Physical Pendulum, Torsion Pendulum
|
|
- Silvia Smith
- 5 years ago
- Views:
Transcription
1 [International Campus Lab] Physical Pendulum, Torsion Pendulum Objective Investigate the motions of physical pendulums and torsion pendulums. Theory Reference Young & Freedman, University Physics (14 th ed.), Pearson, Physical Pendulum (p.475~477) 9.4 Energy in Rotational Motion (p.307~312) 9.5 Parallel-Axis Theorem (p.312~313) 14.4 Application of SHM Angular SHM (p.471) When the body is released, it oscillates about its equilibrium position. The motion is not simple harmonic because the torque ττ zz is proportional to sin θθ rather than to θθ itself. However, if θθ is small, we can approximate sin θθ by θθ in radian. Then the motion is approximately simple harmonic. With this approximation, ττ zz = (mmggdd)θθ (2) 1. Physical Pendulum A physical pendulum is any real pendulum that uses an extended body, as contrasted to the idealized simple pendulum with all of its mass concentrated at a point. Figure 1 shows a body of irregular shape pivoted so that it can turn without friction about an axis through point OO. In equilibrium the center of gravity (cg) is directly below the pivot; in the position shown, the body is displaced from equilibrium by an angle θθ, which we use as a coordinate for the system. The distance from OO to the center of gravity is dd, the moment of inertia of the body about the axis of rotation through OO is II, and the total mass is mm. When the body is displaced as shown, the weight mmgg causes a restoring torque ττ zz = (mmgg)(dd sin θθ) (1) Fig. 1 The restoring torque on the body is proportional to sin θθ, not to θθ. However, for small θθ, sin θθ θθ, so the motion is approximately simple harmonic. 85 Songdogwahak-ro, Yeonsu-gu, Incheon 21983, KOREA ( ) Page 1 / 12
2 Using the rotational analog of Newton s second law for a rigid body, ττ zz = IIαα zz, we find A body doesn t have just one moment of inertia. In fact, it has infinitely many, because there are infinitely many axes about which it might rotate. But there is a simple relationship, (mmggdd)θθ = IIαα zz = II dd2 θθ dddd 2 dd 2 θθ dddd 2 = mmggdd θθ (3) II called the parallel-axis theorem, between II cm (moment of inertia of a body about an axis through its center of mass) and II PP (moment of inertia about any other axis parallel to the origin axis) (Fig. 3): Comparing this with the equation for SHM, aa xx = (kk mm)xx, we see that the role of (kk mm) for the spring-mass system is played here by the quantity (mmggdd II). Thus II PP = II cm + MMdd 2 (6) where MM is the mass of body and dd is the distance between two parallel axes. ωω = mmggdd II TT = 2ππ II mmggdd (4) (5) From Eqs. (5), (6) (mm = MM), II cm = (1 12)MMLL 2, and Fig. 4(a), the period TT of a slender rod with length LL is Figure 2 gives moments of inertia for several familiar shapes in terms of their masses and dimensions. Fig. 2(b) shows that TT = 2ππ LL2 + 12dd 2 12ggdd (7) the moment of inertia of a rectangular plate through center of mass is II cm = (1 12)MM(aa 2 + bb 2 ), however, if aa bb(= LL) then it approximately becomes II cm = (1 12)MMLL 2 as Fig. 2(a). From Eqs. (5), (6) (mm = MM), II cm = (1 2)MMRR 2, and Fig. 4(b), the period TT of a solid cylinder with radius RR is TT = 2ππ RR2 + 2dd 2 2ggdd (8) Fig. 2 Moments of Inertia of Various Bodies Fig. 3 The parallel-axis theorem. Fig. 4 Various physical pendulums 85 Songdogwahak-ro, Yeonsu-gu, Incheon 21983, KOREA ( ) Page 2 / 12
3 The balance disk has a moment of inertia II about its axis. The twisted steel wire exerts a restoring torque ττ zz that is proportional to the angular displacement θθ from the equilibrium position. We write ττ zz = κκκκ, where κκ is a constant called the torsion constant. Using the rotational analog of Newton s second law for a rigid body, ττ zz = IIαα zz = IIdd 2 θθ/ddtt 2, we find κκκκ = IIII or dd 2 θθ dddd 2 = κκ II θθ (9) Fig. 5 A graph of the period TT as a function of distance dd from the center of mass for a 50cm-length slender rod pendulum. This equation is exactly the same as aa xx = (kk mm)xx for simple harmonic motion, with xx replaced by θθ and kk mm replaced by κκ II. So we are dealing with a form of angular simple harmonic motion. The angular frequency ωω and period TT are given by ωω = kk mm and TT = 2ππ mm kk, respectively, with the same replacement: ωω = κκ II (10) TT = 2ππ II κκ (11) Fig. 6 A graph of the period TT as a function of distance dd from the center of mass for a 10cm-radius solid cylinder pendulum 2. Torsion Pendulum A restoring force on a body undergoing periodic motion originates in difference ways in difference situations. Figure 7 shows a kind of torsion pendulum which consists of an elastic object such as a thin steel wire. When it is twisted, it exerts a restoring torque in the opposite direction. Fig. 7 The steel wire exerts a restoring torque that is proportional to the angular displacement θθ, so the motion is angular SHM. 85 Songdogwahak-ro, Yeonsu-gu, Incheon 21983, KOREA ( ) Page 3 / 12
