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UW-Madison PHYSICS 207 - Physics 207, Lecture 13

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Physics 207, Lecture 13, Oct. 15EnergyExample of a conservative system: The simple pendulum.Example: The simple pendulum.Slide 5Slide 6Example The Loop-the-Loop … againSlide 8Example SkateboardSlide 10Potential Energy, Energy Transfer and PathSlide 12Slide 13Elastic vs. Inelastic CollisionsSlide 15Inelastic collision in 1-D: Example 1Slide 17Variable force devices: Hooke’s Law SpringsHome Exercise Hooke’s LawF-s relation for a single DNA moleculeMeasurement technique: optical tweezersForce vs. Energy for a Hooke’s Law springEnergy for a Hooke’s Law springEnergy diagramsSlide 27EquilibriumComment on Energy ConservationSlide 30Physics 207: Lecture 13, Pg 1Physics 207, Lecture 13, Oct. 15Goals:Goals:Assignment: Assignment: HW6 due Wednesday, Oct. 22HW6 due Wednesday, Oct. 22For Monday: Read all of Chapter 11For Monday: Read all of Chapter 11•Chapter 10Chapter 10 Understand the relationship between motion and energy Define Potential Energy in a Hooke’s Law spring Develop and exploit conservation of energy principlein problem solving•Chapter 11Chapter 11 Understand the relationship between force, displacement and workPhysics 207: Lecture 13, Pg 2EnergyIf only “conservative” forces are present, the total energy If only “conservative” forces are present, the total energy ((sum of potential, U, and kinetic energies, K) of a system) of a system is is conservedconservedFor an object in a gravitational “field” Emech = K + UK and U may change, but Emech = K + U remains a fixed value.Emech = K + U = constant Emech is called “mechanical energy”K ≡ ½ mv2U ≡ mgy ½ m vyi2 + mgyi = ½ m vyf2 + mgyfPhysics 207: Lecture 13, Pg 3Example of a conservative system: The simple pendulum.Suppose we release a mass m from rest a distance h1 above its lowest possible point.What is the maximum speed of the mass and where does this happen ?To what height h2 does it rise on the other side ?vh1h2mPhysics 207: Lecture 13, Pg 4Example: The simple pendulum.yy=0y=h1 What is the maximum speed of the mass and where does this happen ?E = K + U = constant and so K is maximum when U is a minimum.Physics 207: Lecture 13, Pg 5Example: The simple pendulum.vh1yy=h1y=0 What is the maximum speed of the mass and where does this happen ?E = K + U = constant and so K is maximum when U is a minimumE = mgh1 at topE = mgh1 = ½ mv2 at bottom of the swingPhysics 207: Lecture 13, Pg 6Example: The simple pendulum.yy=h1=h2y=0 To what height h2 does it rise on the other side?E = K + U = constant and so when U is maximum again (when K = 0) it will be at its highest point.E = mgh1 = mgh2 or h1 = h2Physics 207: Lecture 13, Pg 7ExampleThe Loop-the-Loop … againTo complete the loop the loop, how high do we have to let the release the car?Condition for completing the loop the loop: Circular motion at the top of the loop (ac = v2 / R) Use fact that E = U + K = constant !h ?RCar has mass mRecall that “g” is the source of the centripetal acceleration and N just goes to zero is the limiting case. Also recall the minimum speed at the top isgRvUb=mghU=mg2Ry=0Physics 207: Lecture 13, Pg 8ExampleThe Loop-the-Loop … againUse E = K + U = constantmgh + 0 = mg 2R + ½ mv2 mgh = mg 2R + ½ mgR = 5/2 mgRh = 5/2 RRgRvh ?Physics 207: Lecture 13, Pg 9What speed will the skateboarder reach halfway down the hill if there is no friction and the skateboarder starts at rest? Assume we can treat the skateboarder as a “point”Assume zero of gravitational U is at bottom of the hillR=10 m..m = 25 kgExampleSkateboard..R=10 m30°y=0Physics 207: Lecture 13, Pg 10What speed will the skateboarder reach halfway down the hill if there is no friction and the skateboarder starts at rest? Assume we can treat the skateboarder as “point”Assume zero of gravitational U is at bottom of the hillR=10 m..m = 25 kgExampleSkateboard..R=10 m30°Use E = K + U = constant Ebefore = Eafter0 + m g R = ½ mv2 + mgR (1-sin 30°) mgR/2 = ½ mv2 gR = v2  v= (gR)½ v = (10 x 10)½ = 10 m/sPhysics 207: Lecture 13, Pg 11Potential Energy, Energy Transfer and PathA ball of mass m, initially at rest, is released and follows three difference paths. All surfaces are frictionless 1. Ball is dropped2. Ball slides down a straight incline3. Ball slides down a curved inclineAfter traveling a vertical distance h, how do the three speeds compare?h(A) 1 > 2 > 3 (B) 3 > 2 > 1 (C) 3 = 2 = 1 (D) Can’t tell1 32Physics 207: Lecture 13, Pg 12Potential Energy, Energy Transfer and PathA ball of mass m, initially at rest, is released and follows three difference paths. All surfaces are frictionless 1. The ball is dropped2. The ball slides down a straight incline3. The ball slides down a curved inclineAfter traveling a vertical distance h, how do the three speeds compare?(A) 1 > 2 > 3 (B) 3 > 2 > 1 (C) 3 = 2 = 1 (D) Can’t tellh1 32Physics 207: Lecture 13, Pg 13Now what is the normal force on the skate boarder? R=10 m..m = 25 kgExampleSkateboard..R=10 m30° Fr = mar = m v2 / R = N – mg cos 60°N = m v2 /R + mg cos 60°N = 25 100 / 10 + 25 10 (0.87)N = 250 + 220 =470 Newtons..Nmg60°Physics 207: Lecture 13, Pg 14Elastic vs. Inelastic CollisionsA collision is said to be elastic when energy as well as momentum is conserved before and after the collision. Kbefore = Kafter Carts colliding with a perfect spring, billiard balls, etc.vviPhysics 207: Lecture 13, Pg 15Elastic vs. Inelastic CollisionsA collision is said to be inelastic when energy is not conserved before and after the collision, but momentum is conserved. Kbefore  Kafter Car crashes, collisions where objects stick together, etc.Physics 207: Lecture 13, Pg 16Inelastic collision in 1-D: Example 1A block of mass M is initially at rest on a frictionless horizontal surface. A bullet of mass m is fired at the block with a muzzle velocity (speed) v. The bullet lodges in the block, and the block ends up with a speed V.  What is the initial energy of the system ? What is the final energy of the system ? Is energy conserved?vVbefore afterxPhysics 207: Lecture 13, Pg 17Inelastic collision in 1-D: Example 1What is the momentum of the bullet with speed v ?  What is the initial energy of the system ? What is the final energy of the system ? Is momentum conserved (yes)?  Is energy conserved? Examine Ebefore-EaftervVbefore


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UW-Madison PHYSICS 207 - Physics 207, Lecture 13

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