Department of Mechanical Engineering makina.deu.edu.tr /school/deumak Fluid Mechanics − Chapter III: Fluid Statics Ezan, Erek, Alptekin Content of the Course Chapter 1: Foundations Chapter 2: Fluid Properties Chapter 3: Fluid Statics Chapter 4 / Part I: Fluid in Rigid Body Motion Chapter 4 / Part II: Flowing Fluids – Fluid Kinematics Chapter 4 / Part III: Bernoulli Equation Chapter 5: Control Volume Approach & Continuity Chapter 6: Momentum Equation Chapter 7: The Energy Equation Chapter 8: Dimensional Analysis & Similitude Chapter 9: Flow in Conduits Fluid Mechanics − Chapter III: Fluid Statics 2 || 36 Ezan, Erek, Alptekin Objectives of Chapter III Describing the Pressure Absolute pressure, Gage pressure Pressure Variation with Elevation Hydrostatic Differential Equation, Piezometric Pressure / Head Measuring Pressure Barometer, Bourdon-Gage, Piezometer, Manometer, Transducers Predicting Forces on PLANE Surfaces Resultant Force, Centroid, Center of Pressure Fluid Mechanics − Chapter III: Fluid Statics 3 || 36 Ezan, Erek, Alptekin Pressure – Definition Pressure is defined as a normal force exerted by a fluid per unit area Pressure is a scalar quantity, not a vector; the pressure at a point in a fluid is the same in all directions The pressure at a point in a fluid at rest is independent of direction Blaise Pascal (1623– 1662) Fluid Mechanics − Chapter III: Fluid Statics 4 || 36 Ezan, Erek, Alptekin Pressure at a Point – Pascal’s Law “the pressure at a point in a fluid at rest, or in motion, is independent of direction as long as there are no shearing stresses present” WHY? PROOF y-direction z-direction from geometry Fluid Mechanics − Chapter III: Fluid Statics 5 || 36 Ezan, Erek, Alptekin Pressure at a Point – Pascal’s Law “the pressure at a point in a fluid at rest, or in motion, is independent of direction as long as there are no shearing stresses present” WHY? PROOF y-direction z-direction Considering a point δx, δy, and δz approach to zero, so that or, Fluid Mechanics − Chapter III: Fluid Statics 6 || 36 Ezan, Erek, Alptekin Gage Pressure vs. Absolute Pressure Fluid Mechanics − Chapter III: Fluid Statics 7 || 36 Ezan, Erek, Alptekin Hydraulic Machinery Fluid Mechanics − Chapter III: Fluid Statics 8 || 36 Ezan, Erek, Alptekin PROBLEM 1 – Describing the Pressure The Crosby gage tester shown in the figure is used to calibrate or to test pressure gages. When the weights and the piston together weigh 140 N, the gage being tested indicates 200 kPa. If the piston diameter is 30 mm, what percentage of error exists in the gage? Fluid Mechanics − Chapter III: Fluid Statics 9 || 36 Ezan, Erek, Alptekin Pressure Variation inside a Fluid – Derivation Pressure Variation in a Fluid at Rest Since p depends only on z Fluid Mechanics − Chapter III: Fluid Statics 10 || 36 Ezan, Erek, Alptekin Pressure Variation inside a Fluid – Incompressible Incompressible Fluid The quantity p/γ is a length called the pressure head of the fluid HEAD: The height of a column of fluid of specific weight - γ - required to give a pressure difference of (p1 - p2) Fluid Mechanics − Chapter III: Fluid Statics 11 || 36 Ezan, Erek, Alptekin Exercise 1 – Comparing Pressures Different Sections Fluid Mechanics − Chapter III: Fluid Statics 12 || 36 Ezan, Erek, Alptekin PROBLEM 2 – Absolute vs. Gage Pressure Consider the two tanks shown in Figure. Both tanks are pressurized, with one tank partially filled with gasoline at 20°C and the other tank filled with air at 20°C. The measured gauge pressures at A and B are 80 kPa and 130 kPa, respectively, when the atmospheric pressure is 100 kPa. What is the absolute pressure at A and B? Estimate the gauge pressures at C and D. If atmospheric pressure changes to 80 kPa, what will be the gauge pressures at A, B, C, and D? Fluid Mechanics − Chapter III: Fluid Statics 13 || 36 Ezan, Erek, Alptekin Pressure Variation inside a Fluid – Compressible Pressure variation inside a fluid is defined as follows; Let's consider Ideal-Gases as compressible fluid. The specific weight of an Ideal-Gas could be defined in terms of density and temperature as, Combine equations to obtain: Considering iso-thermal condition, integration yields, Fluid Mechanics − Chapter III: Fluid Statics 14 || 36 Ezan, Erek, Alptekin Pressure Variation inside a Fluid – Liquid vs. Gas Water Air Pressure variation along depth Pressure variation along height Fluid Mechanics − Chapter III: Fluid Statics 15 || 36 Ezan, Erek, Alptekin Pressure Variation inside a Fluid – Compressible Fluid Mechanics − Chapter III: Fluid Statics 16 || 36 Ezan, Erek, Alptekin Pressure Variation inside a Fluid – Compressible Fluid Mechanics − Chapter III: Fluid Statics 17 || 36 Ezan, Erek, Alptekin Standard Sea-level Conditions of Air Fluid Mechanics − Chapter III: Fluid Statics 18 || 36 Ezan, Erek, Alptekin PROBLEM 3 – Pressure