TUTORIAL 1 SIMPLE HARMONIC MOTION Instructor: Kazumi Tolich About tutorials 2 ¨ ¨ ¨ ¨ Tutorials are conceptual exercises that should be worked on in groups. Each slide will consist of a series of questions that you should discuss with the students sitting around you. There will be a few clicker questions per session. Clicker questions are shown in red. There will be several teaching assistants wandering around the room to assist you. If you are having difficulty, they will ask you leading questions to help you understand the idea. I. Hook’s law for spring 3 SIMPLE HARMONIC MOTION ¨ Mech 79 A block of mass m on a frictionless surface is attached to an ideal spring, as shown in figure 1. I. The Hooke’s spring,law withfor a springs spring constant k, is fixed to the wall. The dashed line indicates the position A block of mass m on surface attached to an ideal massless spring, in of the right edge ofa frictionless the spring when theisspring is relaxed, and the block is atasitsshown equilibrium figure 1. The spring, which has spring constant k, is fixed to the wall. The dashed line indicates position. Figures 2 and 3 show the block held in place a distance A to the right and left of the the position of the right edge of the spring when the spring is neither stretched nor compressed respectively. andequilibrium the block isposition, at its equilibrium position. Block is at rest Block is at rest Block is at rest m m A Figure 1 Figure 2 m A Figure 3 Figures 2 and 3 show the block held in place a distance A to the right and left of the equilibrium position, respectively. SIMPLE HARMONIC MOTION Mech 79 I. Hook’s law for spring I. Hooke’s law for springs m A block of mass m on a frictionless surface is attached to an ideal massless spring, as shown in figure 1. The spring, which has spring constant k, is fixed to the wall. The dashed line indicates the position of the right edge of the spring when the spring is neither stretched nor compressed and the block is at its equilibrium position. 4 Figure 1 Block is at rest Block is at rest m A m A Figure 3 Figure 2 Block is at rest Figures 2 and 3 show the block held in place a distance A to the right and left of the equilibrium position, respectively. m m m A Figure 1 A A. In the boxes at right, draw arrows to represent Figure 3 Figure 2 the directions of: Arrows for figure 2 Arrows for figure 3 Position of block Position of block Force on block by spring Force on block by spring Figures 2 and 3 show the block held in place a distance A to the right and left of the equilibrium A. position, In therespectively. boxes at right, draw arrows to represent the directions =0 • the position of the block, x , taking xof: when the block is at its equilibrium position and ¤ The position of the block, 𝐱, taking 𝐱 = 0 when the block is at the equilibrium Arrows for figure 2 Arrows for figure 3 A. In the boxes at right, draw arrows to represent position. • the force on the block by the spring, F. the directions of: Position of block Position of block ⃗. ¤ The force on the block by theUse spring, the 𝐅 arrows that you drew to explain why the • the position of the block, x , taking x = 0 when minus sign is necessary insign the expression the block is at its equilibrium position and ¤ Use the arrows that you drew to explain why the minus is necessary in = –kx (Hooke’s law for an ideal spring). F • the force on the block by the spring, F. Force on block Force on block Hook’s law: 𝐅⃗ = −𝑘𝐱. Use the arrows that you drew to explain why the B. by spring by spring minus sign is necessary in the expression What is the net force on the block when it is held in place as shown in F = –kx (Hooke’s law for an ideal spring). figure 2? B. What is the net force on the block when it is held in place as shown in figure 2? Explain. B. What is the net force on the block when it is held in place as shown in figure 2? Explain. Quiz: T1-1 answer 5 ¨ ¨ ¨ The net force is zero. The block is not accelerating, so according to Newton's 2nd law, the net force on it is zero. ∑ 𝐅⃗ = 𝑚𝒂 SIMPLE HARMONIC MOTION I. Hook’s law for spring 6 Mech 79 I. Hooke’s law for springs A block of mass m on a frictionless surface is attached to an ideal massless spring, as shown in figure 1. The spring, which has spring constant k, is fixed to the wall. The dashed line indicates the position of the right edge of the spring when the spring is neither stretched nor compressed and the block is at its equilibrium position. Block is at rest Block is at rest Block is at rest m m A Figure 1 m A Figure 3 Figure 2 Figures 2 and 3 show the block held in place a distance A to the right and left of the equilibrium position, respectively. ¤ Suppose the hand in figure 2 were suddenly removed. After the hand is Arrows for figureon 2 Arrows figure 3 by the spring be related to the A. In the boxes at