Experiment P-6 Friction Force

Similar documents
Experiment P-17 Magnetic Field Strength

Experiment: Static and Kinetic Friction

STATIC AND KINETIC FRICTION

COEFFICIENT OF KINETIC FRICTION

LAB 6 - GRAVITATIONAL AND PASSIVE FORCES

If you put the same book on a tilted surface the normal force will be less. The magnitude of the normal force will equal: N = W cos θ

LAB 6: GRAVITATIONAL AND PASSIVE FORCES

Work, Power, Energy Multiple Choice. PSI Physics. Multiple Choice Questions

Coefficient of Friction Using a Force Sensor and a Motion Sensor

Physics 111: Lecture 4: Chapter 4 - Forces and Newton s Laws of Motion. Physics is about forces and how the world around us reacts to these forces.

Serway_ISM_V1 1 Chapter 4

Chapter 4. Forces and Newton s Laws of Motion. continued

Kinetic Friction. Experiment #13

Work and Energy. W =!KE = KE f

Resistance in the Mechanical System. Overview

Experiment 5 ~ Friction

Physics Labs with Computers, Vol. 2 P38: Conservation of Linear Momentum A

Kinetic Friction. Experiment #13

physics 111N work & energy

There are four types of friction, they are 1).Static friction 2) Dynamic friction 3) Sliding friction 4) Rolling friction

Chapter 6. Work and Energy

Acceleration of Gravity Lab Basic Version

C B A T 3 T 2 T What is the magnitude of the force T 1? A) 37.5 N B) 75.0 N C) 113 N D) 157 N E) 192 N

Experiment C-31 Color Absorption

Physics: Principles and Applications, 6e Giancoli Chapter 4 Dynamics: Newton's Laws of Motion

FREE FALL. Introduction. Reference Young and Freedman, University Physics, 12 th Edition: Chapter 2, section 2.5

Physics 11 Assignment KEY Dynamics Chapters 4 & 5

VELOCITY, ACCELERATION, FORCE

FRICTION, WORK, AND THE INCLINED PLANE

Chapter 6 Work and Energy

Conceptual Questions: Forces and Newton s Laws

Worksheet #1 Free Body or Force diagrams

Pendulum Force and Centripetal Acceleration

ENERGYand WORK (PART I and II) 9-MAC

B) 286 m C) 325 m D) 367 m Answer: B

1 One Dimensional Horizontal Motion Position vs. time Velocity vs. time

Dynamics Track. Mechanical Force, Impulse and Momentum

v v ax v a x a v a v = = = Since F = ma, it follows that a = F/m. The mass of the arrow is unchanged, and ( )

Name Partners Date. Energy Diagrams I

Displacement (x) Velocity (v) Acceleration (a) x = f(t) differentiate v = dx Acceleration Velocity (v) Displacement x

Prelab Exercises: Hooke's Law and the Behavior of Springs

CHAPTER 6 WORK AND ENERGY

Pulleys, Work, and Energy

Two-Body System: Two Hanging Masses

Determining the Acceleration Due to Gravity

(I) s(t) = s 0 v 0 (t t 0 ) a (t t 0) 2 (II). t 2 = t v 0. At the time. E kin = 1 2 m v2 = 1 2 m (a (t t 0) v 0 ) 2

Simple Harmonic Motion

SHORT ANSWER. Write the word or phrase that best completes each statement or answers the question.

At the skate park on the ramp

Torque and Rotary Motion

EDUH SPORTS MECHANICS

AP Physics - Chapter 8 Practice Test

Newton s Law of Motion

Physics Midterm Review Packet January 2010

Lecture 6. Weight. Tension. Normal Force. Static Friction. Cutnell+Johnson: , second half of section 4.7

STATICS. Introduction VECTOR MECHANICS FOR ENGINEERS: Eighth Edition CHAPTER. Ferdinand P. Beer E. Russell Johnston, Jr.

Lesson 2 - Force, Friction

AP1 Oscillations. 1. Which of the following statements about a spring-block oscillator in simple harmonic motion about its equilibrium point is false?

HW Set VI page 1 of 9 PHYSICS 1401 (1) homework solutions

WORK DONE BY A CONSTANT FORCE

Work Energy & Power. September 2000 Number Work If a force acts on a body and causes it to move, then the force is doing work.

circular motion & gravitation physics 111N

Unit 3 Work and Energy Suggested Time: 25 Hours

Problem Set 1. Ans: a = 1.74 m/s 2, t = 4.80 s

Sample Questions for the AP Physics 1 Exam

University Physics 226N/231N Old Dominion University. Getting Loopy and Friction

Ch 7 Kinetic Energy and Work. Question: 7 Problems: 3, 7, 11, 17, 23, 27, 35, 37, 41, 43

Exam 2 is at 7 pm tomorrow Conflict is at 5:15 pm in 151 Loomis

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

A Determination of g, the Acceleration Due to Gravity, from Newton's Laws of Motion

Data-logger evaluation software GSoft V2.8

The purposes of this experiment are to test Faraday's Law qualitatively and to test Lenz's Law.

Working Model 2D Exercise Problem ME 114 Vehicle Design Dr. Jose Granda. Performed By Jeffrey H. Cho

Forces. When an object is pushed or pulled, we say that a force is exerted on it.

GRAPH MATCHING EQUIPMENT/MATERIALS

ACCELERATION DUE TO GRAVITY

Weight The weight of an object is defined as the gravitational force acting on the object. Unit: Newton (N)

Physics 1A Lecture 10C

Phys222 Winter 2012 Quiz 4 Chapters Name

5. Forces and Motion-I. Force is an interaction that causes the acceleration of a body. A vector quantity.

Determination of Acceleration due to Gravity

Chapter 5 Using Newton s Laws: Friction, Circular Motion, Drag Forces. Copyright 2009 Pearson Education, Inc.

