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Lecture 25

Lecture 25. Today Review:. Exam covers Chapters 14-17 plus angular momentum, rolling motion & torque. Assignment HW11, Due Tuesday, May 6 th For Thursday, read through all of Chapter 18. r i. w i. Angular Momentum Exercise.

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Lecture 25

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  1. Lecture 25 Today Review: • Exam covers Chapters 14-17 plus angular momentum, rolling motion & torque • Assignment • HW11, Due Tuesday, May 6th • For Thursday, read through all of Chapter 18

  2. ri wi Angular Momentum Exercise • A mass m=0.10 kg is attached to a cord passing through a small hole in a frictionless, horizontal surface as in the Figure. The mass is initially orbiting with speed wi = 5 rad / s in a circle of radius ri = 0.20 m. The cord is then slowly pulled from below, and the radius decreases to r = 0.10 m. • What is the final angular velocity ? • Underlying concept: Conservation of Momentum

  3. ri wi Angular Momentum Exercise • A mass m=0.10 kg is attached to a cord passing through a small hole in a frictionless, horizontal surface as in the Figure. The mass is initially orbiting with speed wi = 5 rad / s in a circle of radius ri = 0.20 m. The cord is then slowly pulled from below, and the radius decreases to r = 0.10 m. • What is the final angular velocity ? No external torque implies DL = 0 or Li = Lc Ii wi = Ifwf I for a point mass is mr2where r is the distance to the axis of rotation m ri2wi = m rf2 wf wf = ri2wi / rf2 = (0.20/0.10)2 5 rad/s = 20 rad/s

  4. Example: Throwing ball from stool • A student sits on a stool, initially at rest, but which is free to rotate. The moment of inertia of the student plus the stool is I. They throw a heavy ball of mass M with speed v such that its velocity vector has a perpendicular distance d from the axis of rotation. • What is the angular speed F of the student-stool system after they throw the ball ? M Mv r F d I I Top view: before after

  5. Example: Throwing ball from stool • What is the angular speed F of the student-stool system after they throw the ball ? • Process: (1) Define system (2) Identify Conditions (1) System: student, stool and ball (No Ext. torque, L is constant) (2) Momentum is conserved (check |L| = |r| |p| sin qfor sign) Linit = 0 = Lfinal = -Mvd + I wf M v F d I I Top view: before after

  6. DV Ideal Fluid Bernoulli Equation P1+ ½ r v12 + r g y1 = constant A 5 cm radius horizontal pipe carries water at 10 m/s into a 10 cm radius. ( rwater =103 kg/m3 ) What is the pressure difference? P1+ ½ r v12 = P2+ ½ r v22 DP= ½ r v22 - ½ r v12 DP= ½ r (v22 - v12 ) and A1 v1 = A2 v2 DP= ½ r v22 (1– (A2/A1 )2 ) =0.5 x 1000 kg/m x 100 m2/s2 (1- (25/100)2 ) = 47000 Pa

  7. A water fountain • A fountain, at sea level, consists of a 10 cm radius pipe with a 5 cm radius nozzle. The water sprays up to a height of 20 m. • What is the velocity of the water as it leaves the nozzle? • What volume of the water per second as it leaves the nozzle? • What is the velocity of the water in the pipe? • What is the pressure in the pipe? • How many watts must the water pump supply?

  8. A water fountain • A fountain, at sea level, consists of a 10 cm radius pipe with a 5 cm radius nozzle. The water sprays up to a height of 20 m. • What is the velocity of the water as it leaves the nozzle? Simple Picture: ½mv2=mgh  v=(2gh)½ = (2x10x20)½ = 20 m/s • What volume of the water per second as it leaves the nozzle? Q = A vn = 0.0025 x 20 x 3.14 = 0.155 m3/s • What is the velocity of the water in the pipe? An vn = Ap vp vp = Q /4 = 5 m/s • What is the pressure in the pipe? 1atm + ½ r vn2 = 1 atm + DP + ½ r vp2  1.9 x 105 N/m2 • How many watts must the water pump supply? • Power = Q r g h = 0.0155 m3/s x 103 kg/m3 x 9.8 m/s2 x 20 m = 3x104 W (Comment on syringe injection)

  9. Fluids Buoyancy • A metal cylinder, 0.5 m in radius and 4.0 m high is lowered, as shown, from a massles rope into a vat of oil and water. The tension, T, in the rope goes to zero when the cylinder is half in the oil and half in the water. The densities of the oil is 0.9 gm/cm3 and the water is 1.0 gm/cm3 • What is the average density of the cylinder? • What was the tension in the rope when the cylinder was submerged in the oil?

