Inelastic Collisions Review Impulse/Momentum 3 cases

Slides:



Advertisements
Similar presentations
Momentum-Impulse Theorem Collision:
Advertisements

Chapter 5 Momentum Ewen et al. 2005) Objective: Apply the law of conservation of momentum to both elastic and inelastic collisions of two objects. Apply.
Linear Impulse − Momentum
Copyright © 2012 Pearson Education Inc. PowerPoint ® Lectures for University Physics, Thirteenth Edition – Hugh D. Young and Roger A. Freedman Lectures.
Conservation of Momentum
Chapter 6 Momentum and Collisions 1. Momentum and Impulse 2. Conservation of Momentum 3. 1D Collisions 4. 2D Collisions.
Momentum and Inertia. Momentum Momentum = mass x velocity MV = P Momentum is inertia in motion. A moving object has more p than an object with less m.
1.MOMENTUM l Momentum = mass times velocity Units - kg m/s.
Chapter 7 Impulse and Momentum.
Non-Conservative Forces,
Physics A First Course Forces and Motion Chapter 3.
Chapter 8: Momentum Conservation
Physics 218: Mechanics Instructor: Dr. Tatiana Erukhimova Lecture 27.
Chapter 7 Linear Momentum. Chapter Momentum Linear Momentum- product of mass times velocity p=mvp=momentum units=kg.m/sec Restate Newton’s second.
© Houghton Mifflin Harcourt Publishing Company Section 1 Momentum and Impulse Chapter 6 Linear Momentum Momentum is defined as mass times velocity. Momentum.
Momentum Momentum is defined as “Inertia in Motion” p = mv.
Motion Summary.  Vectors & Scalars  Displacement, Velocity, Acceleration  Equations of motion  Relative motion.
Momentum, Impulse, and Collisions
Notes: Chapter 11.3 Newton’s Third Law of Motion and Momentum.
1 PPMF102– Lecture 3 Linear Momentum. 2 Linear momentum (p) Linear momentum = mass x velocity Linear momentum = mass x velocity p = mv p = mv SI unit:
Force and Potential Energy (3D). Energy Diagram We can glean a lot of information by looking at graph of the potential energy.
REVISION MOMENTUM. the product of an object's mass and its velocity a vector quantity with the same direction as the velocity of the object. MOMENTUM.
Chapter 9 - Collisions Momentum and force Conservation of momentum
Chapter 7 Impulse and Momentum. 7.1 The Impulse-Momentum Theorem DEFINITION OF IMPULSE The impulse of a force is the product of the average force and.
Energy Momentum, Collisions, Impulse. Momentum A measure of how hard it is to stop a moving object A measure of how hard it is to stop a moving object.
Ch 7. Impulse and Momentum
THINGS YOU WANTED TO KNOW, BUT WERE AFRAID TO ASK. IMPULSE AND MOMENTUM.
Physics 218 Lecture 15: Momentum Alexei Safonov.
Elastic and Inelastic Collisions. Elastic Collision If 2 colliding objects are very hard and no heat is produced in the collision, KE is conserved as.
Linear Momentum. 5-1 Linear Momentum Linear Momentum, p – defined as mass x velocity The unit is kgm/s A quantity used in collisions So a small object.
Momentum General Physics. Momentum Mass in motion Symbol: p Equation: p = m  v Units: kg x m/s Vector quantity.
Impulse, Momentum and Collisions. momentum = mass x velocity p = mv units: kgm/s or Ns.
Momentum. The p = m = mass v = velocity Unit: Vector Direction of momentum is determined by the direction of the.
Law of Conservation of Momentum. The Law of Conservation for Momentum Momentum is always conserved in a collision. It is never created or destroyed! (Just.
Conservation of Momentum Physics Chapter 6 Section 2 (Pages )
Momentum Notes. Momentum Momentum ( ρ) – inertia in motion Mass x Velocity ρ = mv measured in kg·m/s.
1 Mr. Moe Mentum. 2 We’ve talked about forces, but how do they affect and relate to motion? If we remember Newton’s 2 nd Law, the net force = time rate.
Chapter 6 and 7. momentum = mass x velocity p = mv units: kgm/s or Ns.
Chapter 9 Linear Momentum Introduction – Our approach Introducing momentum and impulse Conservation of momentum Conservation of energy and/or momentum.
Ch 8 : Conservation of Linear Momentum 1.Linear momentum and conservation 2.Kinetic Energy 3.Collision 1 dim inelastic and elastic nut for 2 dim only inellastic.
Notes: Chapter 11.3 Newton’s Third Law of Motion and Momentum.
AP Phys B Test Review Momentum and Energy 4/28/2008.
Momentum-Impulse Physics 513. Multi-Dimensional Impulse A soccer ball has a mass of 0.40 kg. Initially it is moving to the left at 20 m/s, but then it.
© 2005 Pearson Prentice Hall This work is protected by United States copyright laws and is provided solely for the use of instructors in teaching their.
Momentum Prepared by Gabriel Tan. Recapitalization Momentum is define as p = m v [kgms -1 or Ns]
Formula Momentum (p) = Mass x velocity Unit is kgm/s.
From Last DAY.
LINEAR MOMENTUM The rate of change of the linear momentum of a particle is equal to the net force acting on the particle.
Conservative Forces and Non-Conservative Forces
Momentum Review Energy, Intro Momentum Impulse-Momentum
Linear Momentum AP Physics.
Momentum.
Quiz 1 Period 2.
Linear Momentum.
Linear Momentum and Collisions.
Conservation of Momentum
Collisions In collisions momentum is conserved because all of the forces acting are internal forces. Remember: According to the Law of Conservation of.
Unit 7 Momentum & Collisions 7.5.
Unit 7 Momentum & Collisions 7.5.
Demos Cont’d EDU 412/413.
Section 2 Conservation of Momentum
11-1 Physics I Class 11 Conservative Forces, Non-Conservative Forces, and Collisions.
MOMENTUM (p) is defined as the product of the mass and velocity -is based on Newton’s 2nd Law F = m a F = m Δv t F t = m Δv IMPULSE MOMENTUM.
Conservation of Momentum
Motion Detector Force Probe.
Chapter 2-4 Newton’s Third Law.
Momentum, Impulse, and Collisions
Momentum.
Linear Momentum and Collisions.
Force and Motion (H) Newton's second law. Inertia. Weight.
Presentation transcript:

Inelastic Collisions Review Impulse/Momentum 3 cases Indeterminate Inelastic Collision examples Ballistic Pendulum Other Inelastic examples

“Gravity” movie Newton’s Laws (conservation of momentum) 90 minute orbital time (different orbits?) CO2 fire extinguisher thruster Reentry (she’s going fast!)

Review – Impulse/Momentum Collisions 𝐹 12 =− 𝐹 21 𝑏𝑦 𝑎𝑐𝑡𝑖𝑜𝑛−𝑟𝑒𝑎𝑐𝑡𝑖𝑜𝑛 𝐹 12 ∆𝑡=− 𝐹 21 ∆𝑡 𝐼𝑚𝑝𝑢𝑙𝑠𝑒 1 = 𝐼𝑚𝑝𝑢𝑙𝑠𝑒 2 ∆ 𝑃 1 =−∆ 𝑃 2 (𝑚 1 𝑣 1 ′ − 𝑚 1 𝑣 1 )= −(𝑚 2 𝑣 2 ′ − 𝑚 2 𝑣 2 ) 𝑃 1 + 𝑃 2 = 𝑃 1 ′ + 𝑃 2 ′ 𝑚 1 𝑣 1 + 𝑚 2 𝑣 2 = 𝑚 1 𝑣 1 ′ + 𝑚 2 𝑣 2 ′ F12 = force on 1 due to 2 1 2

