Examples: Mechanical Energy Conservation

Slides:



Advertisements
Similar presentations
Work- Mechanical Energy - To Do Work, Forces Must Cause Displacements frictionlessfrictionlessfrictionlessfrictionless.
Advertisements

Physics 111: Mechanics Lecture 7
Work Done by a Constant Force
Solving Problems with Energy Conservation, continued.
Fisica Generale - Alan Giambattista, Betty McCarty Richardson Copyright © 2008 – The McGraw-Hill Companies s.r.l. 1 Chapter 6: Conservation of Energy Work.
Gravitational potential energy. Conservation of energy
AP Physics B Summer Course 年AP物理B暑假班
Work, Energy, And Power m Honors Physics Lecture Notes.
Conservation of Energy Energy is Conserved!. The total energy (in all forms) in a “closed” system remains constant The total energy (in all forms) in.
Chapter 9:Linear Momentum 8-4 Problem Solving Using Conservation of Mechanical Energy 8-5 The Law of Conservation of Energy 8-6 Energy conservation with.
Conservation of Energy
Conservation of Energy
General Physics 1, Additional questions By/ T.A. Eleyan
1a. Positive and negative work
Example: The simple pendulum l Suppose we release a mass m from rest a distance h 1 above its lowest possible point. ç What is the maximum speed of the.
T101Q7. A spring is compressed a distance of h = 9.80 cm from its relaxed position and a 2.00 kg block is put on top of it (Figure 3). What is the maximum.
Principles of Physics - Foederer. Energy is stored in a spring when work is done to compress or elongate it Compression or elongation= change in length.
Discussions Feb 26 Work Conservation of energy. Work and conservation of energy.
Copyright © 2012 Pearson Education Inc. PowerPoint ® Lectures for University Physics, Thirteenth Edition – Hugh D. Young and Roger A. Freedman Lectures.
Energy – The capacity to do work
Physics 6A Work and Energy examples Prepared by Vince Zaccone For Campus Learning Assistance Services at UCSB.
WORK In order for work to be done, three things are necessary:
Bellringer 10/25 A 95 kg clock initially at rest on a horizontal floor requires a 650 N horizontal force to set it in motion. After the clock is in motion,
Chapter 5 Work, Energy, Power Work The work done by force is defined as the product of that force times the parallel distance over which it acts. The.
WORK AND ENERGY 1. Work Work as you know it means to do something that takes physical or mental effort But in physics is has a very different meaning.
Copyright © 2010 Pearson Education, Inc. Chapter 7 Work and Kinetic Energy.
ADV PHYSICS Chapter 5 Sections 2 and 4. Review  Work – force applied over a given distance W = F Δ x [W] = Joules, J  Assumes the force is constant.
Potential Energy and Conservative Forces
Chapter 5 Work and Energy. 6-1 Work Done by a Constant Force The work done by a constant force is defined as the distance moved multiplied by the component.
Energy m m Physics 2053 Lecture Notes Energy.
Chapter 8 - Potential Energy and Conservation of Energy Conservative vs. Non-conservative Forces Definition of Potential Energy Conservation Of Mechanical.
Review and then some…. Work & Energy Conservative, Non-conservative, and non-constant Forces.
Work and Energy. Work a force that causes a displacement of an object does work on the object W = Fdnewtons times meters (N·m) or joules (J)
Conservation of Energy
Physics 1D03 - Lecture 22 Potential Energy Work and potential energy Conservative and non-conservative forces Gravitational and elastic potential energy.
Conservative Forces: The forces is conservative if the work done by it on a particle that moves between two points depends only on these points and not.
2008 Physics 2111 Fundamentals of Physics Chapter 8 1 Fundamentals of Physics Chapter 8 Potential Energy & Conservation of Energy 1.Potential Energy 2.Path.
Conservation of Energy. Forms of Energy Mechanical Energy Thermal Energy Other forms include.
Physics 6A Work and Energy examples Prepared by Vince Zaccone For Campus Learning Assistance Services at UCSB.
Energy and Energy Conservation. Energy Two types of Energy: 1. Kinetic Energy (KE) - energy of an object due to its motion 2. Potential Energy (PE) -
Conservation of Energy. Conservative Force One for which work done does not depend on the path taken only on initial and final positions Gravity and elastic.
Phys211C7 p1 Kinetic Energy: Energy associated with motion K = ½ mv 2 Work done by a force on an object is that forces contribution to  K may only depend.
Lecture 11: Potential Energy & Energy Conservation.
Conservation of Energy
332 – UNIT 6 WORK & ENERGY.
Motion, Forces and Energy Lecture 7: Potential Energy & Conservation The name potential energy implies that the object in question has the capability of.
Work and Energy x Work and Energy 06.
Ch. 6, Work & Energy, Continued. Summary So Far Work-Energy Theorem: W net = (½)m(v 2 ) 2 - (½)m(v 1 ) 2   KE Total work done by ALL forces! Kinetic.
WHITE BOARD TIME !! CONSERVE ENERGY. E T = PE G + KE + PE S When comparing the energy at two different positions on a system, the total energy at one.
Potential Energy and Conservation of Energy
Lecture 12: Elastic Potential Energy & Energy Conservation.
1. Work [W] = N*m = J Units: Work done by forces that oppose the direction of motion will be negative. Work and energy A. PositiveB. NegativeC. Zero Example:
Chapter 8 Conservation of Energy EXAMPLES. Example 8.1 Free Fall (Example 8.1 Text book) Determine the speed of the ball at y above the ground The sum.
Conservation of Energy
Physics Section 5.2 Define and apply forms of mechanical energy. Energy is the ability to do work. Kinetic energy is the energy of an object due its motion.
Chapter 5 Work and Energy. Question A crate of mass 10 kg is on a ramp that is inclined at an angle of 30⁰ from the horizontal. A force with a magnitude.
Chapter 6 Work and Energy © 2014 Pearson Education, Inc. No need to write information in red.
1a. Positive and negative work
Solving Problems with Energy Conservation.
Work and energy 1. Work Wf = |fk| |Δx| cos(180°) = -|fk| |Δx| < 0
Work Done by a Constant Force
Chapter 5 Work and Energy
Ch. 10 slides WorkEnergy.ppt.
Unit 7: Work, Power, and Mechanical Energy.
Do Now: (Yesterday’s Atwood’s Machine)
Examples: Mechanical Energy Conservation
Potential Energy Problems
Unit 5 ENERGY.
Work, Energy, Power.
Energy Problems.
Presentation transcript:

Examples: Mechanical Energy Conservation

Example 8.3 – Spring Loaded Cork Gun Ball, mass m = 35 g = 0.035 kg in popgun is shot straight up with spring of unknown constant k. Spring is compressed yA = - 0.12 m, below relaxed level, yB = 0. Ball gets to a max height yC = 20.0 m above relaxed end of spring. (A) If no friction, find spring constant k. (B) Find speed of ball at point B. Ball starts from rest. Speeds up as spring pushes against it. As it leaves gun, gravity slows it down. System = ball, gun, Earth. Conservative forces are acting, so use Conservation of Mechanical Energy Initial kinetic energy K = 0. Choose gravitational potential energy Ug = 0 where ball leaves gun. Also elastic potential energy Ue= 0 there. At max height, again have K = 0. Choose Note: Need two types of potential energy!

Mechanical Energy is Conserved!! k = [2mg(yC – yA)/(yA)2] = 958 N/m For entire trip of ball, Mechanical Energy is Conserved!! or: KA + UA = KB + UB = KC + UC. At each point, U = Ug + Ue so, KA+ UgA+ UeA = KB+ UgB + UeB = KC + UgC + UeC (A) To find spring constant k, use: KA+ UgA+ UeA = KC + UgC + UeC or, 0 + mgyA + (½)k(yA)2 = 0 + mgyC + 0, giving k = [2mg(yC – yA)/(yA)2] = 958 N/m (B) To find ball’s speed at point B, use: KA+ UgA+ UeA = KB + UgB + UeB or, (½)m(vB)2 + 0 + 0 = 0 + mgyA + (½)k(yA)2 , giving (vB)2 = [k(yA)2/m] + 2gyA; or, (vB) = 19.8 m/s

Example: Toy Dart Gun + (½)k(x1)2 = (½)m(v2)2 + (½)k(x2)2 Mechanical energy conservation!  (½)m(v1)2 + (½)k(x1)2 = (½)m(v2)2 + (½)k(x2)2 Speed when ? leaves gun? x1 = 0.06 m, v1 = 0, m = 0.1 kg, k = 250 N/m x2 = 0, v2 = ? Find: v2 = 3 m/s ?

