PIRATE SHIP EXAMPLE REPORT WRITE UP

Size: px
Start display at page:

Download "PIRATE SHIP EXAMPLE REPORT WRITE UP"

Transcription

1 PIRATE SHIP EXAMPE REPORT WRITE UP Title Aim period Pirate Ship investiation To find the relationship between the lenth of a pendulum and its Independent variable the lenth of the pendulum. I will use lenths of 0.00, 0.400, 0.600, 0.800, and 1.00m. Dependent variable the period of the pendulum (the time to swin from one side to the other and back aain) (MUST HAVE Independent and dependent variable for Achieved) Control variables (MUST HAVE for Merit/Excellence) 1. I will measure the lenth of the pendulum the same way: from the bottom of the cork that the strin is threaded throuh, to the centre of mass of the pendulum bob.. Use the same ruler all measurements. 3. Release the pendulum from the same anle each time (approximately 15 ) 4. Release the pendulum so that the it swins perpendicular to the slit in the cork that is holdin the strin. Accuracy improvement (MUST HAVE for Merit/Excellence) 1. I will time 10 oscillations and divide by 10 to et the time for one period. This will reduce the effect of random variations in my times.. I will repeat the timin measurement for each lenth 5 times and take the averae. 3. I will reduce parallax error when measurin lenth by makin sure I am viewin the scale at 90, and makin sure the ruler is close to the strins. Method 1. Set up the equipment as shown in the diaram.. Adjust the lenth of the strin to 0.00m 3. Hold the pendulum bob to the side, deflectin it by around 15 and let o 4. Time 10 oscillations and record the time 5. Repeat step 5 until 5 times are recorded. 6. Repeat steps to 6 for lenths of 0.400, 0.600, 0.800, and 1.00m. 7. Process results to enable a relationship to be worked out. C lam p Clamp R uler B ench enth Retort stand Heavy mass to prevent the wood frommovin Bench Mass

2 Results enth of strin, (m) for (m) Must have at least one for Achieved Averae for 10T (s) Rane for 10T (s) Must have T and error bars for Merit/Excellence for 10T Time for one period T (s) for T (s) Times for 10T (s) 0.00 ± ± ± ± ± ± Processin The unprocessed data above would not ive a straiht line raph. As T π T is proportional to, therefore I will need to raph T aainst to et a straiht line raph and work out the equation. enth of strins, (m) for (m) % Unc Abs Unc % Unc 0.00 ± % % ± % % ± % % ± % % ± % % ± % % % and processin optional for Merit/Excellence (as lon as you have correct Time and error bars on your raph) Graph on the next pae The absolute values for are too small to plot on the scale that I have used on my raph Gradient of best fit line (MUST HAVE for Achieved) Rise.5s Run 1.14 m Gradient.5/ (s/ m) Gradient of error line (MUST HAVE for Merit/Excellence) Rise.5s Run 1.06 m Gradient.5/ (s/ m) Difference between radient of best and error line Δradient (1sf) Gradient with.0 ±0.1 (s/ m) (MUST HAVE for Merit/Excellence)

3 Period (s) Period v square root of lenth.50 Error line MUST HAVE for Achieved.00 Error bars on each data point MUST HAVE for Merit/Excellence (can use larest Time for all Time error bars) Best fit line MUST HAVE for Achieved Square root lenth ( m) 3

4 Conclusion - For achieved level The relationship is stated and reconition that the experimental relationship is consistent with the theoretical relationship. In conclusion the period of the pendulum is related to the lenth of the pendulum by T.0 COMPARING, Method 1 Comparin my equation T.0 to the iven equation T π I can see that my radient value,.0, should be equal to π π and.01, which shows that my relationship is consistent with the theory. 9.8 COMPARING, Method Comparin my equation T.0 to the iven equation T π I can see that my radient value,.0, should be equal to π. Rearranin π.0 ives π , which shows that my relationship is consistent with the theory as my value for of 9.87 is close to the theory of

5 Conclusion - For Merit and Excellence level The relationship is stated and an appropriate comparison is made between the theoretical value of the radient and the equivalent experimental value. (Accept a comparison between a constant calculated from the radient and a theoretical value.) The comparison includes a consideration of uncertainties. In conclusion the period of the pendulum is related to the lenth of the pendulum by T (.0 ±0.1) The in the radient is due to the uncertainties that I accounted for durin the experiment and processin of the data. COMPARING, Method 1 Comparin my equation T (.0 ±0.1) to the iven equation T π I can see that my radient value,.0 ±0.1, is equal to π π π and This shows that althouh the value of my best fit line,.0, is slihtly lower than the theoretical value for the radient of.01, it is well within my rane of values for the radient which is 1.9 to.1. My values are between (1.9/.01)x10095% and (.1/.01)x100104% of the theoretical value. COMPARING, Method Comparin my equation T (.0 ±0.1) to the iven equation T π I can see that my radient value,.0 ±0.1, is equal to π So π.0 π Maximum value of radient.1 So π.1 π So Minimum value of radient 1.9 π 1.9 π This shows that althouh the value of iven by my best fit line, 9.87, is hiher than the theoretical value of 9.81, it is well within my rane of values which is 8.95 to My values are between (8.95/9.8)x10091% and (10.94/9.8)x10011% of the theoretical value. 5