variation of air In 2010, the Burj Khalifa skyscraper, was completed and opened in the United Arab Emirates. The final height of the building, which had remained a secret until completion, is 828 m. Estimate the ratio of the pressure at the top of the building to the pressure at its base, assuming the air to be at a common temperature of 15°C. Compare the pressure calculated in part (a) with that obtained by assuming the air to be incompressible with values for air at standard sea level conditions. Fluid Mechanics − Chapter III: Fluid Statics 19 || 36 Ezan, Erek, Alptekin Measuring Pressure – Barometer Evangelista Torricelli (1608– 1647) Fluid Mechanics − Chapter III: Fluid Statics 20 || 36 Ezan, Erek, Alptekin Measuring Pressure – Barometer Fluid Mechanics − Chapter III: Fluid Statics 21 || 36 Ezan, Erek, Alptekin Measuring Pressure – Manometer Manometers use vertical or inclined liquid columns to measure pressure Simple U-Tube Manometer Piezometer Tube Fluid Mechanics − Chapter III: Fluid Statics 22 || 36 Ezan, Erek, Alptekin Measuring Pressure – Manometer Manometers use vertical or inclined liquid columns to measure pressure Differential U-tube Manometer Fluid Mechanics − Chapter III: Fluid Statics Inclined-tube Manometer 23 || 36 Ezan, Erek, Alptekin Measuring Pressure – Bourdon Gage & Transducers Bourdon Gage Fluid Mechanics − Chapter III: Fluid Statics 24 || 36 Ezan, Erek, Alptekin PROBLEM 4 – Manometer A closed tank contains compressed air and oil (SGoil = 0.90) as is shown in Fig. A U-tube manometer using mercury (SGHg = 13.6) is connected to the tank as shown. The column heights are h1 = 36 in. (0.9144 m), h2 = 6 in. (0.1524 m), and h3 = 9 in. (0.2286 m). Determine the pressure reading (in kPa) of the gage. Fluid Mechanics − Chapter III: Fluid Statics 25 || 36 Ezan, Erek, Alptekin PROBLEM 5 – Manometer The ratio of container diameter to tube diameter is 10. When air in the container is at atmospheric pressure, the free surface in the tube is at position 1. When the container is pressurized, the liquid in the tube moves 1 m up the tube from position 1 to position 2. What is the container pressure that causes this deflection? The liquid specific weight is 7850 N/m3. Fluid Mechanics − Chapter III: Fluid Statics 26 || 36 Ezan, Erek, Alptekin Forces on Plane Surfaces (Panels) UNIFORM PRESSURE DISTRIBUTION For a uniform pressure distribution, the CP (Center of Pressure) is located at the centroid of area of the panel… Fluid Mechanics − Chapter III: Fluid Statics 27 || 36 Ezan, Erek, Alptekin Forces on Plane Surfaces (Panels) HYDROSTATIC PRESSURE DISTRIBUTION Notice that the CP is located below the centroid of area Fluid Mechanics − Chapter III: Fluid Statics 28 || 36 Ezan, Erek, Alptekin Forces on Plane Surfaces (Panels) HYDROSTATIC PRESSURE DISTRIBUTION Magnitude of Resultant Hydrostatic Force Fluid Mechanics − Chapter III: Fluid Statics 29 || 36 Ezan, Erek, Alptekin Forces on Plane Surfaces (Panels) HYDROSTATIC PRESSURE DISTRIBUTION Line of Action of the Resultant Force Fluid Mechanics − Chapter III: Fluid Statics 30 || 36 Ezan, Erek, Alptekin Forces on Plane Surfaces (Panels) CENTROIDS AND MOMENTS OF INERTIA OF PLANE AREAS Fluid Mechanics − Chapter III: Fluid Statics 31 || 36 Ezan, Erek, Alptekin PROBLEM 6 – Gate A rectangular gate is hinged at the water line, as shown. The gate is 1.2 m high and 1.8 m wide. The specific weight of water is 9810 N/m3. Find the necessary force (in kN) applied at the bottom of the gate to keep it closed. 0.3 m 1.2 m Fluid Mechanics − Chapter III: Fluid Statics 32 || 36 Ezan, Erek, Alptekin PROBLEM 7 – Gate An elliptical gate covers the end of a pipe 4 m in diameter. If the gate is hinged at the top, what normal force F is required to open the gate when water is 8 m deep above the top of the pipe and the pipe is open to the atmosphere on the other side? Neglect the weight of the gate. Fluid Mechanics − Chapter III: Fluid Statics 33 || 36 Ezan, Erek, Alptekin Buoyancy – Definition BUOYANT FORCE The buoyant force equals the weight of liquid that would be needed to occupy the volume This volume is called the displaced volume A body partially submerged in a liquid. Fluid Mechanics − Chapter III: Fluid Statics A body immersed in a liquid. 34 || 36 Ezan, Erek, Alptekin PROBLEM 8 – Hydrometer If the hydrometer shown sinks 5.3 cm in water (15°C) and the stem sinks 6.3 cm in oil (z = 6.3 cm), what is the specific gravity of the oil? Note that the bulb volume is 1.0 cm3, and the stem area is 0.1 cm2. Fluid Mechanics − Chapter III: Fluid Statics 35 || 36 Ezan, Erek, Alptekin PROBLEM 9 – Buoyancy Determine the minimum volume of concrete (γ = 23.6 kN/m3) needed to keep the gate (1 m wide) in a closed position, with l = 2 m. Note that the hinge is at the bottom of the gate. Fluid Mechanics − Chapter III: Fluid Statics 36 || 36 Ezan, Erek, Alptekin