4 Equipment 1. List Item(s) Qty. Description PC / Software Data Analysis: Capstone 1 Records, displays and analyzes the data measured by various sensors. Interface 1 Data acquisition interface designed for use with various sensors, including power supplies which provide up to 15 watts of power. Force Sensor 1 Measures the magnitude of force. Range: 50N ~ 50N Resolution: 0.03N Rotary Motion Sensor (RMS) 1 Measures rotational or linear position, velocity and acceleration Slender Rod (or Long Rectangular Plate) 1 Length: 500mm Width: 20mm Pivot Point (Holes): 60, 100, 144, 190, 230mm from center of gravity Spherical Cylinder (or Disk) 1 Radius: 100mm Pivot Point (Holes): 30, 50, 70, 90mm from center of gravity Upper Wire Clamp Lower Wire Clamp 1 set Clamp wires. Wires (3 ea) (in the case) 1 set Exerts a restoring torque when twisted. Material: Steel Diameter: 0.8mm, 1.2mm, 1.6mm Balance Disk 1 Has a moment of inertia II = (1 2)MMRR 2 about its axis. 85 Songdogwahak-ro, Yeonsu-gu, Incheon 21983, KOREA ( ) Page 4 / 12
5 Item(s) Qty. Description A-shaped Base Support Rod (600mm) 1 set Provide stable support for experiment set-ups. Ruler 1 Measures length. String / Scissors Shared Exerts a torque to twist a wire. Electronic Balance Shared Measures mass. 2. Details (1) Force Sensor Refer to the Circular Motion and Centripetal Force lab manual. (2) Rotary Motion Sensor It contains a small photogate sensor and an optical code wheel on which dark bands are printed in line. As the shaft of the sensor rotates, the bands block the infrared beam of the photogate, which provides very accurate signals for positioning or timing. The Rotary Motion Sensor is a bidirectional angle sensor designed to measure rotational or linear position, velocity and acceleration. It includes a removable 3-step pulley with 10mm, 29mm, and 48mm diameters. This allows you to convert a linear motion into a rotational motion. 85 Songdogwahak-ro, Yeonsu-gu, Incheon 21983, KOREA ( ) Page 5 / 12
6 Procedure Experiment 1. Physical Pendulum (Slender Rod or Long Rectangular Plate) (1) Set up equipment. (3) Run Capstone software. 1 The interface automatically recognizes the RMS. Mount the RMS on the support rod so that the shaft of the sensor is horizontal (parallel to the table). 2 Adjust the sample rate of measurement. - [Rotary Motion Sensor]: Hz (2) Attach the slender rod to the RMS. Use the mounting thumbscrew to attach the slender rod to the shaft of the sensor through the end hole of the rod, so the pivot point is 230mm above the center of gravity. 3 Add a [Graph], and then select [Time(s)] for the xx-axis and [Angle(rad)] for the yy-axis. 85 Songdogwahak-ro, Yeonsu-gu, Incheon 21983, KOREA ( ) Page 6 / 12
7 (4) Begin recording data. Click [Record] and then let the pendulum swing. 1 With the pendulum on the equilibrium position, click [Record] to begin recording data. 2 Gently start the pendulum swinging with a small amplitude (within 5 ). 3 After 5~6 oscillations, click [Stop] to end recording data. 3 Repeat measuring times for all oscillations and find the period of oscillation. Also, calculate and record the theoretical period of oscillation based on the length dd from the pivot point to the center of gravity TT average (s) TT theory (s) tt nn (s) TT = tt nn tt nn 1 (s) (5) Find the period TT of oscillation. 1 Choose any reference point of measurement (for example, peaks or zero up-crossings). TT = 2ππ LL2 + 12dd 2 12ggdd LL = 500mm dd = 230, 190, 144, 100, 60mm (7) 2 Use [Show coordinate ] to read off the time of the point. (6) Repeat measurement. Repeat steps (4) and (5) for the holes that are dd = 230mm, 190mm, 144mm, 100mm, and 60mm from the center hole. (7) Plot a TT-dd graph. Using your results in step (6), plot a TT-dd graph and compare it with Fig. 5 in Theory section. 85 Songdogwahak-ro, Yeonsu-gu, Incheon 21983, KOREA ( ) Page 7 / 12
8 Experiment 3. Torsion Constant Q How does the period of this pendulum change when the pivot point moves towards the center of gravity? If it does not steadily increase or decrease, at what pivot point does the pendulum have minimum TT. Also, use Eq. (7) to calculate dd under the condition of minimum TT, and compare the theoretical value with your result. (1) Set up your equipment. A Q When the amplitude of this physical pendulum increases, should its period increase or decrease? Why? A 1 Slip the lower wire clamp onto the support rod. 2 Clamp the RMS at the top of the support rod so that the Experiment 2. Physical Pendulum (Solid Cylinder) Repeat the procedure of expt. 1 using a disk. shaft of the sensor is vertical. 3 Align the guide of the upper wire clamp with the slot of the shaft of the RMS. Slide the upper wire clamp onto the shaft and firmly tighten the thumbscrew. 4 Clamp each ends of the wire under the thumbscrew of the upper/lower wire clamp. Be sure that the elbow of the bend in the wire fits snugly against the axle of the thumbscrew. 5 Connect the sensors to the interface. TT = 2ππ RR2 + 2dd 2 2ggdd (8) RR = 100 mm dd = 90, 70, 50, 30 mm 85 Songdogwahak-ro, Yeonsu-gu, Incheon 21983, KOREA ( ) Page 8 / 12