  10. Fluids Buoyancy • r = 0.5 m, h= 4.0 m • roil = 0.9 gm/cm3 rwater = 1.0 gm/cm3 • What is the average density of the cylinder? When T = 0 Fbuoyancy = Wcylinder Fbuoyancy = roil g ½ Vcyl.+ rwater g ½ Vcyl. Wcylinder = rcyl g Vcyl. rcyl g Vcyl. = roil g ½ Vcyl.+ rwater g ½ Vcyl. rcyl = ½ roill.+ ½ rwater What was the tension in the rope when the cylinder was submerged in the oil? Use a Free Body Diagram !

  11. Fluids Buoyancy • r = 0.5 m, h= 4.0 m Vcyl. = p r2 h • roil = 0.9 gm/cm3 rwater = 1.0 gm/cm3 • What is the average density of the cylinder? When T = 0 Fbuoyancy = Wcylinder Fbuoyancy = roil g ½ Vcyl.+ rwater g ½ Vcyl. Wcylinder = rcyl g Vcyl. rcyl g Vcyl. = roil g ½ Vcyl.+ rwater g ½ Vcyl. rcyl = ½ roill.+ ½ rwater = 0.95 gm/cm3 What was the tension in the rope when the cylinder was submerged in the oil? Use a Free Body Diagram! S Fz = 0 = T - Wcylinder + Fbuoyancy T = Wcyl - Fbuoy = g ( rcyl.- roil ) Vcyl T = 9.8 x 0.05 x 103 x p x 0.52 x 4 .0 = 1500 N

  12. A new trick • Two trapeze artists, of mass 100 kg and 50 kg respectively are testing a new trick and want to get the timing right. They both start at the same time using ropes of 10 meter in length and, at the turnaround point the smaller grabs hold of the larger artist and together they swing back to the starting platform. A model of the stunt is shown at right. • How long will this stunt require if the angle is small ?

  13. A new trick • How long will this stunt require? Period of a pendulum is just w = (g/L)½ T = 2p (L/g)½ Time before ½ period Time after ½ period So, t = T = 2p(L/g)½ = 2p sec Key points: Period is one full swing and independent of mass (this is SHM but very different than a spring. SHM requires only a linear restoring force.)

  14. M k m M k m -2 0(≡Xeq) 2 Example • A Hooke’s Law spring, k=200 N/m, is on a horizontal frictionless surface is stretched 2.0 m from its equilibrium position. A 1.0 kg mass is initially attached to the spring however, at a displacement of 1.0 m a 2.0 kg lump of clay is dropped onto the mass. The clay sticks. What is the new amplitude?

  15. M k m M k m -2 0(≡Xeq) 2 Example • A Hooke’s Law spring, k=200 N/m, is on a horizontal frictionless surface is stretched 2.0 m from its equilibrium position. A 1.0 kg mass is initially attached to the spring however, at a displacement of 1.0 m a 2.0 kg lump of clay is dropped onto the mass. What is the new amplitude? Sequence: SHM, collision, SHM ½ k A02 = const. ½ k A02 = ½ mv2 + ½ k (A0/2)2 ¾ k A02 = m v2  v = ( ¾ k A02 / m )½ v = (0.75*200*4 / 1 )½ = 24.5 m/s Conservation of x-momentum: mv= (m+M) V  V = mv/(m+M) V = 24.5/3 m/s = 8.2 m/s

