Physics 101: Lecture 17 Fluids

Similar documents
PHYSICS 220 Lecture 16 Fluids Textbook Sections

States of Matter. Pressure PHYSICS 220. Illustration. Lecture 16. Fluids. Solid. Liquid. Gas. Pressure = F normal / A

Physics 101: Lecture 18 Fluids II

Physics 220: Classical Mechanics

Page 1. Physics 131: Lecture 23. Today s Agenda. Announcements. States of Matter

Phy 212: General Physics II. Daniel Bernoulli ( )

Physics 201 Chapter 13 Lecture 1

Physics 220: Classical Mechanics

TOPICS. Density. Pressure. Variation of Pressure with Depth. Pressure Measurements. Buoyant Forces-Archimedes Principle

Chapter 9: Solids and Fluids

Fluids. Fluid = Gas or Liquid. Density Pressure in a Fluid Buoyancy and Archimedes Principle Fluids in Motion

Physics 207 Lecture 18

Chapter 10. Solids & Liquids

CHAPTER 13. Liquids FLUIDS FLUIDS. Gases. Density! Bulk modulus! Compressibility. To begin with... some important definitions...

Physics 201 Chapter 13 Lecture 1

Liquids CHAPTER 13 FLUIDS FLUIDS. Gases. Density! Bulk modulus! Compressibility. To begin with... some important definitions...

Chapter 15: Fluid Mechanics Dynamics Using Pascal s Law = F 1 = F 2 2 = F 2 A 2

Nicholas J. Giordano. Chapter 10 Fluids

Final Mock Exam PH 221-1D

Physics 123 Unit #1 Review

Fluid Mechanics. Chapter 14. Modified by P. Lam 6_7_2012

EXAM 1 PHYS 103 FALL 2011 A NAME: SECTION

Physics 201, Lecture 26

11/4/2003 PHY Lecture 16 1

There are three phases of matter: Solid, liquid and gas

States of Matter. Physics 201, Lecture 25. Density ρ. Fluids

Pressure in a fluid P P P P

Chapter 15: Fluids. Mass Density = Volume. note : Fluids: substances which flow

Mock Exam III PH 201, PH 221

Types of Forces. Pressure Buoyant Force Friction Normal Force

Physics 207 Lecture 20. Chapter 15, Fluids

Fluids, Continuity, and Bernouli

Figure 1 Answer: = m

Lecture 8 Equilibrium and Elasticity

Chapter 12. Fluid Mechanics. A. The density ρ of a substance of uniform composition is defined as its mass M divided by its volume V.

States of Matter. Chapter 9 Solids and Fluids. Solids: Stress and Strain. Solids: Stress and Strain. Stress = Force Area. Strain =!L L. Example 9.

States of Matter. Chapter 9 Solids and Fluids. Solids: Stress and Strain. Solids: Stress and Strain. Stress = Force Area. Strain =!

Chapter 15. m. The symbolic equation for mass density is: ρ= m V. Table of Densities

DEVIL PHYSICS THE BADDEST CLASS ON CAMPUS IB PHYSICS

11.1 Mass Density. Fluids are materials that can flow, and they include both gases and liquids. The mass density of a liquid or gas is an

Chapter 14. Lecture 1 Fluid Mechanics. Dr. Armen Kocharian

Chapter 14. Fluid Mechanics

DENSITY OF AN IRREGULAR SHAPED OBJECT

43. A person sits on a freely spinning lab stool that has no friction in its axle. When this person extends her arms,

Chapter 9. Solids and Fluids. 1. Introduction. 2. Fluids at Rest. 3. Fluid Motion

Chapter 2. States of Matter

Chapter 9 Solids and Fluids. Elasticity Archimedes Principle Bernoulli s Equation

Jordan University of Science & Technology PHYS 101A Final exam First semester 2007

CHAPTER 4 - STATES OF MATTER. Mr. Polard Physical Science Ingomar Middle School

Exam I Physics 101: Lecture 08 Centripetal Acceleration and Circular Motion Today s lecture will cover Chapter 5 Exam I is Monday, Oct. 7 (2 weeks!

Welcome to: Physics I. I m Dr Alex Pettitt, and I ll be your guide!