9 6 Wind a string around the largest pulley. (2) Set up Capstone software. 1 Configure the Rotary Motion Sensor. - Click the RMS icon and then click the properties button ( ). - Select [Large Pulley (Groove)] for [Linear Accessory]. - [Change Sign] switches the sign of collected RMS data, which depends on the setup status or the rotational direction of the shaft. Check [Change Sign] if required. Caution When you slide the 3-step pulley onto the shaft of the RMS, be sure to align the guide of the pulley with the slot of the shaft. 2 Configure the Force Sensor. Caution If the retaining ring of the sensor shaft gets entangled in a string, SLOWLY and CAREFULLY remove the string. (NEVER apply a firm quick jerk to the string, which causes the retaining ring to warp, and as a result, the sensor to fail.) If it becomes warped, suspend your experiment immediately and visit lab office to replace the sensor. - Click the FS icon and then click the properties button ( ). - Check [Change Sign]. (The sign of FS data is initially negative for the pulling force.) 85 Songdogwahak-ro, Yeonsu-gu, Incheon 21983, KOREA ( ) Page 9 / 12
10 3 Configure calculator. (4) Begin recording data. Define the torque ττ as below, where [Force(N)] is measured data by the Force Sensor, and r is the radius of the 3 rd (largest) pulley (= 24mm). Hold the force sensor parallel to the table at the height of the largest pulley and slowly pull it straight out. If the angle shows negative, change the sign of RMS output (see step (2)-1). 4 Add a graph. Select [Rotary Motion Sensor Angle(rad)] for the xx-axis and [ττ(nm)] (defined in step3) for the yy-axis. (5) Analyze your graph. Find the torsion constant κκ. (3) Zero the Force Sensor. 1 Click [Select range(s) ] icon and then drag the data range of interest. NOTE To zero the sensor, press the [Zero] button on it WITH NO FORCE exerted on the sensor hook. 85 Songdogwahak-ro, Yeonsu-gu, Incheon 21983, KOREA ( ) Page 10 / 12
11 2 Click [Select curve fits ] and select [Linear: mt+b] to find linear fit for selected data points. The torsion constant κκ is equal to the slope of the ττ-θθ graph. (2) Set up your equipment. Use the setup detailed in expt. 3. Remove the string and attach the balance disk to the 3-step pulley with the thumbscrew. (Be careful not to attach the disk directly on the shaft without the pulley.) (6) Repeat measurement for other wires. Repeat steps (4) to (5) using other wires. (3) Configure Capstone software. Follow the setup instruction of the experiment 1. Change [Sample Rate] to Hz or Hz. Experiment 4. Torsion Pendulum (Angular SHM) (4) Begin recording data. (1) Calculate the moment of inertia of the balance disk. Measure the radius and the mass of the balance disk and calculate the theoretical value of II. (Suppose the balance disk is a perfect solid cylinder and apply the relationship II = (1 2)MMRR 2.) Click [Record]. Twist the balance disk about 120~180 and release it. Keep recording data for about 5-6 oscillations and stop recording data. Determine the time for each period of oscillation and verify Eq. (11). TT = 2ππ II κκ (11) (5) Change the wire and repeat step (4). 85 Songdogwahak-ro, Yeonsu-gu, Incheon 21983, KOREA ( ) Page 11 / 12
12 Result & Discussion Your TA will inform you of the guidelines for writing the laboratory report during the lecture. End of LAB Checklist Please put your equipment in order as shown below. Delete your data files from your lab computer. Turn off your lab Computer. Tighten all thumbscrews in position. Put the Wires in the storage case. Leave the Spools of String, Scissors in the basket on the lecture table. 85 Songdogwahak-ro, Yeonsu-gu, Incheon 21983, KOREA ( ) Page 12 / 12
Physical Pendulum Torsion Pendulum
General Physics Lab Department of PHYSICS YONSEI University Lab Manual (Lite) Physical Pendulum / Torsion Pendulum Ver.20180424 NOTICE This LITE version of manual includes only experimental procedures
More informationSimple Harmonic Motion
[International Campus Lab] Objective Investigate simple harmonic motion using an oscillating spring and a simple pendulum. Theory ----------------------------- Reference -------------------------- Young
More informationCircular Motion and Centripetal Force
[For International Campus Lab ONLY] Objective Measure the centripetal force with the radius, mass, and speed of a particle in uniform circular motion. Theory ----------------------------- Reference --------------------------
More informationGyroscope. Objective. Theory. 1. Torque. 2. Angular Momentum. Observe the motions of gyroscope.
[International Campus Lab] Objective Observe the motions of gyroscope. Theory ----------------------------- Reference -------------------------- Young & Freedman, University Physics (14 th ed.), Pearson,
More informationFree Fall and Projectile Motion
[International Campus] Free Fall and Projectile Motion Objective Investigate the motions of a freely falling body and a projectile under the influence of gravity. Find the acceleration due to gravity.