6 Discussion For Excellence - markin schedule: The discussion shows evidence that the student has sufficient depth of understandin of the experimental process to be able address critical issues such as: 1. other variable(s) that could have chaned and sinificantly affected the results, and how they could have chaned the results. (Note that it is not enouh to just state the results would be inaccurate.). the limitations to the theory s applicability both in the practical situation and/or at extreme values of the independent variable. 3. any unexpected outcomes of the processin of the results and a suestion of how they could have been caused and the effect they had on the validity of the conclusion. (Note that the aspects discussed should not be what would normally be considered as mistakes in experimental procedure such as failin to fix a wobbly retort stand - nor should they relate to just standard experimental procedure.) The evidence may be shown in two statements that show ood understandin or at least three (dependin on the depth of the understandin shown) statements that each show some understandin. The discussion points should be well reasoned and include clear and loical links between what has happened and the effect it has had on the results/conclusion. SEE NEXT PAGE FOR EXAMPES T If the line is too steep then is too small <9.81 ine with radient that ives 9.81 If the line is too shallow then is too bi >9.81 6

7 Discussion - examples 1. Control variables that could have affected my experiment One of my control variables was makin sure that I always measured the lenth to the same position on the pendulum bob (i.e. to the centre of mass). If I did not do this, for example if I measured to the top of the pendulum bob, the actual lenth of the pendulum would have been loner than what I measured and the time periods would have been loner. EXTRA: This would affect the radient of my raph by makin it steeper than it should have been. As the radient is equal to π/ this would have iven a value of smaller than 9.81 ms -. a. imitations of the model compared to real life The formula would not apply in real life as the suspensions would be two steel beams, not strin. Because the steel beams have more mass, this would affect the position of the centre of mass, makin it much hiher up than my model. This would make the effective lenth in the real life situation shorter than the lenth to the ships centre of mass, makin its period shorter. b. imitations of the minimum and maximum values of the independent variable The minimum value for which this relationship will apply is limited by the size of the pendulum bob. The fishin sinker that I used is approximately 3.5cm lon, includin the eyelet used to attach the strin, so the pendulum lenth could not be adjusted to lenths shorter than that. 3. Unexpected outcomes of the processin/results (i.e. reasons why your radient / value for could be different to the theory, but NOT mistakes) As the mass swun back and forth it also spun. The spinnin caused the strin to untwist, increasin the lenth of. The increased lenth would cause the time period to be reater, increasin the value of the intercept. I intended to use parallax error reduction, but found it difficult to hold the ruler in place when measurin the loner lenths and ended up lookin down at the scale from above, leadin to the lenth of the pendulum bein loner than intended. This would have made the loner lenths too lon, and iven periods that were too lon. EXTRA: This would affect the radient of my raph by makin it steeper than it should have been. As the radient is equal to π/ this would have iven a value of smaller than 9.81 ms -. When I adjusted the lenth of the pendulum I wound it around the clamp. I noticed that for part of the swin the strin was loner as it swun away from the clamp and shorter when the strin was up aainst the clamp. As I measured from the top of the clamp this would have made the lenths too short for part of the swin and iven times that were shorter than they should have been. EXTRA: This would affect the radient of my raph by makin it shallower than it should have been. As the radient is equal to π/ this would have iven a value of reater than 9.81 ms -. WEAK EXCEENCE With my raph there is an intercept at T -0. s, implyin that the period is neative, which cannot happen. A possible reason for this is the way I timed the pendulum. I juded the end of the 10 oscillations by eye, but if I anticipated the end point too early, my times would be too short, and the periods would be shorter than they should be, causin the neative intercept. CANNOT INCUDE MISTAKES IN THIS SECTION - e.. I accidentally timed 9 oscillations instead of 10, or I accidentally measured 99cm instead of 100cm. 7

Experiment 1: Simple Pendulum

Experiment 1: Simple Pendulum COMSATS Institute of Information Technoloy, Islamabad Campus PHY-108 : Physics Lab 1 (Mechanics of Particles) Experiment 1: Simple Pendulum A simple pendulum consists of a small object (known as the bob)

More information

PHY 133 Lab 1 - The Pendulum

PHY 133 Lab 1 - The Pendulum 3/20/2017 PHY 133 Lab 1 The Pendulum [Stony Brook Physics Laboratory Manuals] Stony Brook Physics Laboratory Manuals PHY 133 Lab 1 - The Pendulum The purpose of this lab is to measure the period of a simple

More information

AS90774 (Physics 3.1) Carry out a practical physics investigation with guidance, that leads to a mathematical relationship (version 2)

AS90774 (Physics 3.1) Carry out a practical physics investigation with guidance, that leads to a mathematical relationship (version 2) Physics Exemplars AS90774 (Physics 3.1) Carry out a practical physics investigation with guidance, that leads to a mathematical relationship (version 2) Level 3, 5 credits. The following extracts from

More information

Experiment 3 The Simple Pendulum

Experiment 3 The Simple Pendulum PHY191 Fall003 Experiment 3: The Simple Pendulum 10/7/004 Pae 1 Suested Readin for this lab Experiment 3 The Simple Pendulum Read Taylor chapter 5. (You can skip section 5.6.IV if you aren't comfortable

More information

Conical Pendulum Linearization Analyses

Conical Pendulum Linearization Analyses European J of Physics Education Volume 7 Issue 3 309-70 Dean et al. Conical Pendulum inearization Analyses Kevin Dean Jyothi Mathew Physics Department he Petroleum Institute Abu Dhabi, PO Box 533 United

More information

Projectile Motion. Equipment: Ballistic Gun Apparatus Projectiles Table Clamps 2-meter Stick Carbon Paper, Scratch Paper, Masking Tape Plumb Bob

Projectile Motion. Equipment: Ballistic Gun Apparatus Projectiles Table Clamps 2-meter Stick Carbon Paper, Scratch Paper, Masking Tape Plumb Bob Purpose: To calculate the initial speed of a projectile by measurin its rane. To predict how far a projectile will travel when fired at different anles, and test these predictions. To predict what anle

More information

OSCILLATIONS

OSCILLATIONS OSCIAIONS Important Points:. Simple Harmonic Motion: a) he acceleration is directly proportional to the displacement of the body from the fixed point and it is always directed towards the fixed point in