Conservation of Momentum 𝑚 1 𝑣 1 + 𝑚 2 𝑣 2 = 𝑚 1 𝑣 1 ′ + 𝑚 2 𝑣 2 ′ Too many variables – 3 possibilities Inelastic – eliminate variable 𝑚 1 𝑣 1 + 𝑚 2 𝑣 2 = 𝑚 1 𝑣′ + 𝑚 2 𝑣′ Elastic - generate 2nd equation 1 2 𝑚 1 𝑣 1 2 + 1 2 𝑚 2 𝑣 2 2 = 1 2 𝑚 1 𝑣 1 ′ 2 + 1 2 𝑚 2 𝑣 2 ′ 2 Indeterminate - need more info

Inelastic Example 1 Conservation of momentum Inelastic 10,000 kg railroad car traveling at 24 m/s strikes a second 10,000 kg car at rest. They couple together, what is final speed? Conservation of momentum 𝑚 1 𝑣 1 + 𝑚 2 𝑣 2 = 𝑚 1 𝑣 1 ′ + 𝑚 2 𝑣 2 ′ Inelastic 𝑚 1 𝑣 1 + 𝑚 2 𝑣 2 = 𝑚 1 𝑣′ + 𝑚 2 𝑣′ 10,000 𝑘𝑔∙ 24 𝑚 𝑠 +0=(10,000 𝑘𝑔+10,000 𝑘𝑔) 𝑣′ 𝑣 ′ =12 𝑚/𝑠

Inelastic Example 1 (cont) Make the moving car 20,000 kg 𝑚 1 𝑣 1 + 𝑚 2 𝑣 2 = 𝑚 1 𝑣′ + 𝑚 2 𝑣′ 20,000 𝑘𝑔∙ 24 𝑚 𝑠 +0=(20,000 𝑘𝑔+10,000 𝑘𝑔) 𝑣′ 𝑣 ′ =16 𝑚/𝑠 Make the stationary car 20,000 kg 10,000 𝑘𝑔∙ 24 𝑚 𝑠 +0=(10,000 𝑘𝑔+20,000 𝑘𝑔) 𝑣′ 𝑣 ′ =8 𝑚/𝑠

Inelastic Example 1 (cont) What happened to the energy? Kinetic energy before 1 2 𝑚 1 𝑣 1 2 + 1 2 𝑚 2 𝑣 2 2 = 1 2 10,000𝑘𝑔 24 𝑚 𝑠 2 =2.88∙ 10 6 𝐽 Kinetic energy after 1 2 (𝑚 1 + 𝑚 2 ) 𝑣′ 2 = 1 2 20,000𝑘𝑔 12 𝑚 𝑠 2 =1.44∙ 10 6 𝐽 Lost in heat

𝑣 1 ′ =−2.5 𝑚/𝑠 in opposite direction Inelastic Example 2 Calculate the recoil velocity of 5 kg rifle that shoots a 0.02 kg bullet at 620 m/s. Conservation of momentum 𝑚 1 𝑣 1 + 𝑚 2 𝑣 2 = 𝑚 1 𝑣 1 ′ + 𝑚 2 𝑣 2 ′ Inelastic collision in reverse. 5 𝑘𝑔∙0 𝑚 𝑠 +.02 𝑘𝑔∙0 𝑚 𝑠 =0=5 𝑘𝑔 ∙𝑣 ′ 1 + .02 𝑘𝑔∙620𝑚/𝑠 𝑣 1 ′ =−2.5 𝑚/𝑠 in opposite direction

Ballistic Pendulum Sequence Solve Backwards! Conservation momentum Conservation of energy Solve Backwards! Step 1: Conservation momentum: 𝑚𝑣= 𝑚+𝑀 𝑣 ′ 𝑣= 𝑚+𝑀 𝑚 𝑣′ Step 2: Conservation of energy: 1 2 𝑚+𝑀 𝑣′ 2 = 𝑚+𝑀 𝑔ℎ 𝑣 ′ = 2𝑔ℎ Combining: 𝑣= 𝑚+𝑀 𝑚 2𝑔ℎ