Physics 110 Third Hour Exam

Physics 201 Lecture 16

Physics 17 Exam #3 November 9, 2009

States of matter. Density high > high >> low (pressure dependent)

Kinematics + Dynamics

m V DEFINITION OF MASS DENSITY The mass density of a substance is the mass of a substance divided by its volume: SI Unit of Mass Density: kg/m 3

Physics 111. Thursday, November 11, 2004

TALLER DE HIDROSTÁTICA

UNIT D: MECHANICAL SYSTEMS

Physics 101: Lecture 08 Centripetal Acceleration and Circular Motion

Chapter: States of Matter

MECHANICAL PROPERTIES OF FLUIDS

Chapter 14 - Fluids. -Archimedes, On Floating Bodies. David J. Starling Penn State Hazleton PHYS 213. Chapter 14 - Fluids. Objectives (Ch 14)

You are responsible for recording your 9 digit PSU Student ID on your scantron form

Final Review, Day 1. Announcements: Web page:

Physics 2c Lecture 9. Recap of Entropy. First part of chapter 18: Hydrostatic Equilibrium Measuring Pressure Pascal's Law Archimedes Principle

Locations by Lab Instructor. Pressure in an oil well. PHYSICS 220 Evening Exam 2. Lecture 18. Fluid Dynamics. See Home Page For lab hours

Announcements 1 Oct 2013

Physics 106 Lecture 13. Fluid Mechanics

Welcome back to Physics 211

Today s lecture. WEST VIRGINIA UNIVERSITY Physics

Physics 153 Introductory Physics II. Week One: FLUIDS. Dr. Joseph J. Trout

CHAPTER 10- GRAVITATION

Chapter 11. Fluids. continued

States of Matter Unit

Physics 107 HOMEWORK ASSIGNMENT #9

Your Comments. Nutcracker

b) (6) What is the volume of the iron cube, in m 3?

Physics - Fluids. Read Page 174 (Density) TQ1. A fluid is what type of matter? TQ2. What is fluid mechanics? TQ3. What is the equation for density?

Fluid Mechanics. Chapter 12. PowerPoint Lectures for University Physics, Thirteenth Edition Hugh D. Young and Roger A. Freedman

University Physics 226N/231N Old Dominion University. Ch 12: Finish Fluid Mechanics Exam Review

Physics 101: Lecture 15 Torque, F=ma for rotation, and Equilibrium

Chapter 9 Fluids. Pressure

All questions are of equal value. No marks are subtracted for wrong answers.

13.7 Power Applied by a Constant Force

PHYSICS HYDROSTATICS FORM 5

Physics 211: Lecture 14. Today s Agenda

Today s Discussion: Fluids Pressure and Pascal s principle Bouyancy, Archimedes principle Bernoulli s equation

Fluid Mechanics. The atmosphere is a fluid!

If we change the quantity causing the deformation from force to force per unit area, we get a relation that does not depend on area.

Review Chapters 1-9. Did you read the article on helmets before coming to class? A. Yes B. No

Fluid dynamics - Equation of. continuity and Bernoulli s principle.

Chapter 12: Gravity, Friction, & Pressure Physical Science, McDougal-Littell, 2008

Section 1 Matter and Energy

UNIVERSITY OF SASKATCHEWAN Department of Physics and Engineering Physics

EQUILIBRIUM OBJECTIVES PRE-LECTURE

Fluid Mechanics. If deformation is small, the stress in a body is proportional to the corresponding

Physics 101: Lecture 13 Rotational Kinetic Energy and Rotational Inertia. Physics 101: Lecture 13, Pg 1

UNIVERSITY OF SASKATCHEWAN Department of Physics and Engineering Physics

Transcription:

Exam III Physics 101: Lecture 17 Fluids Exam 2 is Mon Nov. 4, 7pm Extra office hours on Fri. (see webpage!) Physics 101: Lecture 17, Pg 1

Homework 9 Help A block of mass M 1 = 3 kg rests on a table with which it has a coefficient of friction µ = 0.73. A string attached to the block passes over a pulley to a block of mass M 3 = 5 kg. The pulley is a uniform disk of mass M 2 = 0.7 kg and radius 15 cm. As the mass M 3 falls, the string does not slip on the pulley. Newtons 2 nd Law 1) T 1 f = M 1 a 1 2) T 1 R T 3 R = -I a 2 /R M 1 N M 1 g 3) M 3 g - T 3 = M 3 a 3 x f T 1 T 1 y M 2 T 3 M 3 T 3 M 3 g Notes: 1) f = m M 1 g 2) a 2 = -a 1 / R 3) I = ½ M R 2 4) a 1 = a 3 Rewrite (a = a 1 ) 1) T 1 = M 1 a+mm 1 g 2) T 3 T 1 = ½ M 2 a 3) T 3 = M 3 g M 3 a Physics 101: Lecture 17, Pg 2

Overview F Net = m a F Net Δx = DK F Net Δt = Dp t Net = I a = DL/Dt Today: apply these ideas to molecules in fluids! Physics 101: Lecture 17, Pg 3

