Apr 16 Discussions Hydraulic equilibrium Pressure and depth.

Slides:



Advertisements
Similar presentations
Pressure in fluids.
Advertisements

Phys 250 Ch10 p1 Chapter 10: Fluids Fluids: substances which flow Liquids: take the shape of their container but have a definite volume Gases: take the.
Phy 212: General Physics II Chapter 14: Fluids Lecture Notes.
Copyright © by Holt, Rinehart and Winston. All rights reserved. ResourcesChapter menu Buoyant Force Buoyant force is the upward force exerted on an object.
Liquids and Gasses Matter that “Flows”
Chapter 8 Forces in Fluids
Pharos University ME 259 Fluid Mechanics for Electrical Students Revision for Mid-Term Exam Dr. A. Shibl.
Fluids Gases (compressible) and liquids (incompressible) – density of gases can change dramatically, while that of liquids much less so Gels, colloids,
Oct. 29, 2001 Dr. Larry Dennis, FSU Department of Physics1 Physics 2053C – Fall 2001 Chapter 10 Fluids.
Physics 203 College Physics I Fall 2012
Chapter 3 Section 2 Notes. Fluid  Any substance that has the ability to flow (move on its own) Two States ○ ____________  Can flow because their particles.
General idea:  The column of air exerts a force on the surface of the earth.  This force per area is as large as 1.03x10 5 Pa at sea level, also known.
AP Physics II.A – Fluid Mechanics.
Fluids & Bernoulli’s Equation Chapter Flow of Fluids There are two types of flow that fluids can undergo; Laminar flow Turbulent flow.
Fluid Statics.
Phy 202: General Physics II Ch 11: Fluids. Daniel Bernoulli ( ) Swiss merchant, doctor & mathematician Worked on: –Vibrating strings –Ocean tides.
Fluid Mechanics Chapter 10.
Hydraulic Pumps and Cylinders
Pressure. Solids, Liquids, and Gases  Solid IncompressibleIncompressible Subject to shear forceSubject to shear force  Gas Compressible Not subject.
Pgs  Calculate the pressure exerted by a fluid.  Explain Pascal’s Principle.  Calculate how pressure varies with depth in a fluid.
Terms Density Specific Gravity Pressure Gauge Pressure
© Shannon W. Helzer. All Rights Reserved. Unit 14 Fluid.
AP Physics II.A – Fluid Mechanics.
Chapter 11 Fluids. Density and Specific Gravity The density ρ of an object is its mass per unit volume: The SI unit for density is kg/m 3. Density is.
Warm-up Pick up the free response at the door and begin working on it.
Pressure. Solids, Liquids, and Gases  Solid IncompressibleIncompressible Subject to shear forceSubject to shear force  Gas Compressible Not subject.
Physics 203 – College Physics I Department of Physics – The Citadel Physics 203 College Physics I Fall 2012 S. A. Yost Chapter 10 Part 1 Pressure, Archimedes.
Pressure; Pascal’s Principle
Physics 221 Department of Physics The Citadel Lecture Notes S. Yost November 17, 2008 Hydrostatics: Pressure and Pascal’s Law.
1 Outline Review Pressure and Density. Begin Buoyant Forces. Continuity Equation. Bernoulli’s Principle. CAPA and Examples.
Goal: To understand liquids and gasses Objectives: 1)To understand Pressure 2)To understand Buoyancy 3)To understand Archimedes Principal 4)To learn about.
L 13 Fluids [2]: Statics  fluids at rest  More on fluids.  How can a steel boat float.  A ship can float in a cup of water!  Today’s weather Today’s.
Fluids.
Goal: To understand liquids and gasses Objectives: 1)To understand Pressure 2)To understand Buoyancy 3)To understand Archimedes Principal 4)To learn about.