More informationSimple Harmonic Motion
1. Object Simple Harmonic Motion To determine the period of motion of objects that are executing simple harmonic motion and to check the theoretical prediction of such periods. 2. Apparatus Assorted weights
More informationvv d of the electrons. As a result, there is a net current in
[International Campus] Objective Investigate the effects of current, length of wire and magnetic field strength on a magnetic force. Theory ----------------------------- Reference --------------------------
More informationThe Torsion Pendulum (One or two weights)
The Torsion Pendulum (One or two weights) Exercises I through V form the one-weight experiment. Exercises VI and VII, completed after Exercises I -V, add one weight more. Preparatory Questions: 1. The
More informationPHYSICS LAB Experiment 9 Fall 2004 THE TORSION PENDULUM
PHYSICS 83 - LAB Experiment 9 Fall 004 THE TORSION PENDULUM In this experiment we will study the torsion constants of three different rods, a brass rod, a thin steel rod and a thick steel rod. We will
More informationRotational Motion. 1 Purpose. 2 Theory 2.1 Equation of Motion for a Rotating Rigid Body
Rotational Motion Equipment: Capstone, rotary motion sensor mounted on 80 cm rod and heavy duty bench clamp (PASCO ME-9472), string with loop at one end and small white bead at the other end (125 cm bead
More informationHuman Arm. 1 Purpose. 2 Theory. 2.1 Equation of Motion for a Rotating Rigid Body
Human Arm Equipment: Capstone, Human Arm Model, 45 cm rod, sensor mounting clamp, sensor mounting studs, 2 cord locks, non elastic cord, elastic cord, two blue pasport force sensors, large table clamps,
More informationHB Coupled Pendulums Lab Coupled Pendulums
HB 04-19-00 Coupled Pendulums Lab 1 1 Coupled Pendulums Equipment Rotary Motion sensors mounted on a horizontal rod, vertical rods to hold horizontal rod, bench clamps to hold the vertical rods, rod clamps
More informationWilberforce Pendulum (One or two weights)
Wilberforce Pendulum (One or two weights) For a 1 weight experiment do Part 1 (a) and (b). For a 2 weight experiment do Part1 and Part 2 Recommended readings: 1. R.A.Serway and J.W.Jewett, Jr. Physics
More informationExperiment P30: Centripetal Force on a Pendulum (Force Sensor, Photogate)
PASCO scientific Physics Lab Manual: P30-1 Experiment P30: (Force Sensor, Photogate) Concept Time SW Interface Macintosh File Windows File centripetal force 30 m 500 or 700 P30 Centripetal Force P30_CENT.SWS
More informationSimple Harmonic Motion
Chapter 9 Simple Harmonic Motion In This Chapter: Restoring Force Elastic Potential Energy Simple Harmonic Motion Period and Frequency Displacement, Velocity, and Acceleration Pendulums Restoring Force
More informationMagnetic Fields. Experiment 1. Magnetic Field of a Straight Current-Carrying Conductor
General Physics Lab Department of PHYSICS YONSEI University Lab Manual (Lite) Magnetic Fields Ver.20181029 NOTICE This LITE version of manual includes only experimental procedures for easier reading on
More informationThe Torsion Pendulum
Page 1 of 9 The Torsion Pendulum Introduction: This experiment helps to relate many of the concepts that we see in everyday life. Damped oscillations and pendulums are an everyday occurrence. You will
More informationCoulomb s Law. Equipment list Qty Item Part Number 1 Coulomb Balance ES Voltage Suppy. Purpose
Coulomb s Law Equipment list Qty Item Part Number 1 Coulomb Balance ES-9070 1 Voltage Suppy Purpose In this lab we will be examining the forces that stationary charges particles exert on one another to
More informationRotational Dynamics Smart Pulley
Rotational Dynamics Smart Pulley The motion of the flywheel of a steam engine, an airplane propeller, and any rotating wheel are examples of a very important type of motion called rotational motion. If
More information13-Nov-2015 PHYS Rotational Inertia
Objective Rotational Inertia To determine the rotational inertia of rigid bodies and to investigate its dependence on the distance to the rotation axis. Introduction Rotational Inertia, also known as Moment
More informationThe University of Hong Kong Department of Physics. Physics Laboratory PHYS3350 Classical Mechanics Experiment No The Physical Pendulum Name:
The University of Hong Kong Department of Physics Physics Laboratory PHYS3350 Classical Mechanics Experiment No. 3350-2 The Physical Pendulum Name: University No: Introduction One of the practical uses
More informationSHM Simple Harmonic Motion revised May 23, 2017
SHM Simple Harmonic Motion revised May 3, 017 Learning Objectives: During this lab, you will 1. communicate scientific results in writing.. estimate the uncertainty in a quantity that is calculated from
More informationOscillations. Oscillations and Simple Harmonic Motion
Oscillations AP Physics C Oscillations and Simple Harmonic Motion 1 Equilibrium and Oscillations A marble that is free to roll inside a spherical bowl has an equilibrium position at the bottom of the bowl