More information

The Measurement of the Gravitational Constant g with Kater s Pendulum

The Measurement of the Gravitational Constant g with Kater s Pendulum e Measurement of te Gravitational Constant wit Kater s Pendulum Abstract A Kater s pendulum is set up to measure te period of oscillation usin a lamppotocell module and a ektronix oscilloscope. Usin repeated

More information

3.1. Types of Forces. Measuring Forces. Force Diagrams

3.1. Types of Forces. Measuring Forces. Force Diagrams 3.1 Fiure 1 Forces are all around you. dynamics the study of the causes of motion Types of Forces Forces are all around you, actin on every object that you see. The motion of cars, trucks, planes, and

More information

Problem Set: Fall #1 - Solutions

Problem Set: Fall #1 - Solutions Problem Set: Fall #1 - Solutions 1. (a) The car stops speedin up in the neative direction and beins deceleratin, probably brakin. (b) Calculate the averae velocity over each time interval. v av0 v 0 +

More information

Disclaimer: This lab write-up is not

Disclaimer: This lab write-up is not Disclaimer: This lab write-up is not to be copied, in whole or in part, unless a proper reference is made as to the source. (It is stronly recommended that you use this document only to enerate ideas,

More information

SECTION A Torque and Statics

SECTION A Torque and Statics AP Physics C Multiple Choice Practice Rotation SECTON A Torque and Statics 1. A square piece o plywood on a horizontal tabletop is subjected to the two horizontal orces shown above. Where should a third

More information

Energizing Math with Engineering Applications

Energizing Math with Engineering Applications Enerizin Math with Enineerin Applications Understandin the Math behind Launchin a Straw-Rocket throuh the use of Simulations. Activity created by Ira Rosenthal (rosenthi@palmbeachstate.edu) as part of

More information

Physics 20 Lesson 24 Simple Harmonic Motion Pendulums

Physics 20 Lesson 24 Simple Harmonic Motion Pendulums Physics 0 esson 4 Simple Harmonic Motion Pendulums Refer to Chapter 7 in Pearson for a discussion of simple harmonic motion. I. Simple Harmonic Motion A study of simple harmonic motion (SHM) will take

More information

Mathematical Analysis of Efficiencies in Hydraulic Pumps for Automatic Transmissions

Mathematical Analysis of Efficiencies in Hydraulic Pumps for Automatic Transmissions TECHNICAL PAPER Mathematical Analysis of Efficiencies in Hydraulic Pumps for Automatic Transmissions N. YOSHIDA Y. INAGUMA This paper deals with a mathematical analysis of pump effi ciencies in an internal

More information

Exemplar for Internal Achievement Standard. Physics Level 3 version 2

Exemplar for Internal Achievement Standard. Physics Level 3 version 2 Exemplar for Internal Achievement Standard Physics Level 3 version 2 This exemplar supports assessment against: Achievement Standard 91521 Carry out a practical investigation to test a physics theory relating

More information

RESISTANCE STRAIN GAGES FILLAMENTS EFFECT

RESISTANCE STRAIN GAGES FILLAMENTS EFFECT RESISTANCE STRAIN GAGES FILLAMENTS EFFECT Nashwan T. Younis, Younis@enr.ipfw.edu Department of Mechanical Enineerin, Indiana University-Purdue University Fort Wayne, USA Bonsu Kan, kan@enr.ipfw.edu Department

More information

MATHCHEM 1.0. By Madhavan Narayanan Graduate Student, Department of Chemistry, Temple University

MATHCHEM 1.0. By Madhavan Narayanan Graduate Student, Department of Chemistry, Temple University MATHCHEM.0 By Madhavan Narayanan Graduate Student, Department of Chemistry, Temple University Preface I dedicate this document to my beloved parents and my teachers without whom I would not have had the

More information

AAPT UNITED STATES PHYSICS TEAM AIP 2009

AAPT UNITED STATES PHYSICS TEAM AIP 2009 2009 F = ma Exam 1 AAPT UNITED STATES PHYSICS TEAM AIP 2009 2009 F = ma Contest 25 QUESTIONS - 75 MINUTES INSTRUCTIONS DO NOT OPEN THIS TEST UNTI YOU ARE TOD TO BEGIN Use = 10 N/k throuhout this contest.

More information

9. v > 7.3 mi/h x < 2.5 or x > x between 1350 and 5650 hot dogs

9. v > 7.3 mi/h x < 2.5 or x > x between 1350 and 5650 hot dogs .5 Etra Practice. no solution. (, 0) and ( 9, ). (, ) and (, ). (, 0) and (, 0) 5. no solution. ( + 5 5 + 5, ) and ( 5 5 5, ) 7. (0, ) and (, 0). (, ) and (, 0) 9. (, 0) 0. no solution. (, 5). a. Sample

More information

An improved calculation of the mass for the resonant spring pendulum

An improved calculation of the mass for the resonant spring pendulum An improved calculation of the mass for the resonant sprin pendulum Joseph Christensen a) Department of Physics, McMurry University, Abilene, Texas 79697 Received 8 January 00; accepted January 00 When

More information

Copyright 2012 Nelson Education Ltd. Chapter 2: Dynamics 2.6-1

Copyright 2012 Nelson Education Ltd. Chapter 2: Dynamics 2.6-1 Section.6: Physics Journal: The Physics of Downhill Skiin Section.6 Questions, pae 94 1. Answers may vary. Sample answers: Four forces that act on a downhill skier are the force of ravity, the normal force

More information

ARTICLE IN PRESS. Nuclear Instruments and Methods in Physics Research A

ARTICLE IN PRESS. Nuclear Instruments and Methods in Physics Research A Nuclear Instruments and Methods in Physics Research A 66 (29) 517 522 Contents lists available at ScienceDirect Nuclear Instruments and Methods in Physics Research A journal homepae: www.elsevier.com/locate/nima