Pressure is in Force per unit area F = Force in N A = Area in m 2 P = pressure in N/m 2 (Pascals - Pa)
Pressure and Fluids § 12.1–12.3. Density Relating “how big” to “how much” § 12.1.
14.2 Essential Questions What is Archimedes’ principle?
Physics 1B03summer-Lecture 12 1 Survey + $150 !!! The Faculty of Science is conducting an online survey to help us better understand your educational and.
Solids and Fluids Chapter 9. Phases of Matter  Solid – definite shape and volume  Liquid – definite volume but assumes the shape of its container 
L 13 Fluids [2]: Statics  fluids at rest  More on fluids.  How can a steel boat float.  A ship can float in a cup of water!  Today’s weather Today’s.
Fluids Honors Physics. Liquids In a liquid, molecules flow freely from position to position by sliding over each other Have definite volume Do not have.
Chapter 9.1 Review Fluids. 1. What are the properties of a fluid? What states of matter are fluids?
CHAPTER 9 Solids and Fluids Fluid Mechanics (only) pages
Formative Assessment. 1a. Convert Torr absolute to gauge pressure psi. (11.2 psi gauge ) 1.00 atm = 1.013x10 5 Pa = kPa = 760. Torr = 14.7.
Unit 7: Pressure MC Textbook Chp 7 GLM Red Book Chp 6.
Pressure and Fluids § 15.1–15.5. Density Relating “how big” to “how much” § 15.1.
Chapter 7 Forces in Fluids.
L 13 Fluids [2]: Statics  fluids at rest  More on fluids.  How can a steel boat float.  A ship can float in a cup of water!  Today’s weather Today’s.
Wednesday, Apr. 14, 2004PHYS , Spring 2004 Dr. Jaehoon Yu 1 PHYS 1441 – Section 004 Lecture #20 Wednesday, Apr. 14, 2004 Dr. Jaehoon Yu Variation.
PHYSICS OF FLUIDS.
Pascal’s Principle Contents: How to calculate Whiteboards.
L 13 Fluids [2]: Statics  fluids at rest  More on fluids at rest  How is atmospheric pressure measured?  Today’s weather Today’s weather Today’s weather.
Today (Chapter 10, Fluids)  Review for Exam 2 Tomorrow (Chapters 6-10)  Review Concepts from Tuesday  Continuity Equation  Bernoulli’s Equation  Applications/Examples.
Why does he need to equalise his ears on the way down? What would happen if he just shot up to the surface from 20m down?
Pressure 1 Pa = 1 Nm-2 Pressure is defined as force per unit area.
Bernoulli and Flow Continuity.  U-Tube Manometer  Used to measure pressure of a fluid  Principles involved: ◦ The pressure is the same in equal elevations.
Phys 250 Ch10 p1 Chapter 10: Fluids Fluids: substances which flow Liquids: take the shape of their container but have a definite volume Gases: take the.
Day 63, Wednesday, 2 December, 2015 Fluid Mechanics Problems Quick review Pressure, Pascal’s Principle, Archimedes's principle, Pressure at depth Problems.
Hydrostatics and Fluid Dynamics
Chapter 11 Fluids.
Fluids Objectives: Pressure inside fluids Hydraulic Lift
FLUIDS Pressure (P = F/A) The relationship is → P = Po + gh
When you catch a deep-sea fish, why does its eyes pop-out?
Physics 21.
DENSITY AND PRESSURE.
When you catch a deep-sea fish, why does its eyes pop-out?
 water at 4° C = x 103 kg/m3 SI unit = kg/m3  varies with temperature and pressure Significantly for gases Not much for liquids or solids.
FLUIDS A fluid is any substance that flows and conforms to the boundaries of its container. A fluid could be a gas or a liquid. An ideal fluid is assumed.
Warm-up Page 83, 1. All fluids exert a __________. pressure Page 83, 2. The equation for pressure is: Pressure = force/area Page 83, 3. The SI unit for.
Chapter 11 Fluids.
Presentation transcript:

Apr 16 Discussions Hydraulic equilibrium Pressure and depth

Q1: Pressure Which of the following situations represents the greatest pressure? (Recall that P=F/A) A) the weight of 10 tons on 1.0 square meter B) the weight of 100 kg on 100 square centimeters C) the weight of 1.0 kg on 1.0 square centimeter D) the force of your pencil (say, 1 Newton) on its point

Q1: Pressure Which of the following situations represents the greatest pressure? (Recall that P=F/A) D) the force of your pencil (say, 1 Newton) on its point: P = F/A = (1 N)/(1 mm) 2 =10 6 Pa?

P1: Hydraulic lift Because of your physics knowledge, you are asked to advise on the design of a hydraulic lift in a car repair garage that must be able to hold a 3 ton vehicle. The piston that supports the vehicle platform has a diameter of 30 cm and a mass of 1 ton. A pump pushes fluid into the piston’s cylinder through a 3 cm diameter pipe. What is the minimum pressure that needs to be exerted on the bottom of the piston to support the vehicle? What is the minimum force that the piston on the pump needs to exert on the fluid entering the pipe to hold the vehicle in place? F W Use g=10 m/s 2

Hydraulic lift-2 The force the large piston supports is its own weight plus the weight of the vehicle (4 ton=4000 kg): W tot =m tot g = (4000 kg)(10 m/s 2 )=40 kN P = W tot /A = (40 kN)/(  (0.15 m) 2 )=5.7x10 5 Pa The small piston needs to be able to sustain this pressure. The force necessary is: F = PA pipe = (5.7x10 5 Pa)(  (0.015 m) 2 )=400 N Another way to see this is that since the pipe has 1/100 of the cross-sectional area of the large piston, the necessary force is 1/100 of the total weight (40 kN)/100 = 0.4 kN = 400 N. Note that this is about 90 lb.

P2: Pressure below the surface You are designing a deep sea exploration vessel. From P201 you recall that pressure increases as you go beneath the surface of the ocean, the pressure of the atmosphere at sea level is approximately 100 kPa, and the density of water is 1025 kg/m 3. What pressure does your vessel need to withstand if it is to reach at the deepest part of the ocean (about 10 km deep)? Metals such as titanium have compressive strengths over 500 MPa, but metals are not transparent and you want your vessel to have a window. Glass has a compressive strength of approximately 50 MPa. What do you recommend about providing the ability to pressurize your vessel?

Pressure below the surface-2 The pressure is  gd+Po =(1025 kg/m 3 )(10 m/s 2 )(10000m)=10 8 N/m 2 =100 MPa (about 1000 atm), since every 10 meter of depth is equivalent to an extra atmosphere-equivalent of pressure. Your window will not be able to withstand this unless you pressurize your vessel to over 50 MPa (so the pressure difference is less than 50 MPa). It would be best to do this gradually on the way down (you don’t want it to be 50 MPa internally at the surface, since your window would blow out!)

P3: Water Supply 1 Water supplies are pressurized for several reasons, but to provide sufficient flow, they need to be pressurized. A city is to have a 24-inch (60 cm) diameter supply line that is to provide 20 million gallon/day of flow (3.75 liter = 1gallon). What flow velocity is needed? According to Bernoulli’s Law, what is the minimum pressure drop between the storage tank and the entrance to the pipe needed to produce this velocity?

Water supply-1 The volume flow rate= 20x10 6 gal/day(3.75 liter/gal)(1 m 3 /1000 liter) =75x10 3 m 3 /day(1 day/86400 s)=0.87 m 3 /s =Av flow =  (0.30 m) 2 v flow v flow =3.1 m/s The pressure must obey: P tank =P pipe +(1/2)  v 2 The pressure drop is: P tank -P pipe =(1/2)  v 2 =(1/2)(1000 kg/m 3 )(3.1 m/s) 2 =5000 Pa

Water supply-2 The end of the city water supply pipe is 60 meter above the entrance to the pipe. A pump provides the necessary pressure. What pressure is required at the exit of the pump for the water to reach city, if the pressure at the city end needs to be at least 200 kPa?

Water supply-2 The end of the city water supply pipe is 60 meter above the entrance to the pipe. A pump provides the necessary pressure. What pressure is required at the exit of the pump for the water to reach city, if the pressure at the city end needs to be at least 200 kPa? P pump +  gh pump =P city +  gh city P pump =P city +  g(h city -h pump ) =(200 kPa)+(1000 kg/m 3 )(10 m/s 2 )(60 m)=800 kPa