PHY 231 1 PHYSICS 231 Lecture 29: Problems Remco Zegers Walk-in hour: Thursday 11:30-13:30 am Helproom.

Slides:



Advertisements
Similar presentations
Rotational Equilibrium and Rotational Dynamics
Advertisements

PHY PHYSICS 231 Lecture 26: Ideal gases Remco Zegers Walk-in hour: Thursday 11:30-13:30 am Helproom.
Fluid Mechanics Density is mass per unit of volume. ρ = m / V ρ = density m = mass (kg) V = volume (m 3 ) Things with low densities float in things with.
Chapter 9 Solids and Fluids 1. Introduction 2. Fluids at Rest 3. Fluid Motion.
Chapter 14: Fluid mechanics
Static Fluids Fluids are substances, such as liquids and gases, that have no rigidity. A fluid lacks a fixed shape and assumes the shape of its container.
Physics 203 College Physics I Fall 2012
Fluid Mechanics Chapter 9.
Problems from old midterm 3
Midterm 3 - overview.  =I  (compare to  F=ma ) Moment of inertia I: I=(  m i r i 2 )  : angular acceleration I depends on the choice of rotation.
PHY PHYSICS 231 Lecture 20: Angular momentum Remco Zegers Walk-in hour: Thursday 11:30-13:30 am Helproom Neutron star.
Physics 102 Part II Thermal Physics Moza M. Al-Rabban Professor of Physics Fluids (2)
PHY PHYSICS 231 Lecture 24: Ideal gases Remco Zegers Walk-in hour:Tue 4-5 pm Helproom.
PHY PHYSICS 231 Lecture 19: More about rotations Remco Zegers Walk-in hour: Thursday 11:30-13:30 am Helproom Demo: fighting sticks.
PHY PHYSICS 231 Lecture 20: Angular momentum Remco Zegers Walk-in hour: Thursday 11:30-13:30 am Helproom Neutron star.
PHY PHYSICS 231 Lecture 21: Angular momentum Remco Zegers Walk-in hour: Monday 9:15-10:15 am Helproom Neutron star.
PHYSICS 231 Lecture 28: Thermal conduction
PHY PHYSICS 231 Lecture 19: More about rotations Remco Zegers Walk-in hour: Thursday 11:30-13:30 am Helproom Demo: fighting sticks.
PHY PHYSICS 231 Lecture 24: Buoyancy and Fluid Motion Remco Zegers Walk-in hour: Monday 9:15-10:15 am Helproom.
PHY PHYSICS 231 Lecture 22: fluids and viscous flow Remco Zegers Walk-in hour: Tue 4-5 pm Helproom.
PHYSICS 231 Lecture 24: Walking on water & other ‘magic’
PHY PHYSICS 231 Lecture 21: Buoyancy and Fluid Motion Remco Zegers Walk-in hour: Tue 4-5 pm Helproom.
PHY PHYSICS 231 Lecture 22: fluids and viscous flow Remco Zegers Walk-in hour: Tue 4-5 pm Helproom.
PHY PHYSICS 231 Lecture 19: Angular momentum Remco Zegers Walk-in hour: Tue 4:00-5:00 am Helproom Neutron star.
Static Fluids Fluids are substances, such as liquids and gases, that have no rigidity. A fluid lacks a fixed shape and assumes the shape of its container.
Unit 3 - FLUID MECHANICS.
Fluids Fluids flow – conform to shape of container –liquids OR gas.
Fluid Mechanics Ellen Akers. Fluids A fluid is a substance that has the ability to flow and change its shape. Gases and liquids are both fluids. Liquids.
Angular Momentum of a Particle
PHY PHYSICS 231 Lecture 30: review Remco Zegers Walk-in hour: Monday 9:15-10:15 am Helproom.
PHY PHYSICS 231 Lecture 30: review Remco Zegers Walk-in hour: Monday 9:15-10:15 am Helproom.
Monday, Nov. 22, 2004PHYS , Fall 2004 Dr. Jaehoon Yu 1 1.Density and Specific Gravity 2.Fluid and Pressure 3.Absolute and Relative Pressure 4.Pascal’s.
Chapter 9 Fluid Mechanics.
Physics 1B03summer-Lecture 12 1 Day of Wrath Tuesday June 16 9:30-11:30 am CNH MC Questions, Cumulative.