More informationE X P E R I M E N T 11
E X P E R I M E N T 11 Conservation of Angular Momentum Produced by the Physics Staff at Collin College Copyright Collin College Physics Department. All Rights Reserved. University Physics, Exp 11: Conservation
More informationSimple Harmonic Motion Investigating a Mass Oscillating on a Spring
17 Investigating a Mass Oscillating on a Spring A spring that is hanging vertically from a support with no mass at the end of the spring has a length L (called its rest length). When a mass is added to
More informationExperiment 11: Rotational Inertia of Disk and Ring
Experiment 11: Rotational Inertia of Disk and Ring Equipment Required ScienceWorkshop 750 Interface (CI- 6450 or CI-7599) Mini-Rotational Accessory (CI-6691) Base and Support Rod (ME-9355) Paper clips
More informationActivity P20: Conservation of Mechanical Energy (Force Sensor, Photogate)
Name Class Date Activity P20: Conservation of Mechanical Energy (Force Sensor, Photogate) Concept DataStudio ScienceWorkshop (Mac) ScienceWorkshop (Win) Energy P20 Mechanical Energy.DS P23 Cons. Mechanical
More informationWilberforce Pendulum (One or two weights)
Wilberforce Pendulum (One or two weights) For a 1 weight experiment do Part 1 (a) and (b). For a weight experiment do Part1 and Part Recommended readings: 1. PHY15 University of Toronto. Selected Material
More informationUnit 7: Oscillations
Text: Chapter 15 Unit 7: Oscillations NAME: Problems (p. 405-412) #1: 1, 7, 13, 17, 24, 26, 28, 32, 35 (simple harmonic motion, springs) #2: 45, 46, 49, 51, 75 (pendulums) Vocabulary: simple harmonic motion,
More informationSemester I lab quiz Study Guide (Mechanics) Physics 135/163
Semester I lab quiz Study Guide (Mechanics) Physics 135/163 In this guide, lab titles/topics are listed alphabetically, with a page break in between each one. You are allowed to refer to your own handwritten
More informationPhysics Labs with Computers, Vol. 1 P14: Simple Harmonic Motion - Mass on a Spring A
Activity P14: Simple Harmonic Motion - Mass on a Spring (Force Sensor, Motion Sensor) Concept DataStudio ScienceWorkshop (Mac) ScienceWorkshop (Win) Harmonic motion P14 SHM.DS P19 SHM Mass on a Spring
More informationPhysics 1050 Experiment 6. Moment of Inertia
Physics 1050 Moment of Inertia Prelab uestions These questions need to be completed before entering the lab. Please show all workings. Prelab 1 Sketch a graph of torque vs angular acceleration. Normal
More informationChapter 14: Periodic motion
Chapter 14: Periodic motion Describing oscillations Simple harmonic motion Energy of simple harmonic motion Applications of simple harmonic motion Simple pendulum & physical pendulum Damped oscillations
More informationOscillations. PHYS 101 Previous Exam Problems CHAPTER. Simple harmonic motion Mass-spring system Energy in SHM Pendulums
PHYS 101 Previous Exam Problems CHAPTER 15 Oscillations Simple harmonic motion Mass-spring system Energy in SHM Pendulums 1. The displacement of a particle oscillating along the x axis is given as a function
More informationLab 10 Circular Motion and Centripetal Acceleration
Lab 10 Circular Motion and Centripetal Equipment Calculator, Computer, PASCO 850 Universal Interface Partially-assembled Centripetal Force Apparatus Photogate Cable Pair of Banana Wires Objective Verify
More informationAngular Momentum. 1. Object. 2. Apparatus. 3. Theory
ngular Momentum. Object To verify conservation of angular momentum, determine the moment of inertia for various objects and look at the exchange of angular momentum in different situations.. pparatus rotational
More informationPeriodic Motion. Periodic motion is motion of an object that. regularly repeats
Periodic Motion Periodic motion is motion of an object that regularly repeats The object returns to a given position after a fixed time interval A special kind of periodic motion occurs in mechanical systems
More informationUpdated 2013 (Mathematica Version) M1.1. Lab M1: The Simple Pendulum
Updated 2013 (Mathematica Version) M1.1 Introduction. Lab M1: The Simple Pendulum The simple pendulum is a favorite introductory exercise because Galileo's experiments on pendulums in the early 1600s are
More informationPreLab 2 - Simple Harmonic Motion: Pendulum (adapted from PASCO- PS-2826 Manual)
Musical Acoustics Lab, C. Bertulani, 2012 PreLab 2 - Simple Harmonic Motion: Pendulum (adapted from PASCO- PS-2826 Manual) A body is said to be in a position of stable equilibrium if, after displacement
More informationPre-Lab Exercise Full Name:
L07 Rotational Motion and the Moment of Inertia 1 Pre-Lab Exercise Full Name: Lab Section: Hand this in at the beginning of the lab period. The grade for these exercises will be included in your lab grade
More informationLab 11 Simple Harmonic Motion A study of the kind of motion that results from the force applied to an object by a spring