right, draw arrows to represent the removed, how would force the forblock the directions of: Position of block Position of block net force onx, the taking xblock? = 0 when • the position of the block, the block is at its equilibrium position and C. Use Newton’s second law to write an expression for the acceleration, 𝐚, of the block in terms of 𝐱, 𝑘, and 𝑚 for an instant after the block has been released. • the force on the block by the spring, F. Use the arrows that you drew to explain why the minus sign is necessary in the expression F = –kx (Hooke’s law for an ideal spring). Force on block by spring Force on block by spring B. What is the net force on the block when it is held in place as shown in figure 2? Explain. Mech 80 Simple harmonic motion II. Simple harmonic motion 7 ¨ A. Mech Simple harmonic motion II. Simple harmonic motion 80 A pendulum is hung directly above the block-spring system II.𝑚 Simple harmonic motion above the blockA pendulum with a mass is hung directly from section I. The block andisthe bob both have A pendulum hungpendulum directly above the block-spring system spring system from section I. The length of the pendulum 𝑙. from section I. The block and the pendulum bob both mass m. The spring constant is k, and the length of the ishave mass m. The spring constant is k, and the length of the Thependulum parameters theparameters systems been chosen such that is l.ofThe of the systems have been pendulum is have l. The parameters of the systems have been chosen such that the block is always directly below the that the block isbob. always below thechosen block issuch always directly below the directly pendulum bob.the pendulum pendulum bob. A. In the spaces below, draw a on vector to represent net Draw a vector to represent the net force the blocktheand force on each object when it is on the far left as shown. A. bob In the spaces a vector to represent the net the when it isbelow, on thedraw far left as shown. Net force on block Net force on bob force on each object when it is on the far left as shown. Net force on block Net force on bob l l m k m Equilibrium k position m m B. Suppose that the masses of the block and the pendulum bob were doubled, and the block and Equilibrium bob were then released from rest at the far left position. position The following questions serve as a guide to help you determine whether the block would remain directly below the pendulum bob at all times. Quiz: T1-2 answer Mech 80 8 ¨ ¨ ¨ Simple harmonic motion Simple harmonic motion The net force on the bob isII.tangent to its path A pendulum is hung directly above the block-spring system toward the equilibrium position. from section I. The block and the pendulum bob both have 𝐓 m. The spring constant is k, and the length of /0 the The bob is not acceleratingmass radially or pendulum is l. from The parameters of the systems have been chosenof suchacceleration that the block is always directly below the toward the pivot. The direction pendulum bob. does not have any component in the radial In the spaces below, draw a vector to represent the net direction. The component ofA. the in thewhen it is on the far left as shown. forceweight on each object radial direction is balanced withNetthe forcetension on block in Net force on bob the string. The weight of the bob has a component tangent to the path toward the equilibrium position. 𝐖/2 l m k m Equilibrium position B. Suppose that the masses of the block and the pendulum bob were doubled, and the block and bob were then released from rest at the far left position. The following questions serve as a guide to help you determine whether the block would remain directly below the pendulum bob at all times. II. Simple harmonic motion 9 ¨ ¨ 1. Suppose that the masses of the block and the pendulum bob were doubled, and the block and bob were then released from rest at the far left position. The following questions serve as a guide to help you determine whether the block would remain directly below the pendulum bob at all times. As a result of doubling the masses of the block and pendulum bob, would the following quantities increase by a factor of 2, decrease by a factor of 2, or remain the same? ¤ the magnitude of the net force on the block, 𝐹456, /9:;< , or the bob, 𝐹456, /:/ , when it is at the far left Quiz: T1-3 answer 10 ¨ ¨ increase by a factor of 2 The weight of the bob doubles, so does its component tangent to the path. 𝐓/0 𝐖/2 II. Simple harmonic motion 11 As a result of doubling the masses of the block and pendulum bob, 1. ¤ ¤ would the time it takes for each object to travel from the far left position to the equilibrium position, ∆𝑡/9:;< or ∆𝑡/:/ , increase, decrease, or remain the same? Check that your answers regarding ∆𝑡/9:;< and ∆𝑡/:/ are consistent with the relationships below: (Hint: For each object, what is the relationship between ∆𝑡 and the period of oscillation, 𝑇?) 2. 