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.
Advanced Physics Chapter 10 Fluids. Chapter 10 Fluids 10.1 Phases of Matter 10.2 Density and Specific Gravity 10.3 Pressure in Fluids 10.4 Atmospheric.
Fluid Mechanics Chapter 13 2 Fluid Anything that can flow A liquid or a gas Physics Chapter 13.
Warm-up Pick up the free response at the door and begin working on it.
Fluid Mechanics Chapter 8.
Density. Density Densities of some common materials Substance Density (kg/m3) Aluminum 2700 Bone Water 1000 Ice 920 Saltwater 1025 Blood.
Chapter 14: Solids, Liquids, and Gases
Fluids.
Physics 201: Lecture 19, Pg 1 Lecture 19 Goals: Specify rolling motion (center of mass velocity to angular velocity Compare kinetic and rotational energies.
Physics 203 – College Physics I Department of Physics – The Citadel Physics 203 College Physics I Fall 2012 S. A. Yost Chapter 8 Part 3 Chapter 9 Angular.
Physics 207: Lecture 25, Pg 1 Lecture 25 Today Review: Exam covers Chapters plus angular momentum, rolling motion & torque Exam covers Chapters
1 Fluid Mechanics Chapter 13 2 Fluid Anything that can flow A liquid or a gas.
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.
Density Densities of some common materials SubstanceDensity (kg/m 3 ) Aluminum2700 Bone Water1000 Ice920 Saltwater1025 Blood1050 Gasoline
Introduction To Fluids. Density  = m/V  = m/V   : density (kg/m 3 )  m: mass (kg)  V: volume (m 3 )
Lecture 19: Introduction to Solids & Fluids. Questions of Yesterday 1) A solid sphere and a hoop of equal radius and mass are both rolled up an incline.
Wednesday, Nov. 24, 2004PHYS , Fall 2004 Dr. Jaehoon Yu 1 1.Quiz Workout 2.Buoyant Force and Archimedes’ Principle 3.Flow Rate and Continuity Equation.
CHAPTER 9 Solids and Fluids Fluid Mechanics (only) pages
Monday, Apr. 19, 2004PHYS , Spring 2004 Dr. Jaehoon Yu 1 PHYS 1441 – Section 004 Lecture #21 Monday, Apr. 19, 2004 Dr. Jaehoon Yu Buoyant Force.
Fluids. Introduction The 3 most common states of matter are: –Solid: fixed shape and size (fixed volume) –Liquid: takes the shape of the container and.
Chapter 14 Fluids.
PHY PHYSICS 231 Lecture 18: equilibrium & revision Remco Zegers Walk-in hour: Thursday 11:30-13:30 am Helproom.
Chapter 9 Pretest Fluids
Pressure and Fluids § 15.1–15.5. Density Relating “how big” to “how much” § 15.1.
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.
PHY PHYSICS 231 Lecture 24: Buoyancy and Fluid Motion Remco Zegers Walk-in hour: Monday 9:15-10:15 am Helproom.
Fluid Mechanics Chapter 8. Fluids Ability to flow Ability to change shape Both liquids and gases Only liquids have definite volume.
Physics Chapter 9: Fluid Mechanics. Fluids  Fluids  Definition - Materials that Flow  Liquids  Definite Volume  Non-Compressible  Gasses  No Definite.
Ying Yi PhD Chapter 11 Fluids 1 PHYS HCC. Outline PHYS HCC 2 Density and Pressure Pressure and Depth in a Static fluid Buoyant Forces and Archimedes’
Chapter 12: Forces and Fluids
PHYSICS 231 Lecture 29: Problems
Fluid Mechanics Presentation on FLUID STATICS BY Group:
Physics 21.
Halliday/Resnick/Walker Fundamentals of Physics 8th edition
Fluids Liquids and Gases Chapter 11.
A solid cylinder with a radius of 4
Presentation transcript:

PHY PHYSICS 231 Lecture 29: Problems Remco Zegers Walk-in hour: Thursday 11:30-13:30 am Helproom

PHY Figure skating A male figure-skater rotates around a vertical axis (1 rev/s) while holding his partner at 1.5 m. He then pulls her towards him (1 m distance). A) How fast will he rotate now? Assume no net torque is exerted on the skaters. B) If the woman is 55 kg, how much work has the man done while pulling? A) Use conservation of angular momentum: L i =I i  i =M partner r i 2  i = M*1.5 2 *2  *1=14.1M kgm 2 /s L f =I f  f =M partner r f 2  f =M*1 2 *  f L i =L f so,  f =14.1 rad/s=2.25 rev/s B) Consider the change in rotational KE initial: KE=½I  i 2 =½mr i 2  i 2 =0.5*55*1.5 2 *(2  ) 2 =2443 J final: KE=½I  f 2 =½mr f 2  f 2 =0.5*55*1 2 * =5467 J difference: 3024 J: equals the work done by the man.

PHY Ball on a upward slope A ball (r=0.1 m) is rolled up a slope. Its linear velocity at the base is 10 m/s. How high will it go? (assume the ball does not slip and given I ball =2/5*Mr 2. Use conservation of mechanical energy. Initial: ½mv 2 +½I  2 +mgh= ½mv 2 +½2/5mr 2 (v/r) 2 +mgh= =0.7mv 2 =70m Final: ½mv 2 +½I  2 +mgh=mgh=9.8mh KE final =KE initial so h=70/9.8=7.1 m

PHY Ball game In a children’s game at a fair, buckets are placed at 1m from the center around which they all rotate (I total =50kg/m 2, 1rev/s). The children try to throw balls in the buckets. After 50 balls have gone in the buckets, the wheel has slowed down to 0.5 rev/s. How heavy is one ball? 1 rev/s Top view Use conservation of angular momentum: Initial L=I  =50*2  =100  Final L=I  =(50+N balls m balls r)*  =(50+50*m*1)  L initial =L final so 50m=50 m=1 kg.

PHY Bulk modulus A rubber ball, with bulk modulus B, volume V at 1 atm. increases its volume by 1 cm 3 when put in a vacuum chamber (P=0). If a ball of the same material but 5 times larger in volume at 1 atm, is put under a pressure of 3 atm, how much will its volume shrink? B=-  P/(  V/V) First case (1 atm -> vacuum): B=(-1 atm)/(-1 cm 3 /V) Second case (1 atm -> 3 atm): B=(2 atm)/(  V/5V) B is a constant, so must be equal in both cases:  V=10 cm 3 If you are not sure whether you need to convert to SI units, just do it: it is a bit of extra work, but at least you are sure it’s okay.

PHY Buoyant forces When submerged in water an object weighs 1.6N. At the same time, the water level in the water container (with A=0.01 m 2 ) rises 0.01 m. What is the specific gravity (sg) of the object? (  water =1.0x10 3 kg/m 3 ) A=0.01 m 2 Use the fact that the Buoyant force on a submerged object equals the weight of the displaced water. W=F g -B =M object g-M water,displaced g =  object V object g-  water V object g =V object g (  object -  water ) 1.6N=0.01*0.01*g(  object -  water )=1.0x10 -4 *9.8*  water (sg-1) sg=2.63

PHY Keep it coming. A plastic bag contains a glucose solution. The part of the bag that is not filled is under vacuum. If the pressure in a blood vein is 1.33x10 4 Pa, how high must one hang the bag to make sure the solution (specific gravity 1.02) enters the body? (  w =1.0x10 3 kg/m 3 ) P=P 0 +  gh 1.33x10 4 =0+1.02*1.0x10 3 *9.8*h h=1.33 m

PHY Titanic: After the Titanic sunk, 10 people manage to seek refuge on a 2x4m wooden raft. It is still 1.0 cm above water. A heavy debate follows when another person (60 kg) wants to board as well. Fortunately, a PHY231 student is among the 10. Can she convince the others that itis safe to pull the person on board without the whole raft sinking? (  w =1.0x10 3 kg/m 3 ) With 10 people: F g =B (M raft +M 10 )g=V displaced,before  w g With 11 people: F g =(M raft +M 10 +M 1 )g B=(V displaced,before +V extra )  w g stationary if F g =B (M raft +M 10 )g+M 1 g=(V displaced,before +V extra )  w g M 1 g=V extra  w g so V extra =(M 1 /  w ) V extra =60/1.0x10 3 =0.06m 3 V extra =LxWxH=8H=0.06 so H=0.75cm so there is still 0.25cm to spare!