Lab 11 Simple Harmonic Motion A study of the kind of motion that results from the force applied to an object by a spring Print Your Name Print Your Partners' Names Instructions April 20, 2016 Before lab,
More informationLAB #8: SIMPLE HARMONIC MOTION
OBJECTIVES: LAB #8: SIPLE HARONIC OTION To study the motion of two systems that closely resembles simple harmonic motion. EQUIPENT: Equipment Needed Qty Equipment Needed Qty Balance 1 Table Clamp w/rod
More informationLab 10 - Harmonic Motion and the Pendulum
Lab 10 Harmonic Motion and the Pendulum L10-1 Name Date Partners Lab 10 - Harmonic Motion and the Pendulum L (measured from the suspension point to the center of mass) Groove marking the center of mass
More informationActivity P08: Newton's Second Law - Constant Force (Force Sensor, Motion Sensor)
Activity P08: Newton's Second Law - Constant Force (Force Sensor, Motion Sensor) Concept DataStudio ScienceWorkshop (Mac) ScienceWorkshop (Win) Newton s Laws P08 Constant Force.DS P11 Constant Force P11_CONF.SWS
More informationExperiment P28: Conservation of Linear and Angular Momentum (Smart Pulley)
PASCO scientific Physics Lab Manual: P28-1 Experiment P28: Conservation of Linear and Angular Momentum (Smart Pulley) Concept Time SW Interface Macintosh File Windows File rotational motion 45 m 500 or
More informationPhysics 1020 Experiment 6. Equilibrium of a Rigid Body
1 2 Introduction Static equilibrium is defined as a state where an object is not moving in any way. The two conditions for the equilibrium of a rigid body (such as a meter stick) are 1. the vector sum
More informationEXPERIMENT 7: ANGULAR KINEMATICS AND TORQUE (V_3)
TA name Lab section Date TA Initials (on completion) Name UW Student ID # Lab Partner(s) EXPERIMENT 7: ANGULAR KINEMATICS AND TORQUE (V_3) 121 Textbook Reference: Knight, Chapter 13.1-3, 6. SYNOPSIS In
More informationCollege Physics I Laboratory Angular Momentum
College Physics I Laboratory Angular Momentum Purpose PHSX 206N To investigate conservation of angular momentum by directly measuring the moment of inertia and angular velocities for initial and final
More informationLab M4: The Torsional Pendulum and Moment of Inertia
M4.1 Lab M4: The Torsional Pendulum and Moment of Inertia Introduction A torsional pendulum, or torsional oscillator, consists of a disk-like mass suspended from a thin rod or wire. When the mass is twisted
More informationIntroduction to Simple Harmonic Motion
Introduction to Prelab Prelab 1: Write the objective of your experiment. Prelab 2: Write the relevant theory of this experiment. Prelab 3: List your apparatus and sketch your setup.! Have these ready to
More informationChapter 14 Oscillations. Copyright 2009 Pearson Education, Inc.
Chapter 14 Oscillations Oscillations of a Spring Simple Harmonic Motion Energy in the Simple Harmonic Oscillator Simple Harmonic Motion Related to Uniform Circular Motion The Simple Pendulum The Physical
More informationPhysics 2001/2051 The Compound Pendulum Experiment 4 and Helical Springs
PY001/051 Compound Pendulum and Helical Springs Experiment 4 Physics 001/051 The Compound Pendulum Experiment 4 and Helical Springs Prelab 1 Read the following background/setup and ensure you are familiar
More informationInclined Plane Dynamics Set
Instruction Manual 012-10874A *012-10874* Inclined Plane Dynamics Set ME-6966 Table of Contents Included Equipment..................................................... 3 Related Equipment.....................................................
More informationAP Physics. Harmonic Motion. Multiple Choice. Test E
AP Physics Harmonic Motion Multiple Choice Test E A 0.10-Kg block is attached to a spring, initially unstretched, of force constant k = 40 N m as shown below. The block is released from rest at t = 0 sec.
More informationActivity P24: Conservation of Linear and Angular Momentum (Photogate/Pulley System)
Name Class Date Activity P24: Conservation of Linear and Angular Momentum (Photogate/Pulley System) Concept DataStudio ScienceWorkshop (Mac) ScienceWorkshop (Win) Momentum P24 Linear Angular.DS P28 Cons
More informationPHYSICS 289 Experiment 1 Fall 2006 SIMPLE HARMONIC MOTION I
PHYSICS 289 Experiment 1 Fall 2006 SIMPLE HARMONIC MOTION I (A short report is required for this lab. Just fill in the worksheet, make the graphs, and provide answers to the questions. Be sure to include
More informationThe Damped Pendulum. Physics 211 Lab 3 3/18/2016
PHYS11 Lab 3 Physics 11 Lab 3 3/18/16 Objective The objective of this lab is to record the angular position of the pendulum vs. time with and without damping. The data is then analyzed and compared to
More informationSimple Harmonic Motion - MBL
Simple Harmonic Motion - MBL In this experiment you will use a pendulum to investigate different aspects of simple harmonic motion. You will first examine qualitatively the period of a pendulum, as well
More informationKinematics. Become comfortable with the data aquisition hardware and software used in the physics lab.