3. would the magnitude of the acceleration of each object, 𝑎/9:;< or 𝑎/:/ , when it is at the far left increase by a factor of 2, decrease by a factor of 2, or remain the same? ¤ 𝑇/9:;< = 2𝜋 𝑚⁄𝑘 (period of oscillation for a mass on a spring) ¤ 𝑇/:/ = 2𝜋 𝑙⁄𝑔 (period of oscillation for a simple pendulum) Will the block and pendulum bob still move together after their masses have been doubled? If not, describe what additional changes could be made so that the block and pendulum bob would again move together. Quiz: T1-4 answer 12 ¨ ¨ No The period of oscillation is increased by 2 for the block, but it remains the same for the bob. E F ¨ ∆𝑡/9:;< = 𝑇/9:;< = ¨ ∆𝑡/:/ = 𝑇/:/ = E F E F E F E G 2𝜋 𝑚⁄𝑘 = 𝜋 𝑚⁄𝑘 (depends on mass) E G 2𝜋 𝑙 ⁄𝑔 = 𝜋 𝑙 ⁄𝑔 (independent of mass) • Tbob = 2π l/g (period of oscillation for a simple pendulum) III. Energy of a simple harmonic oscillator 3. Will the block and pendulum bob still move together after their masses have been doubled? If not, describe what additional changes could be made so that the block and pendulum bob would again move together. 13 ¨ The diagram at right is a plot of the total III. Energy of a simple harmonic oscillator energy of a The horizontal block-spring system as diagram at right is a plot of the total energy of a block-spring system asblock a functionwith of the a function ofhorizontal the position of the position of the block with respect to its equilibrium The block oscillates with aThe maximum distance respect to itsposition. equilibrium position. block from equilibrium of A. oscillates withA. aWhat maximum distance from feature of the diagram shows that the total energy of the system is conserved as the block equilibrium of A. oscillates? E Etot -A B. Determine what fraction of the total energy is potential energy when the block is at (1) x = +A and (2) x = +A/2. (Hint: U = 1/2 kx2.) +A x oscillation, T?) • Tblock = 2π m/k (period of oscillation for a mass on a spring) III. Energy of a simple harmonic oscillator • Tbob = 2π l/g (period of oscillation for a simple pendulum) 14 A. B. C. D. What feature of the diagram shows is conserved as the block oscillates? 3. Will the block and pendulum bob still move together after their masses have been doubled? If not, describe what additional changes could be made so that the block and bob would again of move together. thatpendulum the total energy the system Determine what fraction of the total energy is potential energy, 𝑈 = III. Energy of a simple harmonic oscillator 1⁄2 𝑘𝑥 G , when the block is at 𝑥 =The+𝐴 and 𝑥 = + 𝐴⁄2. Plot the diagram at right is a plot of the total energy of a horizontal potential energy stored in the spring as ablock-spring function system of 𝑥.as a function of the E Etot position of the block with respect to its equilibrium maximum distance kinetic position. energyTheofblock theoscillates block,with 𝐾,aas a function from equilibrium of A. On the same axes, plot the of 𝑥. (Hint: What function must be added to the potential energy to A. What feature of the diagram shows that the total equal the total energy of the system?) Label so asthat you energy of theyour systemgraphs is conserved the block oscillates? can easily distinguish the kinetic energy 𝐾 from the potential energy 𝑈. Is the time that the block takes to move from 𝑥 = 0 to 𝑥 = + 𝐴⁄2 -A greater than, less than, or equal to the time that the block takes to move from 𝑥 = + 𝐴⁄2 to 𝑥 = +𝐴? Explain how your answer is total consistent B. Determine what fraction of the energy is potential energy when the block is at (1) x = +A and (2) x = +A/2. (Hint: U = 1/2 kx .) with your graph of the kinetic energy. +A 2 On the same axes above, plot the potential energy stored in the spring, U, as a function of x. x Quiz: T1-5 answer 15 ¨ ¨ ¨ ¨ Less than As the block moves from 𝑥 = 0 to 𝑥 = + 𝐴⁄2, the kinetic energy is always greater than its kinetic energy as the block moves from 𝑥 = + 𝐴⁄2 to 𝑥 = +𝐴. So, the speed of the block is also always greater than its as the block moves from 𝑥 = + 𝐴⁄2 to 𝑥 = +𝐴. The faster it moves, the less time it takes to cover the same distance. oscillation, T?) • Tblock = 2π m/k (period of oscillation for a mass on a spring) III. Energy of a simple harmonic oscillator • Tbob = 2π l/g (period of oscillation for a simple pendulum) 16 3. Will the block and pendulum bob still move together after their masses have been doubled? If not, describe what additional changes could be made so that the block and pendulum bob would again move together. Consider two points, P and Q, to the right of the block’s equilibrium position. Point P has position 𝑥 = + 𝐴⁄2. Point Q is the point for which the kinetic energy and the potential energy of III. Energy of a simple harmonic oscillator the system are each equal to half the total energy. The diagram at right is a plot of the total energy of a E. 1. 