Fluids States of Matter Solid Hold Volume Hold Shape Liquid Hold Volume Adapt Shape Gas Adapt Volume Adapt Shape Physics 101: Lecture 17, Pg 4

Qualitative Demonstration of Pressure Force due to molecules of fluid colliding with container. Impulse F av Dt = Dp Average Pressure = F / A y average vertical force = f y = Dp y Dt = D mv y Dt Physics 101: Lecture 17, Pg 5

Atmospheric Pressure Basically weight of atmosphere! Air molecules are colliding with you right now! Pressure = 1x10 5 N/m 2 = 14.7 lbs/in 2! Example: Sphere with r = 0.1 m Magdeburg Spheres demo A = 4 p r 2 =.125 m 2 F = 12,000 Newtons (over 2,500 lbs)! Can demo Physics 101: Lecture 17, Pg 6

Pascal s Principle A change in pressure at any point in a confined fluid is transmitted everywhere in the fluid. Hydraulic Lift DP 1 = DP 2 F 1 /A 1 = F 2 / A 2 F 1 = F 2 (A 1 /A 2 ) lift demo Compare the work done by F 1 with the work done by F 2 A) W 1 > W 2 B) W 1 = W 2 C) W 1 < W 2 W = F d cos q W 1 = F 1 d 1 = F 2 (A 1 / A 2 ) d 1 but: A 1 d 1 = V 1 = V 2 = A 2 d 2 = F 2 V 2 / A 2 = F 2 d 2 = W 2 Physics 101: Lecture 17, Pg 7

Gravity and Pressure Two identical light containers are filled with water. The first is completely full of water, the second container is filled only ½ way. Compare the pressure each container exerts on the table. 1 2 A) P 1 > P 2 B) P 1 = P 2 C) P 1 < P 2 P = F/A = mg / A Cup 1 has greater mass, but same area Under water P = P atmosphere + r g h Physics 101: Lecture 17, Pg 8

Pascal s Principle (Restated) 1. Without gravity: Pressure of a confined fluid is everywhere the same. 2. With gravity: P = P atm + r g h Density r = M/V Pressure of a fluid is everywhere the same at the same depth. [vases demo] In general: in a confined fluid, change in pressure is everywhere the same. Physics 101: Lecture 17, Pg 9

Dam ACT B A A Two dams of equal height prevent water from entering the basin. Compare the net force due to the water on the two dams. A) F A > F B B) F A =F B C) F A < F B F = P A, and pressure is rgh. Same pressure, same area, same force even though more water in B! Physics 101: Lecture 17, Pg 10

Pressure and Depth Barometer: a way to measure atmospheric pressure For non-moving fluids, pressure depends only on depth. p 2 = p 1 + rgh P atm - 0 = rgh Measure h, determine p atm example--mercury p 1 =0 p 2 =p atm h r = 13,600 kg/m 3 p atm = 1.05 x 10 5 Pa h = 0.757 m = 757 mm = 29.80 (for 1 atm) Physics 101: Lecture 17, Pg 11

Checkpoint Is it possible to stand on the roof of a five story (50 foot) tall house and drink, using a straw, from a glass on the ground? 1.No 2.Yes p=0 p a h P a = r gh h = Pa rg The atmospheric pressure applied to the liquid will only be able to lift the liquid to a limited height no matter how hard you suck on the straw. Certainly trees have developed some mechanism to transport water from ground level, through their vascular tissues, and to their leaves (which can be higher that 50 feet) [demo] Physics 101: Lecture 17, Pg 12

Archimedes Principle Determine force of fluid on immersed cube Draw FBD» F B = F 2 F 1» = P 2 A P 1 A» = (P 2 P 1 )A» = r g d A» = r g V» = (M fluid /V) g V» = M fluid g Buoyant force is weight of displaced fluid! Physics 101: Lecture 17, Pg 13

Archimedes Example A cube of plastic 4.0 cm on a side with density = 0.8 g/cm 3 is floating in the water. When a 9 gram coin is placed on the block, how much does it sink below the water surface? Mg F b mg F Net = m a = 0 F b Mg mg = 0 h r g V disp = (M+m) g V disp = (M+m) / r h A = (M+m) / r h = (M + m)/ (r A) = (51.2+9)/(1 x 4 x 4) = 3.76 cm [coke demo] M = r plastic V cube = 4x4x4x0.8 = 51.2 g Physics 101: Lecture 17, Pg 14

Summary Pressure is force exerted by molecules bouncing off container P = F/A Gravity/weight affects pressure P = P 0 + rgd Buoyant force is weight of displaced fluid. F = r g V Physics 101: Lecture 17, Pg 15