Kinematics Objective Upon completing this experiment you should Become comfortable with the data aquisition hardware and software used in the physics lab. Have a better understanding of the graphical analysis
More informationBallistic Pendulum. Equipment. Introduction. Setup
35 Ballistic Pendulum 35 - Page 1 of 5 Equipment Ballistic Pendulum 1 Rotary Motion Sensor PS-2120A 2 Photogate Head ME-9498A 1 Mounting Bracket ME-6821A 1 Large Table Clamp ME-9472 1 90 cm rod ME-8738
More informationLab 10: Harmonic Motion and the Pendulum
Lab 10 Harmonic Motion and the Pendulum 119 Name Date Partners Lab 10: Harmonic Motion and the Pendulum OVERVIEW A body is said to be in a position of stable equilibrium if, after displacement in any direction,
More informationActivity P15: Simple Harmonic Oscillation (Force Sensor, Photogate)
Activity P15: Simple Harmonic Oscillation (Force Sensor, Photogate) Concept DataStudio ScienceWorkshop (Mac) ScienceWorkshop (Win) Harmonic motion P15 Oscillation.DS P21 Harmonic Oscillation P21_HARM.SWS
More informationPhysics Labs with Computers, Vol. 1 P23: Conservation of Angular Momentum A
Activity P23: Conservation of Angular Momentum (Rotary Motion Sensor) Concept DataStudio ScienceWorkshop (Mac) ScienceWorkshop (Win) Rotational motion P23 Angular Momentum.DS (See end of activity) (See
More informationAP Physics C Mechanics Objectives
AP Physics C Mechanics Objectives I. KINEMATICS A. Motion in One Dimension 1. The relationships among position, velocity and acceleration a. Given a graph of position vs. time, identify or sketch a graph
More informationRotational Dynamics. Moment of Inertia of a point mass about an axis of rotation a distance r away: I m = mr 2
Rotational Dynamics Objective: To investigate the behavior of a rotating system subjected to internal torques and external torques. To apply knowledge gained from the linear momentum lab to its rotational
More informationMagnetic Force and Current Balance
Pre-Lab Quiz / PHYS 224 Magnetic Force and Current Balance Name Lab Section 1. What do you investigate in this lab? 2. Consider two parallel straight wires carrying electric current in opposite directions
More informationLAB 5: ROTATIONAL DYNAMICS
1 Name Date Day/Time of Lab Partner(s) Lab TA OBJECTIVES LAB 5: ROTATIONAL DYNAMICS To investigate and understand moment of inertia as it relates to rotational motion. To relate angular and linear position,
More informationPhysics for Scientists and Engineers 4th Edition, 2017
A Correlation of Physics for Scientists and Engineers 4th Edition, 2017 To the AP Physics C: Mechanics Course Descriptions AP is a trademark registered and/or owned by the College Board, which was not
More informationTOPIC E: OSCILLATIONS EXAMPLES SPRING Q1. Find general solutions for the following differential equations:
TOPIC E: OSCILLATIONS EXAMPLES SPRING 2019 Mathematics of Oscillating Systems Q1. Find general solutions for the following differential equations: Undamped Free Vibration Q2. A 4 g mass is suspended by
More informationMoment of inertia and angular acceleration
Principle A known torque is applied to a body that can rotate about a fixed axis with minimal friction. Angle and angular velocity are measured over the time and the moment of inertia is determined. The
More informationExp. #1-1 : Measurement of the Characteristics of the Centripetal Force by Using Springs and a Computer Interface
PAGE 1/13 Exp. #1-1 : Measurement of the Characteristics of the Centripetal Force by Using Springs and a Computer Interface Student ID Major Name Team No. Experiment Lecturer Student's Mentioned Items
More informationTeacher s notes 35 Conservation of angular momentum (1)
Sensors: Loggers: Rotary Motion Any EASYSENSE Physics Logging time: 10 seconds Teacher s notes 35 Conservation of angular momentum (1) Introduction The use of the disc accessories allows the Rotary Motion
More informationExperiment P26: Rotational Inertia (Smart Pulley)
PASCO scientific Physics Lab Manual P26-1 Experiment P26: (Smart Pulley) Concept Time SW Interface Macintosh file Windows file rotational motion 45 m 500 or 700 P26 P26_ROTA.SWS EQUIPMENT NEEDED Interface
More informationLAB 10: HARMONIC MOTION AND THE PENDULUM
163 Name Date Partners LAB 10: HARMONIC MOION AND HE PENDULUM Galileo reportedly began his study of the pendulum in 1581 while watching this chandelier swing in Pisa, Italy OVERVIEW A body is said to be
More information!T = 2# T = 2! " The velocity and acceleration of the object are found by taking the first and second derivative of the position:
A pendulum swinging back and forth or a mass oscillating on a spring are two examples of (SHM.) SHM occurs any time the position of an object as a function of time can be represented by a sine wave. We
More informationLab Exercise #3: Torsion
Lab Exercise #3: Pre-lab assignment: Yes No Goals: 1. To evaluate the equations of angular displacement, shear stress, and shear strain for a shaft undergoing torsional stress. Principles: testing of round
More informationLaboratory Manual Experiment NE02 - Rotary Motions Department of Physics The University of Hong Kong
Laboratory Manual Experiment NE02 - Rotary Motions Department of Physics The University of Hong Kong In this set of experiments, the moment of inertia of rotating objects of different shapes and the law
More informationPHY 123 Lab 9 Simple Harmonic Motion
PHY 123 Lab 9 Simple Harmonic Motion (updated 11/17/16) The purpose of this lab is to study simple harmonic motion of a system consisting of a mass attached to a spring. You will establish the relationship
More informationName Class Date. Activity P21: Kinetic Friction (Photogate/Pulley System)
Name Class Date Activity P21: Kinetic Friction (Photogate/Pulley System) Concept DataStudio ScienceWorkshop (Mac) ScienceWorkshop (Win) Newton s Laws P21 Kinetic Friction.DS P25 Kinetic Friction P25_KINE.SWS
More informationTIphysics.com. Physics. Pendulum Explorations ID: By Irina Lyublinskaya
Pendulum Explorations ID: 17 By Irina Lyublinskaya Time required 90 minutes Topic: Circular and Simple Harmonic Motion Explore what factors affect the period of pendulum oscillations. Measure the period
More informationMULTIPLE CHOICE. Choose the one alternative that best completes the statement or answers the question.