2. 3. horizontal system as a function of the Is point Q to the left of, to the right of, orblock-spring at the same position as point position of the block with respect to its equilibrium P? Mark the locations of points Pposition. and QThe onblock the oscillates 𝑥-axis above. with a maximum distance from equilibrium of A. When the block is at point P, is the kinetic energy of the system greater A. What feature of the diagram shows that the total than, less than, or equal to the potential energy? Explain how you can energy of the system is conserved as the block oscillates? tell from the graph. Calculate the ratio of the kinetic energy to the potential energy when the block is at point P (i.e., at 𝑥 = + 𝐴⁄2). E Etot -A +A B. Determine what fraction of the total energy is potential energy when the block is at (1) x = +A and (2) x = +A/2. (Hint: U = 1/2 kx2.) On the same axes above, plot the potential energy stored in the spring, U, as a function of x. x Quiz: T1-6 17 ¨ 3 ¨ The total mechanical energy is constant and given by 𝐸 = 𝑈 + 𝐾 = 𝑘𝐴G . ¨ E G This can be obtained at the turning point, where 𝐾 = 0, and all the mechanical energy is due to the potential energy. E O G G G E = 𝑘𝐴G . ¨ Potential energy at 𝑥 = + 𝐴⁄2 is 𝑈 = 𝑘 + ¨ Kinetic energy at 𝑥 = + 𝐴⁄2 is 𝐾 = 𝐸 − 𝑈 = 𝑘𝐴G − 𝑘𝐴G = 𝑘𝐴G . ¨ The ratio is R S = T VOW U X VOW U =3 P E E Q G P P oscillation, T?) • Tblock = 2π m/k (period of oscillation for a mass on a spring) III. Energy of a simple harmonic oscillator • Tbob = 2π l/g (period of oscillation for a simple pendulum) 18 3. Will the block and pendulum bob still move together after their masses have been doubled? If not, describe what additional changes could be made so that the block and pendulum bob would again move together. Suppose that the block were replaced by a block with half the mass and released from rest III. Energy of a simple harmonic oscillator at 𝑥 = +𝐴. The diagram at right is a plot of the total energy of a F. 1. 2. horizontal block-spring system as a function of the position of the block with respect to its equilibrium position. The block oscillates with a maximum distance from equilibrium of A. E Describe any resulting changes in the three energy graphs (𝐸6:6Z9 , 𝑈, 𝐾). Explain. A. What feature of the diagram shows that the total the system isof conserved as the block Is it possible to determineenergy the ofperiod oscillation oscillates? of a mass-spring system using information from -A energy graphs alone? If so, describe the steps you would take to determineB. the period. If ofnot, state Determine what fraction the total energy is potential energy when the block is at (1) x = +A and (2) x = +A/2. (Hint: U = 1/2 kx .) what other information you would need. Etot +A 2 On the same axes above, plot the potential energy stored in the spring, U, as a function of x. x Quiz: T1-7 answer 19 ¨ ¨ No From the amplitude and the total mechanical energy, you can determine the E E spring constant since at the turning point, 𝐸 = 𝑈 + 𝐾 = 𝑘𝐴G + 0 = 𝑘𝐴G . G ¨ But to determine the oscillation period, you need to know the mass: 𝑇/9:;< = 2𝜋 𝑚⁄𝑘. G III. Energy of a simple harmonic oscillator 20 Simple harmonic motion Mec 83 Suppose instead that the original block were released from rest ⁄2released at 𝑥 = − 𝐴⁄2 and movedG.between the positions 𝑥 =block −𝐴 and from rest at x = -A/2 and moved Suppose instead that the original were between the positions x = -A/2 and x = +A/2. 𝑥 = + 𝐴⁄2. G. 1. 2. 3. 4. E 1. As result of this change, woulddecrease, the total energy As a result of this change, would thea total energy increase, or increase, decrease, or remain the same? remain the same? Explain. Explain. On the axes at right, graph the total energy, 𝐸6:6Z9,45[ , potential energy 𝑈45[ , and kinetic energy 𝐾45[ for the new motion. Does any part of the new set of graphs exactly coincide with any part of the previous set of graphs? Explain. Is the time that the block takes to move from 𝑥 = 0 to 𝑥 = + 𝐴⁄2 2. to Onthe the time axes atthat right, graph the total greater than, less than, or equal the block tookenergy to move Etotal, new, potential energy Unew, and kinetic energy from 𝑥 = 0 to 𝑥 = + 𝐴⁄2 beforeKthe amplitude of oscillation was new for the new motion. reduced? Explain. Etot, old -A +A 3. Does any part of the new set of graphs exactly coincide with any part of the previous set of graphs? Explain. x Quiz: T1-8 answer 21 ¨ ¨ ¨ ¨ Greater than The total mechanical energy is reduced to 𝐸45[ = E 𝑘 G O G + G E F = 𝐸:9\ . The potential energy curve between 𝑥 = − 𝐴⁄2 and 𝑥 = + 𝐴⁄2 remains the same. So, the kinetic energy between 𝑥 = − 𝐴⁄2 and 𝑥 = + 𝐴⁄2 is always smaller in the new case than the old case, implying that the block is moving slower in the new case.
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