More information

Circular_Gravitation_P1 [22 marks]

Circular_Gravitation_P1 [22 marks] Circular_Gravitation_P1 [ marks] 1. An object of mass m at the end of a strin of lenth r moves in a vertical circle at a constant anular speed ω. What is the tension in the strin when the object is at

More information

PHYS 124 Section A01 Final Examination Autumn 2006

PHYS 124 Section A01 Final Examination Autumn 2006 PHYS 14 Section A1 Final Examination Autumn 6 Name : S Student ID Number : Instructor : Marc de Montiny Time : Monday, December 18, 6 9: 11: AM Room : Tory Lecture (Turtle) TL-B Instructions : This booklet

More information

ONLINE: MATHEMATICS EXTENSION 2 Topic 6 MECHANICS 6.3 HARMONIC MOTION

ONLINE: MATHEMATICS EXTENSION 2 Topic 6 MECHANICS 6.3 HARMONIC MOTION ONINE: MATHEMATICS EXTENSION Topic 6 MECHANICS 6.3 HARMONIC MOTION Vibrations or oscillations are motions that repeated more or less reularly in time. The topic is very broad and diverse and covers phenomena

More information

Kinetics of a Reaction

Kinetics of a Reaction P.O. Box 219 Batavia, Illinois 60510 1-800-452-1261 flinn@flinnsci.com Visit our website at: www.flinnsci.com 2003 Flinn Scientific, Inc. All Rihts Reserved. Your Safer Source for Science Supplies Kinetics

More information

This is a repository copy of The effects of gas-phase and in-depth radiation absorption on ignition and steady burning rate of PMMA.

This is a repository copy of The effects of gas-phase and in-depth radiation absorption on ignition and steady burning rate of PMMA. This is a repository copy of The effects of as-phase and in-depth radiation absorption on inition and steady burnin rate of PMMA. White ose esearch Online UL for this paper: http://eprints.whiterose.ac.uk/9515/

More information

(a) 1m s -2 (b) 2 m s -2 (c) zero (d) -1 m s -2

(a) 1m s -2 (b) 2 m s -2 (c) zero (d) -1 m s -2 11 th Physics - Unit 2 Kinematics Solutions for the Textbook Problems One Marks 1. Which one of the followin Cartesian coordinate system is not followed in physics? 5. If a particle has neative velocity

More information

Linearized optimal power flow

Linearized optimal power flow Linearized optimal power flow. Some introductory comments The advantae of the economic dispatch formulation to obtain minimum cost allocation of demand to the eneration units is that it is computationally

More information

f 1. (8.1.1) This means that SI unit for frequency is going to be s 1 also known as Hertz d1hz

f 1. (8.1.1) This means that SI unit for frequency is going to be s 1 also known as Hertz d1hz ecture 8-1 Oscillations 1. Oscillations Simple Harmonic Motion So far we have considered two basic types of motion: translational motion and rotational motion. But these are not the only types of motion

More information

11 Free vibrations: one degree of freedom

11 Free vibrations: one degree of freedom 11 Free vibrations: one deree of freedom 11.1 A uniform riid disk of radius r and mass m rolls without slippin inside a circular track of radius R, as shown in the fiure. The centroidal moment of inertia

More information

Name Section Lab on Motion: Measuring Time and Gravity with a Pendulum Introduction: Have you ever considered what the word time means?

Name Section Lab on Motion: Measuring Time and Gravity with a Pendulum Introduction: Have you ever considered what the word time means? Name Section Lab on Motion: Meaurin Time and Gravity with a Pendulum Introduction: Have you ever conidered what the word time mean? For example what i the meanin of when we ay it take two minute to boil

More information

20. Given: m = 75 kg ; a! = 2.0 m/s 2 [up] Required: F! N Analysis:! F! y. = m a!. Choose up as the positive direction. Solution:! F! y. = m a!!

20. Given: m = 75 kg ; a! = 2.0 m/s 2 [up] Required: F! N Analysis:! F! y. = m a!. Choose up as the positive direction. Solution:! F! y. = m a!! Chapter Review, paes 100 105 Knowlede 1. (b). (a) 3. (c) 4. (a) 5. (d) 6. (a) 7. (d) 8. (c) 9. (b) 10. False. If only three force of equal manitude act on an object, the object may or may not have a non-zero

More information

1 CHAPTER 7 PROJECTILES. 7.1 No Air Resistance

1 CHAPTER 7 PROJECTILES. 7.1 No Air Resistance CHAPTER 7 PROJECTILES 7 No Air Resistance We suppose that a particle is projected from a point O at the oriin of a coordinate system, the y-axis bein vertical and the x-axis directed alon the round The

More information

Physical Properties: Identification of a Pure Liquid

Physical Properties: Identification of a Pure Liquid EXPERIMENT Physical Properties: Identification of a Pure Liquid 6 To identify an unknown liquid by comparin the experimental and theoretical boilin points and densities. OBJECTIVE A P P A R A T U S balance

More information

Core practical 9: Investigate the relationship between the force exerted on an object and its change of momentum

Core practical 9: Investigate the relationship between the force exerted on an object and its change of momentum Core practical 9 Teacher sheet Core practical 9: Objective To determine the momentum change of a trolley when a force acts on it, as a function of time Safety There are trolleys and masses in motion so

More information

Physics 18 Spring 2011 Homework 2 - Solutions Wednesday January 26, 2011

Physics 18 Spring 2011 Homework 2 - Solutions Wednesday January 26, 2011 Physics 18 Sprin 011 Homework - s Wednesday January 6, 011 Make sure your name is on your homework, and please box your final answer. Because we will be ivin partial credit, be sure to attempt all the