PHY Bernoulli A=5cm 2 A=2cm 2, P=1 atm 2m Water flows over a height of 2m through an oddly shaped pipe. A) If the fluid velocity is 1 m/s at the bottom, what is it at the top? B) What is the water pressure at the top? A) Use the equation of continuity: A 1 v 1 =A 2 v 2 5*v top =2*1 v top =0.4 m/s B) Use Bernoulli. P top +½  v top 2 +  gh top = P bot +½  v bot 2 +  gh bot P top +0.5*(1E+03)* (1E+3)*9.8*2=(1E+05)+0.5*(1E+03)1 2 P top =80820 Pa.  =1.0x10 3 kg/m 3

PHY Centipede A centipede (100 legs) decides to cross a lake. The contact length between each of his legs and the water is 1mm. If its mass is 2g and  water =0.073 N/m will he succeed? Assume that the angle  =45 0. FsFs FsFs FgFg  1 leg F g =0.002*9.8=0.0196N F surface tension,vertical =100*2  water L contact sin  =200*0.073*0.001*0.707 =0.010N F g >F surface tension, vertical : he sinks!

PHY Ch. 10 Metal hoop A metal (thermal expansion coefficient  =17x / 0 C) hoop of radius 0.10 m is heated from 20 0 C to C. By how much does its radius change? 0.1m  L=  L 0  T =17x10 -6 (2  r 0 )80=8.5x10 -4 m r new =(L 0 +  L)/2  =L 0 /2  +  L/2  =r x10 -4 m

PHY : Diving Bell A cylindrical diving bell (diameter 3m and 4m tall, with an open bottom is submerged to a depth of 220m in the sea. The surface temperature is 25 0 C and at 220m, T=5 0 C. The density of sea water is 1025 kg/m 3. How high does the sea water rise in the bell when it is submerged? Consider the air in the bell. P surf =1.0x10 5 Pa V surf =  r 2 h=28.3m 3 T surf =25+273=298K P sub =P 0 +  w g*depth=2.3x10 6 Pa V sub =? T sub =5+273=278K Next, use PV/T=constant P surf V surf /T surf =P sub V sub /T sub plug in the numbers and find: V sub =1.15m 3 (this is the amount of volume taken by the air left) V taken by water = =27.15m 3 =  r 2 h h=27.15/  r 2 =3.8m rise of water level in bell.

PHY : Moles Two moles of Nitrogen gas (N 2 ) are enclosed in a cylinder with a moveable piston. A) If the temperature is 298 K and the pressure is 1.01x10 6 Pa, what is the volume (R=8.31 J/molK)? b) What is the average kinetic energy of the molecules? k B =1.38x J/K A)PV=nRT V=nRT/P =2*8.31*298/1.01x10 6 =4.9E-03 m 3 B) E kin,average =½mv 2 =3/2k B T=3/2*1.38x *298=6.2x J

PHY Ch 11: 3*10 3 J of heat is transferred to a 1cm 3 cube of gold at T=20 o C Will all the gold have melted afterwards? L f =6.44x10 4 J/kg T melt =1063 o C c specific =129 J/kg 0 C  =19.3x10 3 kg/m 3. When Solid: m=  V=(19.3x10 3 )x(1x10 -6 m 3 )=1.93x10 -2 kg. Q=cm  T=129*1.93x10 -2 *  T=2.5  T To raise to melting point:  T=( )=1043 o C, so Q=2608J During the phase change from solid to liquid: Q=L f m Q=6.44x10 4 *1.93x10 -2 =1.24x10 3 J to make liquid. Total needed: 3850 J, only 3000 J available, doesn’t melt completely.

PHY : Heat transfer 3 A hot block and a cold block are thermally connected. Three different methods to transfer heat are proposed as shown. Which one is the most efficient way (fastest) to transfer heat fro hot to cold and what are the relative rates of transfer? Area: A Length L 0.1A 0.2L 4A 5L A: cross section surface of black wire,L:its length Use: P=kA  T/L Case 1: P~A/L Case 2: P~0.1A/0.2L=0.5A/L Case 3: P~4A/5L=0.8L P 1 :P 2 :P 3 = 1:0.5:0.8 First case is most efficient. 1 2

PHY Thermal equilibrium 20g of a solid at 70 0 C is placed in 100g of a fluid at 20 o C. After waiting a while the temperature of the whole system is 30 o C and stays that way. The specific heat of the solid is: a)Equal to that of the fluid b)Less than that of the fluid c)Larger than that of the fluid d)Unknown; different phases cannot be compared e)Unknown; different materials cannot be compared Q fluid =-Q solid m fluid c fluid (T final -T fluid )=-m solid c solid (T final -T solid ) C fluid -m solid (T final -T solid ) C solid m fluid (T final -T fluid ) == -20(30-70) 100(30-20) = 0.8 C solid >C fluid