  16. M k m M k m -2 0(≡Xeq) 2 Example • A Hooke’s Law spring, k=200 N/m, is on a horizontal frictionless surface is stretched 2.0 m from its equilibrium position. A 1.0 kg mass is initially attached to the spring however, at a displacement of 1.0 m a 2.0 kg lump of clay is dropped onto the mass. The clay sticks. What is the new amplitude? Sequence: SHM, collision, SHM V = 24.5/3 m/s = 8.2 m/s ½ k Af2 = const. ½ k Af2 = ½ (m+M)V2 + ½ k (Ai)2 Af2 = [(m+M)V2 /k + (Ai)2 ]½ Af2 = [3 x 8.22 /200 + (1)2 ]½ Af2 = [1 + 1]½ Af2 = 1.4 m Key point: K+U is constant in SHM

  17. Fluids Buoyancy & SHM • A metal cylinder, 0.5 m in radius and 4.0 m high is lowered, as shown, from a rope into a vat of oil and water. The tension, T, in the rope goes to zero when the cylinder is half in the oil and half in the water. The densities of the oil is 0.9 gm/cm3 and the water is 1.0 gm/cm3 • Refer to earlier example • Now the metal cylinder is lifted slightly from its equilibrium position. What is the relationship between the displacement and the rope’s tension? • If the rope is cut and the drum undergoes SHM, what is the period of the oscillation if undamped?

  18. Fluids Buoyancy & SHM • Refer to earlier example • Now the metal cylinder is lifted Dy from its equilibrium position. What is the relationship between the displacement and the rope’s tension? 0 = T + Fbuoyancy – Wcylinder T = - Fbuoyancy + Wcylinder T =-[rog(h/2+Dy) Ac+rwgAc(h/2-Dy)] + Wcyl T =-[ghAc(ro +rw)/2 + Dy gAc(ro -rw)]+ Wcyl T =-[Wcyl + Dy gAc(ro -rw)]+ Wcyl T = [ g Ac (rw -ro) ] Dy If the is rope cut, net force is towards equilibrium position with a proportionality constant g Ac (rw -ro) [& with g=10 m/s2] If F = - k Dy then k = g Ac (ro -rw) = p/4 x103 N/m

  19. Fluids Buoyancy & SHM • A metal cylinder, 0.5 m in radius and 4.0 m high is lowered, as shown, from a rope into a vat of oil and water. The tension, T, in the rope goes to zero when the cylinder is half in the oil and half in the water. The densities of the oil is 0.9 gm/cm3 and the water is 1.0 gm/cm3 • If the rope is cut and the drum undergoes SHM, what is the period of the oscillation if undamped? F = ma = - k Dy and with SHM …. w = (k/m)½ where k is a “spring” constant and m is the inertial mass (resistance to motion), the cylinder Sow = (1000p /4 mcyl)½ = (1000p / 4rcylVcyl)½ = ( 0.25/0.95 )½ = 0.51 rad/sec T = 3.2 sec

  20. Underdamped SHM if If the period is 2.0 sec and, after four cycles, the amplitude drops by 75%, what is the time constant? Four cycles implies 8 sec So 0.25 A0 = A0 exp(-4 b/m) ln(1/4)= -4 1/t t = -4 / ln(1/4) = 2.9 sec

  21. |L|=mvrperpendicular Ch. 12

  22. Hooke’s Law Springs and a Restoring Force • Key fact: w = (k / m)½ is general result where k reflects a constant of the linear restoring force and m is the inertial response (e.g., the “physical pendulum” where w = (k / I)½

  23. Simple Harmonic Motion Maximum potential energy Maximum kinetic energy

  24. Resonance and damping • Energy transfer is optimal when the driving force varies at the resonant frequency. • Types of motion • Undamped • Underdamped • Critically damped • Overdamped

  25. Fluid Flow

  26. Density and pressure

  27. Response to forces

  28. States of Matter and Phase Diagrams

  29. Ideal gas equation of state

  30. pV diagrams

  31. Thermodynamics

  32. Work, Pressure, Volume, Heat T can change! In steady-state T=constant and so heat in equals heat out

  33. Gas Processes

  34. Lecture 25 • Exam covers Chapters 14-17 plus angular momentum, rolling motion & torque • Assignment • HW11, Due Tuesday, May 6th • For Thursday, read through all of Chapter 18

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