More information

UNIVERSITY OF SASKATCHEWAN Department of Physics and Engineering Physics

UNIVERSITY OF SASKATCHEWAN Department of Physics and Engineering Physics UNIVRSITY OF SASKATCHWAN Department of Physics and nineerin Physics Physics 115.3 MIDTRM TST October 3, 009 Time: 90 minutes NAM: (Last) Please Print (Given) STUDNT NO.: LCTUR SCTION (please check): 01

More information

UNIVERSITY OF SASKATCHEWAN Department of Physics and Engineering Physics

UNIVERSITY OF SASKATCHEWAN Department of Physics and Engineering Physics UNIVRSITY OF SASKATCHWAN Department of Physics and nineerin Physics Physics 115.3 MIDTRM TST Alternative Sittin October 009 Time: 90 minutes NAM: (Last) Please Print (Given) STUDNT NO.: LCTUR SCTION (please

More information

AS Physics Past Paper Questions

AS Physics Past Paper Questions AS Physics Past Paper Questions You may find the following useful for the uncertainty parts: Absolute Uncertainty If you only have one reading, or all repeat readings are the same, the absolute uncertainty

More information

Educational Objectives Determine which variable affects the frequency of a simple pendulum.

Educational Objectives Determine which variable affects the frequency of a simple pendulum. Physics Workshop Main Topic Subtopic Learning Level Technology Level Activity Type Motion Periodic Motion Middle Low Student Teacher s Notes Description: Test the length, mass, and amplitude of a pendulum

More information

Mathematics Extension 1 Time allowed: 2 hours (plus 5 minutes reading time)

Mathematics Extension 1 Time allowed: 2 hours (plus 5 minutes reading time) Name: Teacher: Class: FORT STREET HIGH SCHOOL 0 HIGHER SCHOOL CERTIFICATE COURSE ASSESSMENT TASK : TRIAL HSC Mathematics Extension Time allowed: hours (plus 5 minutes readin time) Syllabus Assessment Area

More information

Exemplar for Internal Achievement Standard. Physics Level 1

Exemplar for Internal Achievement Standard. Physics Level 1 Exemplar for internal assessment resource Physics for Achievement Standard 90935 Exemplar for Internal Achievement Standard Physics Level 1 This exemplar supports assessment against: Achievement Standard

More information

Practice exam-style paper

Practice exam-style paper Practice exam-style paper Paper 6 Alternative to Practical Write your answers on the question paper. The number of marks is given in brackets [ ] at the end of each question or part question. 1 A student

More information

Exam 2A Solution. 1. A baseball is thrown vertically upward and feels no air resistance. As it is rising

Exam 2A Solution. 1. A baseball is thrown vertically upward and feels no air resistance. As it is rising Exam 2A Solution 1. A baseball is thrown vertically upward and feels no air resistance. As it is risin Solution: Possible answers: A) both its momentum and its mechanical enery are conserved - incorrect.

More information

On the falling (or not) of the folded inextensible string

On the falling (or not) of the folded inextensible string On the fallin (or not) of the folded inextensible strin Tyler McMillen Proram in Applied and Computational Mathematics, Princeton University, Fine Hall, Princeton, NJ 8544-1 e-mail: mcmillen@princeton.edu

More information

Investigating a pendulum

Investigating a pendulum P3 3.6 Student practical sheet Investigating a pendulum The period of a pendulum is the time it takes to complete one swing. Different pendulums have different periods, so what determines the period of

More information

Answer Key Lesson 4: Mass vs. Volume: Proportions and Density

Answer Key Lesson 4: Mass vs. Volume: Proportions and Density Answer Key Lesson : ass vs. olume: Proportions and Density Student Guide ass vs. olume: Proportions and Density r. oreno s lass is experimentin with thins that sink and float. This piee of lay sinks in

More information

Lab 10: Harmonic Motion and the Pendulum

Lab 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 information

4.3. Solving Friction Problems. Static Friction Problems. Tutorial 1 Static Friction Acting on Several Objects. Sample Problem 1.

4.3. Solving Friction Problems. Static Friction Problems. Tutorial 1 Static Friction Acting on Several Objects. Sample Problem 1. Solvin Friction Problems Sometimes friction is desirable and we want to increase the coefficient of friction to help keep objects at rest. For example, a runnin shoe is typically desined to have a lare

More information

(A) (B) (C) (D) None of these

(A) (B) (C) (D) None of these Exercise OBJECTIVE PROBLEMS. Action and reaction (A) act on two different objects (C) have opposite directions. Which fiure represents the correct F.B.D. of rod of mass m as shown in fiure : (B) have equal

More information

2015 (A) Roll No. INTERMEDIATE PART-I (11 th CLASS)

2015 (A) Roll No. INTERMEDIATE PART-I (11 th CLASS) Number: 647 (1) Liht year is a unit of:- () he resultant of two forces 30 N and 40 N actin parallel to each other is:- (3) A ball is allowed to fall freely from certain heiht. It covers a distance in first

More information

Length & Time Question Paper 2

Length & Time Question Paper 2 Length & Time Question Paper 2 Level IGCSE Subject Physics Exam Board CIE Topic General Physics Sub-Topic Length & Time Paper Type Alternative to Practical Booklet Question Paper 2 Time Allowed: 60 minutes

More information

Physics 11 Fall 2012 Practice Problems 2 - Solutions

Physics 11 Fall 2012 Practice Problems 2 - Solutions Physics 11 Fall 01 Practice Problems - s 1. True or false (inore any effects due to air resistance): (a) When a projectile is fired horizontally, it takes the same amount of time to reach the round as