Example: Two Kinds of PE m =2.6 kg h =0.55 m Y = 0.15 m k = ? A two step problem: STEP 1: (a)  (b)  (½)m(v1)2 + mgy1 = (½)m(v2)2 + mgy2 v1 = 0, y1 = h = 0.55 m, y2 =0 . Find: v2 = 3.28 m/s STEP 2: (b)  (c) (both gravity & spring PE)  (½)m(v2)2+(½)k(y2)2+mgy2 = (½)m(v3)2 + (½)k(y3)2 + mgy3 y3 = Y = 0.15m, y2 = 0  (½)m(v2)2 = (½)kY2 - mgY Solve for k & get k = 1590 N/m ALTERNATE SOLUTION: (a)  (c) skipping (b) v1 = 0 v2 = ? v3 = 0

Section 8.3: Problems with Friction We had, in general: WNC = K + U WNC = Work done by non-conservative forces K = Change in KE U = Change in PE (conservative forces) Friction is a non-conservative force! So, if friction is present, we have (WNC  Wf) Wf = Work done by friction In moving through a distance d, force of kinetics friction fk does work Wf = - fkd

When friction is present, we have: Wf = -fkd = K + U = Kf – Ki + Uf – Ui Also now, K + U  Constant! Instead, Ki + Ui+ Wf = Kf + Uf OR: Ki + Ui - fkd = Kf+ Uf For gravitational PE: (½)m(vi)2 + mgyi = (½)m(vf)2 + mgyf + fkd For elastic or spring PE: (½)m(vi)2 + (½)k(xi)2 = (½)m(vf)2 + (½)k(xf)2 + fkd

Example: Roller Coaster with Friction m=1000 kg, d=400 m, y1=40 m, y2= 25 m, v1= y2 = 0, fk = ? (½)m(v1)2 + mgy1 = (½)m(v2)2 + mgy2 + fkd  fk= 370 N

Ex. 8.4 – Block Pulled on Rough Surface A block, mass m = 6 kg, is pulled by constant horizontal force F = 12 N. over a rough horizontal surface. Kinetic friction coefficient μk = 0.15. Moves a distance Δx = 3 m. Find the final speed.

Example 8.6 – Block – Spring System A mass m = 1.6 kg, is attached to ideal spring of constant k = 1,000 N/m. Spring is compressed x = - 2.0 cm = - 2  10-2 m & is released from rest. (A) Find the speed at x = 0 if there is no friction. (B) Find the speed at x = 0 if there is a constant friction force fk = 4 N.

Ex. 8.7 – Crate Sliding Down a Ramp Crate, mass m = 3.0 kg, starts from rest at height yi = 0.5 m & slides down a ramp, length d = 1.0 m & incline angle θ = 30°. Constant friction force fk = 5 N. Continues to move on horizontal surface after. (A) Find the speed at the bottom. (B) Assuming the same friction force, find the distance on then horizontal surface that the crate moves after it leaves the ramp.

Ex. 8.8 – Block-Spring Collision Block, mass m = 0.8 kg, gets initial velocity vA = 1.2 m/s to right. Collides with spring with constant k = 50 N/m. (A) If no friction, find the maximum compression distance xmax of spring after collision. (B) There is a constant friction force fk between block & surface. Coefficient of friction is μk = 0.5. Find the maximum compression distance xC now.

Ex. 8.9 – Connected Blocks in Motion Two blocks, masses m1 & m2, are connected by spring of constant k. m1 moves on horizontal surface with friction. Released from rest when spring is relaxed when m2 at height h above floor. Eventually stops when m2 is on floor. Calculate the kinetic friction coefficient μk between m1 & table.