EXPERIMENT 8 BALLISTIC PENDULUM. Figure 1 Setup to determine the initial speed of the projectile using the Blackwood Pendulum

Similar documents
THE BALLISTIC PENDULUM AND THE LAW OF CONSERVATION OF ENERGY

The Ballistic Pendulum

Ballistic Pendulum and Projectile Motion

Lab 8: Ballistic Pendulum

Linear Momentum and Collisions Conservation of linear momentum

Ballistic Pendulum. Caution

Ballistic Pendulum. Equipment- ballistic pendulum apparatus, 2 meter ruler, 30 cm ruler, blank paper, carbon paper, masking tape, scale PRECAUTION

Energy in Collisions Problems AP Physics C

The Ballistic Pendulum

11 M36 M36.1 ANALYSIS OF A COMPLETELY INELASTIC COLLISION OBJECT The object of this experiment is to examine a completely inelastic collision between

Phy211: General Physics I Lab page 1 of 5 PCC-Cascade

PHYSICS LAB Experiment 8 Fall 2004 BALLISTIC PENDULUM

Physics 30 - Ballistic Pendulum Lab 2010, Science Kit All Rights Reserved

Your Thoughts. What is the difference between elastic collision and inelastic collision?

11 M36 M36.1 ANALYSIS OF A PERFECTLY INELASTIC COLLISION OBJECT The object of this experiment is to examine a perfectly inelastic collision between a

(a) Taking the derivative of the position vector with respect to time, we have, in SI units (m/s),

PHYS 1111L - Introductory Physics Laboratory I

Ballistic Pendulum (Inelastic Collision)

Lab 10: Ballistic Pendulum

AP Physics Chapter 9 QUIZ

Physics Kinematics: Projectile Motion. Science and Mathematics Education Research Group

Purpose of the experiment

10. Ballistic Pendulum*

AP Physics C. Momentum. Free Response Problems

12-Nov-17 PHYS Inelastic Collision. To study the laws of conservation of linear momentum and energy in a completely inelastic collision.

4 A mass-spring oscillating system undergoes SHM with a period T. What is the period of the system if the amplitude is doubled?

1 of 6 10/21/2009 6:33 PM

Experiment 4: Projectile Motion

Simple Harmonic Motion Practice Problems PSI AP Physics 1

A. unchanged increased B. unchanged unchanged C. increased increased D. increased unchanged

1. A tennis ball of mass m moving horizontally with speed u strikes a vertical tennis racket. The ball bounces back with a horizontal speed v.

A ballistic pendulum

AP Physics C: Mechanics Practice (Systems of Particles and Linear Momentum)

EXAM 3 MECHANICS 40% of the final grade

Ch 7 Impulse-Momentum Theorem, Conservation of Momentum, and Collisions

The world is charged with the grandeur of God.

2007 Problem Topic Comment 1 Kinematics Position-time equation Kinematics 7 2 Kinematics Velocity-time graph Dynamics 6 3 Kinematics Average velocity

PHYSICS FORMULAS. A. B = A x B x + A y B y + A z B z = A B cos (A,B)

Ch 10 HW: Problem Spring Force

AP Physics Free Response Practice Oscillations

Conservation of Momentum in Two Dimensions

Ballistic Pendulum. Equipment. Introduction. Setup

Module 17: Systems, Conservation of Momentum and Center of Mass

Today s topic: IMPULSE AND MOMENTUM CONSERVATION

N12/4/PHYSI/SPM/ENG/TZ0/XX. Physics Standard level Paper 1. Tuesday 13 November 2012 (afternoon) 45 minutes INSTRUCTIONS TO CANDIDATES

CJ57.P.003 REASONING AND SOLUTION According to the impulse-momentum theorem (see Equation 7.4), F t = mv

Displacement, Time, Velocity

End-of-Chapter Exercises

Name ID Section. 1. One mile is equal to 1609 m; 1 hour is equal to 3600 s. The highway speed limit of 65 mph is equivalent to the speed of:

Elastic collisions in one dimension Mixed Exercise 4

Physics 2211 A & B Quiz #4 Solutions Fall 2016

Activity P24: Conservation of Linear and Angular Momentum (Photogate/Pulley System)

Conservation of Momentum

Simple Harmonic Motion Practice Problems PSI AP Physics B

Frames of Reference, Energy and Momentum, with

Potential Energy & Conservation of Energy

UNIVERSITY OF SASKATCHEWAN Department of Physics and Engineering Physics

8.01x Classical Mechanics, Fall 2016 Massachusetts Institute of Technology. Problem Set 8

Physics 4A Solutions to Chapter 4 Homework

CHAPTER 3: Kinematics in Two Dimensions; Vectors

11 M36 M36.1 ANALYSIS OF A PERFECTLY INELASTIC COLLISION The object of this experiment is to examine a perfectly inelastic collision between a steel

Physics 211: Lecture 14. Today s Agenda

E X P E R I M E N T 11

Lecture 12! Center of mass! Uniform circular motion!