More information

Physics lab Hooke s Law and Pendulums

Physics 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 information

Expanded Knowledge on Orifice Meter Response to Wet Gas Flows

Expanded Knowledge on Orifice Meter Response to Wet Gas Flows 32 nd International North Sea Flow Measurement Workshop 21-24 October 2014 Expanded Knowlede on Orifice Meter Response to Wet Gas Flows Richard Steven, Colorado Enineerin Experiment Station Inc Josh Kinney,

More information

(C) 7 s. (C) 13 s. (C) 10 m

(C) 7 s. (C) 13 s. (C) 10 m NAME: Ms. Dwarka, Principal Period: #: WC Bryant HS Ms. Simonds, AP Science Base your answers to questions 1 throuh 3 on the position versus time raph below which shows the motion of a particle on a straiht

More information

Conical Pendulum: Part 2 A Detailed Theoretical and Computational Analysis of the Period, Tension and Centripetal Forces

Conical Pendulum: Part 2 A Detailed Theoretical and Computational Analysis of the Period, Tension and Centripetal Forces European J of Physics Education Volume 8 Issue 1 1309-70 Dean onical Pendulum: Part A Detailed heoretical and omputational Analysis of the Period, ension and entripetal orces Kevin Dean Physics Department,

More information

GRADE 11 EXAMINATION NOVEMBER EXAMINER: Mrs C Jacobsz. MODERATORs: Ms M Eastes, Mrs T Thorne and Mrs V Rixon

GRADE 11 EXAMINATION NOVEMBER EXAMINER: Mrs C Jacobsz. MODERATORs: Ms M Eastes, Mrs T Thorne and Mrs V Rixon GRADE 11 EXAMINATION NOVEMBER 2015 DURBAN GIRLS' COLLEGE MATHEMATICS PAPER 1 TIME: 3 HOURS 150 MARKS EXAMINER: Mrs C Jacobsz MODERATORs: Ms M Eastes, Mrs T Thorne and Mrs V Rion PLEASE READ THE FOLLOWING

More information

Dielectric characteristics of glass fibre reinforced plastics and their components

Dielectric characteristics of glass fibre reinforced plastics and their components Plasticheskie Massy, No. 11, 2004, pp. 20 22 Dielectric characteristics of lass fibre reinforced plastics and their components V. I. Sokolov, S. I. Shalunov, I. G. Gurtovnik, L. G. Mikheeva, and I. D.

More information

CHAPTER 1 NUMBER BASES MATHEMATICS 5

CHAPTER 1 NUMBER BASES MATHEMATICS 5 CHAPTER NUMBER BASES MATHEMATICS 5 Number Bases Students will be tauht to:. Underst use the concept of number in base two, eiht five. Students will be able to: (i) State zero, one, two, three,, as a number

More information

5 Shallow water Q-G theory.

5 Shallow water Q-G theory. 5 Shallow water Q-G theory. So far we have discussed the fact that lare scale motions in the extra-tropical atmosphere are close to eostrophic balance i.e. the Rossby number is small. We have examined

More information

Apparatus: Stopwatch, meter rule, a retort stand, clamp, string and pendulum bob.

Apparatus: Stopwatch, meter rule, a retort stand, clamp, string and pendulum bob. Pre-Lab Questions 2 Topic: Acceleration due to gravity, g Learning Outcomes: To enable the students to (i) state the general pattern of variation of g on earth based on latitude. (ii) state the reasons

More information

Design of Chevron Gusset Plates

Design of Chevron Gusset Plates 017 SEAOC CONENTION PROCEEDINGS Desin of Chevron Gusset Plates Rafael Sali, Director of Seismic Desin Walter P Moore San Francisco, California Leih Arber, Senior Enineer American Institute of Steel Construction

More information

Problem Set 5 Solutions

Problem Set 5 Solutions Problem Set 5 Solutions Dorian Abbot APM47 0/8/04. (a) We consider π θ π. The pendulum pointin down corresponds to θ=0 and the pendulum pointin up corresponds to θ π. Define ν θ. The system can be rewritten:

More information

2.3. PBL Equations for Mean Flow and Their Applications

2.3. PBL Equations for Mean Flow and Their Applications .3. PBL Equations for Mean Flow and Their Applications Read Holton Section 5.3!.3.1. The PBL Momentum Equations We have derived the Reynolds averaed equations in the previous section, and they describe

More information

Stochastic simulations of genetic switch systems

Stochastic simulations of genetic switch systems Stochastic simulations of enetic switch systems Adiel Loiner, 1 Azi Lipshtat, 2 Nathalie Q. Balaban, 1 and Ofer Biham 1 1 Racah Institute of Physics, The Hebrew University, Jerusalem 91904, Israel 2 Department

More information

Chapter 8 Applications of Newton s Second Law

Chapter 8 Applications of Newton s Second Law 81 Force Laws 2 Chapter 8 Applications of Newton s Second Law 811 Hooke s Law 2 822 Principle of Equivalence: 6 823 Gravitational Force near the Surface of the Earth 7 824 Electric Chare and Coulomb s

More information

Metric System. Scientific Measurements

Metric System. Scientific Measurements Metric System Scientific Measurements Metric System Developed by the French in the late 1700 s. Based on powers of ten, so it is very easy to use. Used by almost every country in the world, with the notable

More information

v( t) g 2 v 0 sin θ ( ) ( ) g t ( ) = 0

v( t) g 2 v 0 sin θ ( ) ( ) g t ( ) = 0 PROJECTILE MOTION Velocity We seek to explore the velocity of the projectile, includin its final value as it hits the round, or a taret above the round. The anle made by the velocity vector with the local

More information

8-99 M,Y and O. E:\public_html\8-99 elevated tank problem.mcd 1 / 11 9/4/99 / 8:03 AM elevated tank problem.mcd last save 9/4/99 / 8:03 AM