Ballistic Pendulum Example For h2 𝑣 2 = 𝑚+𝑀 𝑚 2𝑔 ℎ 2 𝑣 1 = 𝑚+𝑀 𝑚 2𝑔 ℎ 1 Combining 𝑣 2 𝑣 1 = 𝑚+𝑀 𝑚 2𝑔 ℎ 2 𝑚+𝑀 𝑚 2𝑔 ℎ 1 = ℎ 2 ℎ 1

Example 1 1. Conservation momentum 2. Conservation energy 𝑚 𝑏𝑢𝑙 + 𝑚 𝑏𝑙𝑜𝑐𝑘 𝑣 ′ = 𝑚 𝑏𝑢𝑙 𝑣 𝑏𝑢𝑙 + 𝑚 𝑏𝑙𝑜𝑐𝑘 𝑣 𝑏𝑙𝑜𝑐𝑘 .029 𝑘𝑔+1.4 𝑘𝑔 𝑣 ′ =.029 𝑘𝑔 510 𝑚 𝑠 +0 𝑣′=10.3 𝑚/𝑠 2. Conservation energy 1 2 𝑚 𝑏𝑢𝑙 + 𝑚 𝑏𝑙𝑜𝑐𝑘 𝑣′ 2 = 𝑚 𝑏𝑢𝑙 + 𝑚 𝑏𝑙𝑜𝑐𝑘 𝑔ℎ ℎ= 𝑣′ 2 2𝑔 =5.47 𝑚

Example 2 1. Conservation of momentum 2. Work-energy 0− 1 2 𝑚 𝑏𝑢𝑙 + 𝑚 𝑏𝑙𝑜𝑐𝑘 𝑣 ′ 2 = −𝜇 𝑘 𝑚 𝑏𝑢𝑙 + 𝑚 𝑏𝑙𝑜𝑐𝑘 𝑔 𝑥 𝑣 ′ = 2𝜇 𝑘 𝑔 𝑥 𝑣 ′ = 2∙0.25∙9.8 𝑚 𝑠 2 ∙9.5 𝑚 =6.82 𝑚 𝑠 1. Conservation of momentum 𝑚 𝑏𝑢𝑙 𝑣 𝑏𝑢𝑙 + 𝑚 𝑏𝑙𝑜𝑐𝑘 𝑣 𝑏𝑙𝑜𝑐𝑘 = 𝑚 𝑏𝑢𝑙 + 𝑚 𝑏𝑙𝑜𝑐𝑘 𝑣 ′ 𝑣 𝑏𝑢𝑙= 𝑚 𝑏𝑢𝑙 + 𝑚 𝑏𝑙𝑜𝑐𝑘 𝑚 𝑏𝑢𝑙 𝑣 ′ =375 𝑚 𝑠

Inelastic car collision Work-energy 0− 1 2 𝑚 𝑆𝐶 + 𝑚 𝑆𝑈𝑉 𝑣 ′ 2 = −𝜇 𝑘 𝑚 𝑆𝐶 + 𝑚 𝑆𝑈𝑉 𝑔 𝑥 𝑣 ′ = 2𝜇 𝑘 𝑔 𝑥 𝑣 ′ = 2∙0.8∙9.8 𝑚 𝑠 2 ∙2.8 𝑚 =6.62 𝑚 𝑠 Conservation of momentum 𝑚 𝑆𝐶 𝑣 𝑆𝐶 + 𝑚 𝑆𝑈𝑉 𝑣 𝑆𝑈𝑉 = 𝑚 𝑆𝐶 + 𝑚 𝑆𝑈𝑉 𝑣 ′ 𝑣 𝑆𝐶= 𝑚 𝑆𝐶 + 𝑚 𝑆𝑈𝑉 𝑚 𝑆𝐶 𝑣 ′ = 920 𝑘𝑔+2300 𝑘𝑔 920 𝑘𝑔 6.62 𝑚 𝑠 =23.2 𝑚/𝑠