Exam Name MULTIPLE CHOICE. Choose the one alternative that best completes the statement or answers the question. 1) A 4.8-kg block attached to a spring executes simple harmonic motion on a frictionless
More informationDriven Harmonic Oscillator
Driven Harmonic Oscillator Physics 6B Lab Experiment 1 APPARATUS Computer and interface Mechanical vibrator and spring holder Stands, etc. to hold vibrator Motion sensor C-209 spring Weight holder and
More informationLab Partner(s) TA Initials (on completion) EXPERIMENT 7: ANGULAR KINEMATICS AND TORQUE
TA name Lab section Date TA Initials (on completion) Name UW Student ID # Lab Partner(s) EXPERIMENT 7: ANGULAR KINEMATICS AND TORQUE 117 Textbook Reference: Walker, Chapter 10-1,2, Chapter 11-1,3 SYNOPSIS
More informationFundamentals Physics. Chapter 15 Oscillations
Fundamentals Physics Tenth Edition Halliday Chapter 15 Oscillations 15-1 Simple Harmonic Motion (1 of 20) Learning Objectives 15.01 Distinguish simple harmonic motion from other types of periodic motion.
More informationRotational Dynamics. Goals and Introduction
Rotational Dynamics Goals and Introduction In translational dynamics, we use the quantities displacement, velocity, acceleration, mass and force to model the motion of objects. In that model, a net force
More information2007 Problem Topic Comment 1 Kinematics Position-time equation Kinematics 7 2 Kinematics Velocity-time graph Dynamics 6 3 Kinematics Average velocity
2007 Problem Topic Comment 1 Kinematics Position-time equation Kinematics 7 2 Kinematics Velocity-time graph Dynamics 6 3 Kinematics Average velocity Energy 7 4 Kinematics Free fall Collisions 3 5 Dynamics
More informationPHYSICS 107 FINAL EXAMINATION
PRINTED NAME: Problem Score 1 /20 2 /20 3 /20 4 /20 5 /20 6 /20 Total /120 PHYSICS 107 FINAL EXAMINATION January 24, 2001 8:30 11:30 am When you are told to begin, check that this examination booklet contains
More informationCHAPTER 12 OSCILLATORY MOTION
CHAPTER 1 OSCILLATORY MOTION Before starting the discussion of the chapter s concepts it is worth to define some terms we will use frequently in this chapter: 1. The period of the motion, T, is the time
More informationSecond Law. In this experiment you will verify the relationship between acceleration and force predicted by Newton s second law.
Second Law Objective In this experiment you will verify the relationship between acceleration and force predicted by Newton s second law. Apparatus Table clamp, Vertical rod, Right-angle clamp, Horizontal
More informationChapter 14 Periodic Motion
Chapter 14 Periodic Motion 1 Describing Oscillation First, we want to describe the kinematical and dynamical quantities associated with Simple Harmonic Motion (SHM), for example, x, v x, a x, and F x.
More informationPhysics 4A Lab: Simple Harmonic Motion
Name: Date: Lab Partner: Physics 4A Lab: Simple Harmonic Motion Objective: To investigate the simple harmonic motion associated with a mass hanging on a spring. To use hook s law and SHM graphs to calculate
More informationLab M1: The Simple Pendulum
Spring 2003 M1.1 Introduction. Lab M1: The Simple Pendulum The simple pendulum is a favorite introductory exercise because Galileo's experiments on pendulums in the early 1600s are usually regarded as
More information6. Find the net torque on the wheel in Figure about the axle through O if a = 10.0 cm and b = 25.0 cm.
1. During a certain period of time, the angular position of a swinging door is described by θ = 5.00 + 10.0t + 2.00t 2, where θ is in radians and t is in seconds. Determine the angular position, angular
More informationNewton s Second Law. Newton s Second Law of Motion describes the results of a net (non-zero) force F acting on a body of mass m.
Newton s Second Law Newton s Second Law of Motion describes the results of a net (non-zero) force F acting on a body of mass m. F net = ma (1) It should come as no surprise that this force produces an
More informationis acting on a body of mass m = 3.0 kg and changes its velocity from an initial
PHYS 101 second major Exam Term 102 (Zero Version) Q1. A 15.0-kg block is pulled over a rough, horizontal surface by a constant force of 70.0 N acting at an angle of 20.0 above the horizontal. The block
More informationPhysics lab Hooke s Law and Pendulums
Name: Date: Physics lab Hooke s Law and Pendulums Part A: Hooke s Law Introduction Hooke s Law explains the relationship between the force exerted on a spring, the stretch of the string, and the spring
More informationLAB 6: WORK AND ENERGY
93 Name Date Partners LAB 6: WORK AND ENERGY OBJECTIVES OVERVIEW Energy is the only life and is from the Body; and Reason is the bound or outward circumference of energy. Energy is eternal delight. William
More informationLab 11: Rotational Dynamics
Lab 11: Rotational Dynamics Objectives: To understand the relationship between net torque and angular acceleration. To understand the concept of the moment of inertia. To understand the concept of angular
More informationSummer Physics 41 Pretest. Shorty Shorts (2 pts ea): Circle the best answer. Show work if a calculation is required.
Summer Physics 41 Pretest Name: Shorty Shorts (2 pts ea): Circle the best answer. Show work if a calculation is required. 1. An object hangs in equilibrium suspended by two identical ropes. Which rope
More informationRotational Motion. Figure 1: Torsional harmonic oscillator. The locations of the rotor and fiber are indicated.
Rotational Motion 1 Purpose The main purpose of this laboratory is to familiarize you with the use of the Torsional Harmonic Oscillator (THO) that will be the subject of the final lab of the course on
More information