8-99 M,Y and O. E:\public_html\8-99 elevated tank problem.mcd 1 / 11 9/4/99 / 8:03 AM elevated tank problem.mcd last save 9/4/99 / 8:03 AM 8-99 M,Y and O The pressure at section shown in the Fi. below is not to fall below 50 lb / in when the flowrate in the tank varies from 0 to cfs and the branch line is shut off. Determine the minimum heiht

More information

STOCHASTICALLY GENERATED MULTIGROUP DIFFUSION COEFFICIENTS

STOCHASTICALLY GENERATED MULTIGROUP DIFFUSION COEFFICIENTS STOCHASTICALLY GENERATED MULTIGROUP DIFFUSION COEFFICIENTS A Thesis Presented to The Academic Faculty by Justin M. Pounders In Partial Fulfillment of the Requirements for the Deree Master of Science in

More information

PHYS 100: Lecture 4 PROJECTILE MOTION. y = (v 0 /v T ) x (g/2v T2 )x 2. Velocity of Train v T. Physics 100 Lecture 4, Slide y(m)

PHYS 100: Lecture 4 PROJECTILE MOTION. y = (v 0 /v T ) x (g/2v T2 )x 2. Velocity of Train v T. Physics 100 Lecture 4, Slide y(m) PHYS : Lecture 4 PROJECTILE MOTION.4. Velocity of Train T y(m).8.6.4. 5 5 x(m) y ( / T ) x (/ T )x Physics Lecture 4, Slide Music Who is the Artist? A) Miles Dais B) Wynton Marsalis C) Chris Botti D) Nina

More information

Assignment 6. Name MULTIPLE CHOICE. Choose the one alternative that best completes the statement or answers the question.

Assignment 6. Name MULTIPLE CHOICE. Choose the one alternative that best completes the statement or answers the question. Assinment 6 Name MULTIPLE CHOICE. Choose the one alternative that best completes the statement or answers the question. Round your answer, if appropriate. 1) A man 6 ft tall walks at a rate of 3 ft/sec

More information

ESCI 344 Tropical Meteorology Lesson 12 Tropical Cyclones: Motion and Analysis

ESCI 344 Tropical Meteorology Lesson 12 Tropical Cyclones: Motion and Analysis ESCI 344 Tropical Meteoroloy Lesson 12 Tropical Cyclones: Motion and Analysis References: A Global View of Tropical Cyclones, Elsberry (ed.) The Hurricane, Pielke Forecasters Guide to Tropical Meteoroloy,

More information

An Experimental study of Coupling between Combustor Pressure, Fuel/Air Mixing, and Flame Behavior

An Experimental study of Coupling between Combustor Pressure, Fuel/Air Mixing, and Flame Behavior An Experimental study of Couplin between Combustor Pressure, Fuel/Air Mixin, and Flame Behavior D. M. Kan, F. E. C. Culick Jet Propulsion Center/Department of Mechanical Enineerin California Institute

More information

Ballistics Car P3-3527

Ballistics Car P3-3527 WWW.ARBORSCI.COM Ballistics Car P3-3527 BACKGROUND: The Ballistic Car demonstrates that the horizontal motion of an object is unaffected by forces which act solely in the vertical direction. It consists

More information

MASSACHUSETTS INSTITUTE OF TECHNOLOGY Department of Physics. Physics 8.01x Fall Term 2001 EXAM 1 SOLUTIONS

MASSACHUSETTS INSTITUTE OF TECHNOLOGY Department of Physics. Physics 8.01x Fall Term 2001 EXAM 1 SOLUTIONS MASSACHUSETTS INSTITUTE OF TECHNOLOGY Department of Physics Physics 8.01x Fall Term 2001 EXAM 1 SOLUTIONS Problem 1: We define a vertical coordinate system with positive upwards. The only forces actin

More information

Chapter K. Oscillatory Motion. Blinn College - Physics Terry Honan. Interactive Figure

Chapter K. Oscillatory Motion. Blinn College - Physics Terry Honan. Interactive Figure K. - Simple Harmonic Motion Chapter K Oscillatory Motion Blinn Collee - Physics 2425 - Terry Honan The Mass-Sprin System Interactive Fiure Consider a mass slidin without friction on a horizontal surface.

More information

C. Non-linear Difference and Differential Equations: Linearization and Phase Diagram Technique

C. Non-linear Difference and Differential Equations: Linearization and Phase Diagram Technique C. Non-linear Difference and Differential Equations: Linearization and Phase Diaram Technique So far we have discussed methods of solvin linear difference and differential equations. Let us now discuss

More information

University of Groningen. Functional encapsulation of small particles Laksmana, Fesia Lestari

University of Groningen. Functional encapsulation of small particles Laksmana, Fesia Lestari University of Groninen Functional encapsulation of small particles Laksmana, Fesia Lestari IMPORTANT NOTE: You are advised to consult the publisher's version (publisher's PDF) if you wish to cite from

More information

Midterm Feb. 17, 2009 Physics 110B Secret No.=

Midterm Feb. 17, 2009 Physics 110B Secret No.= Midterm Feb. 17, 29 Physics 11B Secret No.= PROBLEM (1) (4 points) The radient operator = x i ê i transforms like a vector. Use ɛ ijk to prove that if B( r) = A( r), then B( r) =. B i = x i x i = x j =

More information

Achievement Standard (Physics 2.1)

Achievement Standard (Physics 2.1) Achievement Standard 91168 (Physics 2.1) Guidelines What follows is an interpretation of the standard. It has not been approved by the NZQA. Aim Aim The aim of the experiment will be to find the relationship

More information

Follows the revised HSC syllabus prescribed by the Maharashtra State Board of Secondary and Higher Secondary Education, Pune.