Exercise 6: The conservation of energy and momentum

DEVIL PHYSICS THE BADDEST CLASS ON CAMPUS AP PHYSICS

Page 1. t F t m v. N s kg s. J F t SPH4U. From Newton Two New Concepts Impulse & Momentum. Agenda

Motion in Two and Three Dimensions

Lecture 11. Impulse/Momentum. Conservation of Momentum. Cutnell+Johnson: Impulse and Momentum

Motion in Two and Three Dimensions

Chapter 9. Linear Momentum and Collisions

Chap. 8: Collisions and Momentum Conservation

Experiment P28: Conservation of Linear and Angular Momentum (Smart Pulley)

CEE 271: Applied Mechanics II, Dynamics Lecture 17: Ch.15, Sec.2 4

4.) A baseball that weighs 1.6 N leaves a bat with a speed of 40.0 m/s. Calculate the kinetic energy of the ball. 130 J

Old Exams Questions Ch. 8 T072 Q2.: Q5. Q7.

King Fahd University of Petroleum and Minerals Department of Physics. Final Exam 041. Answer key - First choice is the correct answer

Physics Courseware Physics I Energy Conservation

Chapter 7. Impulse and Momentum

(D) Based on Ft = m v, doubling the mass would require twice the time for same momentum change

General Physics I Lab. M7 Conservation of Angular Momentum

LABORATORY VI. ROTATIONAL DYNAMICS

VISUAL PHYSICS ONLINE RECTLINEAR MOTION: UNIFORM ACCELERATION

Energy problems look like this: Momentum conservation problems. Example 8-1. Momentum is a VECTOR Example 8-2

Problems. 66 km/h B km/h 30 A. v A. 1.5 ft

Multiple Choice -- TEST III

AP Physics B Summer Assignment

An Introduction. Work

PHYS 1303 Final Exam Example Questions

frictionless horizontal surface. The bullet penetrates the block and emerges with a velocity of o

PHYS 1303 Final Exam Example Questions

(A) 10 m (B) 20 m (C) 25 m (D) 30 m (E) 40 m

FOCUS ON CONCEPTS Section 7.1 The Impulse Momentum Theorem

AP Mechanics Summer Assignment

Kinematics of Particles

Axis Balanced Forces Centripetal force. Change in velocity Circular Motion Circular orbit Collision. Conservation of Energy

CIRCULAR MOTION EXERCISE 1 1. d = rate of change of angle

14300 Dynamics Carts w/o Hoops Teachers Instructions

Center of Mass & Linear Momentum

Practice Problems for Exam 2 Solutions

Transcription:

EXPERIMENT 8 BALLISTIC PENDULUM I. Introduction. The objectie of this eperiment is to determine the initial elocity of a projectile fired from a gun by two methods. In the first the projectile undergoes an inelastic collision imbedding itself in the pendulum bob after which the projectile and body together rise to a height h as shown in Fig. 1. The laws of conseration of momentum and energy are used to work backward from the height data to the initial elocity of the projectile. The second method is to determine the initial elocity determined the horizontal range of the projectile when it is fired from the same gun. The two initial elocities and their respectie standard deiations are compared. Figure 1 Setup to determine the initial speed of the projectile using the Blackwood Pendulum 1. Determination of the initial elocity of the projectile from the Blackwood Ballistic Pendulum: The Blackwood pendulum is shown in Fig.1. A ball of mass m and elocity is fired into a pendulum bob of mass M and is embedded. The system of combined masses then moes away with an initial elocity V and rises until it reaches a maimum height h ma and stops. The restraining force of the rod at any point in the path is perpendicular to the elocity so it doesn t affect the magnitude of the elocity. In order to determine the elocity with which the ball is fired, it is necessary to use the principle of conseration of momentum and the principle of conseration of energy. The