Follows the revised HSC syllabus prescribed by the Maharashtra State Board of Secondary and Higher Secondary Education, Pune. Follows the revised HSC syllabus prescribed by the Maharashtra State Board of Secondary and Hiher Secondary Education, Pune. STD. XII Sci. A collection of Board 013 to 017 Questions Physics Chemistry Mathematics

More information

PHYSICS 0625/6 PAPER 6 Alternative to Practical MAY/JUNE SESSION 2000

PHYSICS 0625/6 PAPER 6 Alternative to Practical MAY/JUNE SESSION 2000 Centre Number Candidate Number Candidate Name International General Certificate of Secondary Education UNIVERSITY OF CAMBRIDGE LOCAL EXAMINATIONS SYNDICATE PHYSICS 0625/6 PAPER 6 Alternative to Practical

More information

This relationship is known as the ideal gas law and is mathematically described with the formula below:

This relationship is known as the ideal gas law and is mathematically described with the formula below: Chemistry 20 Ideal as law If we combine all the information contained in Boyle s, Charles and Avoadro s laws, we can derive an expression that describes the temperature, pressure and volume of a as. This

More information

Problems of the 9 th International Physics Olympiads (Budapest, Hungary, 1976)

Problems of the 9 th International Physics Olympiads (Budapest, Hungary, 1976) Problems of the 9 th International Physics Olympiads (Budapest, Hunary, 1976) Theoretical problems Problem 1 A hollow sphere of radius R = 0.5 m rotates about a vertical axis throuh its centre with an

More information

Level 3 Physics, 2018

Level 3 Physics, 2018 91523 915230 3SUPERVISOR S Level 3 Physics, 2018 91523 Demonstrate understanding of wave systems 2.00 p.m. Tuesday 20 November 2018 Credits: Four Achievement Achievement with Merit Achievement with Excellence

More information

Study of the Implications of Whitecap Intermittency on the Uniform Sea-salt Aerosol Source Approximation and Deposition Velocity

Study of the Implications of Whitecap Intermittency on the Uniform Sea-salt Aerosol Source Approximation and Deposition Velocity Naval Research Laboratory Washinton, DC 375-53 NRL/MR/7--7-986 Study of the Implications of Whitecap Intermittency on the Uniform Sea-salt Aerosol Source Approximation and Deposition Velocity William A.

More information

Lab 12: Periodic Motion

Lab 12: Periodic Motion Lab 12: Periodic Motion Objectives: To devise an experiment to test variables that might affect the period of a pendulum To carry out an experiment testing variables that might affect the period of a pendulum,

More information

LATERAL SPREADING OF SLOPES Data report on tests SKH-5-12 S.K. Haigh 1 CUED/D-SOILS/TR317 (2002)

LATERAL SPREADING OF SLOPES Data report on tests SKH-5-12 S.K. Haigh 1 CUED/D-SOILS/TR317 (2002) LATERAL SPREADING OF SLOPES Data report on tests SKH-5-12 S.K. Haih 1 CUED/D-SOILS/TR317 (22) 1 Research Associate, Cambride University Enineerin Department Table of Contents Table of Contents i List

More information

Foundation on Compressible Fluid Flow

Foundation on Compressible Fluid Flow Chapter Foundation on Compressible Fluid Flow. COMRESSIBLE FLUIDS In everyday life one reconizes three states of matter, namely, solid, liquid and aseous. Solids, liquids and ases are all comprised of

More information

Student Exploration: Simple Harmonic Motion

Student Exploration: Simple Harmonic Motion Nae: Date: Student Exploration: Siple Haronic Motion Vocabulary: controlled experient, haronic otion, oscillation, pendulu, period, sprin, sprin constant Prior Knowlede Questions (Do these BEFORE usin

More information

ViscoData & ViscoShift

ViscoData & ViscoShift Introductory Theory Manual ViscoData & ViscoShift (Preliminary Version) Contents ) Preface 2) Introduction 3) Dynamic mechanical properties 4) sin ViscoShift and ViscoData 5) Concludin remarks 6) Refereces

More information

Pendulums. P3 3.6 Lesson guide. Resources available. Specification. Keywords. Points to note. Lesson objectives

Pendulums. P3 3.6 Lesson guide. Resources available. Specification. Keywords. Points to note. Lesson objectives P3 3.6 Lesson guide Pendulums This lesson explains the relationship between the time period and frequency of a pendulum, and looks at the factors that affect the period of a pendulum. Resources available

More information

EXPERIMENTAL PROJECT Rigid Pendulum Experiment

EXPERIMENTAL PROJECT Rigid Pendulum Experiment EXPERIMENTAL PROJECT 2012-2013 Rigid Pendulum Experiment INTRODUCTION The simple pendulum is familiar idea to many students as they will have seen a small mass swinging from side to side at the end of

More information

Lab: Simple Harmonic Motion: Pendulum Mr. Fineman

Lab: Simple Harmonic Motion: Pendulum Mr. Fineman Lab Partners: Lab: Simple Harmonic Motion: Pendulum Mr. Fineman Objective: Students will determine the factors that affect the period of a pendulum, and explain how their experimental results differ to

More information

2.2 Differentiation and Integration of Vector-Valued Functions

2.2 Differentiation and Integration of Vector-Valued Functions .. DIFFERENTIATION AND INTEGRATION OF VECTOR-VALUED FUNCTIONS133. Differentiation and Interation of Vector-Valued Functions Simply put, we differentiate and interate vector functions by differentiatin

More information

What Causes Image Intensity Changes?

What Causes Image Intensity Changes? Ede Detection l Why Detect Edes? u Information reduction l Replace imae by a cartoon in which objects and surface markins are outlined create line drawin description l These are the most informative parts

More information