m momentum of the ball before impact is. The instant after the collision the combined masses moe away with momentum m MV. The conseration of momentum requires m ( m M ) V (1) At collision, a significant fraction of the kinetic energy is dissipated into unrecoerable forms because the leaf spring in the bob is deformed, the friction between the ball and the bob, and sound waes. After the projectile is embedded in the bob and assuming no friction in the pendulum mount, the total mechanical energy is a constant. This can be seen from the general epression relating work and energy: K U K U h h h h ma ma () There is no eternal work done but the combined mass rises until it stops Kh ma so the conseration of energy yields 1 mmghma h mmv (3) Eliminating V using Eqs. (1) and (3), m M gh (4) ma h m All of the quantities on the right-hand side of the equation can be readily measured so the magnitude of is determined from these alues.. Determination of initial elocity from the Trajectory When a projectile is fired horizontally from a height y and strikes the ground or a table, a determination of the range proides the initial elocity of the projectile. Fig. shows the setup for the measurement. Figure. The trajectory for a projectile fire horizontally

The general equations of motion in two dimensions, (,y), for a mass in free fall and no acceleration along the horizontal component, are: and 1 y y y t gt t (6) (5) where and y are the initial displacements. If the projectile is fired horizontally, y =. Taking =, and eliminating the common parameter t of Eqs. (5), and (6), we can write: or y y g g y y If we measure from the point of impact, y = and = R, so that g y R (7) II Equipment and Procedure Equipment Procedure Ballistic Pendulum, paper, carbon paper, rubber mat 1. Ballistic Pendulum a. Detach the pendulum. Determine the mass of the pendulum and separately that of the projectile (ball). Record these masses. b. The pendulum has a small pawl at its base that moes smoothly oer a ertical stem with a cured serrated surface which catches a pawl on the pendulum bob as soon as it tries to return, that is, at its maimum height. Fire the projectile si times and record the position of the pawl on the serrated surface. Record which serration the pawl is on each time. Then determine the aerage position of the pawl on the serrated surface. c. Set the pendulum so that the pawl is on the aerage serration. There is a center of mass pointed on the housing of the pendulum. Measure the change in height

of the center of mass pointer on the pendulum at the aerage serration from its hanging position. Eq. 4 then yields the initial elocity of the projectile.. Trajectory Procedure. a. Leel the base of the gun and mark the position of the base so that it can be returned to that position if it moes. b. Measure the height of the bottom of the ball aboe the table. c. Fire the projectile a few times to see its approimate range on the table. Make sure the tension in the spring remains constant by tightening the knob at the end of the gun after each firing. Check the position of the base each time the gun is fired to make sure the position hasn t changed. Readjust the position of the base if necessary. After the range has been established, tape carbon backed paper in that range so the impact points can be determined. d. Fire the projectile si times and measure the impact position along the table from the un-cocked position of the ball to the middle of the point of impact on the table. Make sure the tension in the spring has remained constant by tightening the knob at the end of the gun after each firing and readjust the position of the base if necessary. Determine the aerage distance and the standard deiation of the mean of the distance. Use a backstop to aoid hitting other students or the wall.. III Data A. Ballistic Pendulum Trial Table 1. Height of Pawl in terms of Serration Pawl Height (Serration) B. Range Height y of the bottom of the ball aboe the table Table. Range of projectile fired from a height y and the differences from the aerage, R. Trial Ri Ri R R R i

IV. RESULTS A. Determine the aerage elocity of the projectile from for the Ballistic Pendulum procedure, Eq. (4) and the standard deiation from the aerage elocity m M m gh = m/s m/s B. Determine the aerage elocity of the projectile from the range procedure, Eq. (7) and the standard deiation from the aerage R m/s g y = = m/s C. Calculate the percent difference between the aerage elocities determined in A. and B. V. Conclusion and Discussion 1. Is the aerage initial elocity determined by the two methods consistent (a small percent difference)? If so, eamine the standard deiations of the mean for the two procedures. Do they indicate if one method is preferable? If one of the standard deiations is greater than the other what may be the cause?. Determine the kinetic energy of the system before impact and after the projectile has lodged in the pendulum. If there is a difference, account for it. 3. Does any friction present in the pendulum support change the height of the swing? 4. The pendulum system rotates after the collision. The kinetic energy of this rotating system has been neglected in the calculation of the kinetic energy. What effect does this hae on the determination of the height achieed by the bob? 5. Is the horizontal force on the pendulum is zero during the collision? What eidence do you hae that it is or is not?