Uniformly Accelerated Motion

WORKSHEET: KINETIC AND POTENTIAL ENERGY PROBLEMS

Experiment 6: Magnetic Force on a Current Carrying Wire

Conservation of Energy Physics Lab VI

Chapter 8: Potential Energy and Conservation of Energy. Work and kinetic energy are energies of motion.

AP Physics C Fall Final Web Review

Free Fall: Observing and Analyzing the Free Fall Motion of a Bouncing Ping-Pong Ball and Calculating the Free Fall Acceleration (Teacher s Guide)

LAB 4: MOMENTUM AND COLLISIONS

PENDULUM PERIODS. First Last. Partners: student1, student2, and student3

Physics 125 Practice Exam #3 Chapters 6-7 Professor Siegel

8. Potential Energy and Conservation of Energy Potential Energy: When an object has potential to have work done on it, it is said to have potential

Lecture-IV. Contact forces & Newton s laws of motion

Forces. Definition Friction Falling Objects Projectiles Newton s Laws of Motion Momentum Universal Forces Fluid Pressure Hydraulics Buoyancy

W02D2-2 Table Problem Newton s Laws of Motion: Solution

Lesson 39: Kinetic Energy & Potential Energy

Steps to Solving Newtons Laws Problems.

Video Killed the Radio Star! Watch a video of me explaining the difference between static and kinetic friction by clicking here.

Transcription:

1 Experiment P-6 Friction Force Objectives To learn about the relationship between force, normal force and coefficient. To observe changes in the force within different surfaces and different masses. To calculate the coefficients (static and kinetic) in these different conditions. Modules and Sensors PC + NeuLog application USB-200 module NUL-211 Force logger sensor Equipment and Accessories Rough and smooth wooden block with hook 20 cm of thread 1000 g mass 500 g mass The items above are included in the NeuLog Mechanics kit, MEC-KIT.

2 Introduction Friction force is created when two surfaces move or try to move against each other. The direction of the force is always opposite to the direction of motion (or motion attempt) and parallel to the surface, therefore it resists the relative motion of the surfaces. Friction force depends on the roughness of the surfaces, and the "normal force" which presses the surfaces together. It can be described by the following equation: When the object is on a horizontal surface and there are not any other force components acting on it perpendicular to the surface, then the normal force equals the object's weight, thus: The coefficient of is the ratio between the force of and the normal force that presses the surfaces together. Because it is a force divided by a force, does not have any units. Friction force depends on the object's mass (part of the normal force), however the coefficient is not a function of mass; it depends only on the properties of the surfaces. When an object is at rest, the amount of force required to move it is usually greater than the force required to keep it moving. Therefore, typically there is a difference between the coefficient of static (before motion starts) and the kinetic (in motion). The static coefficient is calculated at the threshold of motion while the kinetic coefficient is calculated during motion ( force is constant). In this experiment we will use a force sensor to study the al force of different surfaces and different weights.

3 Procedure Experiment setup 1. Set up the experiment as shown in the picture below. 2. Place a block with one smooth side and one rough side on the table. The rough side should be in contact with the table. 3. Attach the block to the force sensor's hook with a thread. There should be around 10 cm between the block and the force sensor. 4. Place the 1 kg mass (1000 g) on the block. We add weight to the block in order to see the different types of forces.

4 Sensor setup 5. Connect the USB module to the PC. 6. Connect the force sensor to the USB-200 module. Note: The following application functions are explained in short. It is recommended to practice the NeuLog application functions (as described in the user manual) beforehand. 7. Run the NeuLog application and check that the force sensor is identified.

5 Settings 8. Click on the On-line Experiment icon in the NeuLog main icon bar. 9. Click on the Sensor's Module box. 10. Click on the Push=Negative button to get positive values when pulling the hook.

11. Click on the Range button. 12. Select the +/- 10 N button to change the sensor's mode. 6 13. Click on the Experiment setup icon and set the: Experiment duration to 5 seconds Sampling rate to 50 per second

7 Testing and measurements Note: The orientation of the sensor is very important. Before each measurement, hold the sensor in the same position you will use for the specific experiment and zero it. 14. Sensor Zeroing: hold the sensor in its proper position (on the table) and press the button in the sensor s box for about 3 seconds. Alternatively, you can click on the Reset button in the Module Setup box menu. 15. Click on the Run experiment icon to start the measurement. 16. Hold the force sensor on the table and slowly pull the block horizontally while increasing the force (the direction should be in a straight line); when you reach a certain force the block will start to move, keep the block moving at a about the same velocity until the end of the measurement. The part in which you increase the applied force should be done in around one second. Practice this until you see a relatively smooth motion in your graph.

8 17. If needed, click on the Zoom fit icon (or click on the Zoom icon and locate the mouse cursor at a point above the graph and press its left button; keep it pressed and create a rectangle that includes the whole graph). 18. Your graph should be similar to the following: Static Kinetic Transition point Before applying force on the bock 19. Save your graph. 20. The sensor measures the resistance of the block to motion i.e. the force. At the beginning of the graph, the force is zero because the block does not move and there isn't any applied force on it. As we apply force on the block by pulling it, the block resists and do not move, at this part, the force equals the applied force and is considered static. The highest possible static value is called the transition point. We can use this value in order to calculate the static coefficient:

9 After this point the block starts moving as we pull it, the force decreases and then becomes constant. We can use the value at this range to calculate the kinetic coefficient: 21. It is recommended to repeat every measurement three times. 22. In each graph, click on the Select Zone icon and select the part between the transition point static force and the other one to the point where the force becomes constant. 23. In the sample experiment, the force at the transition point is 5.42 N. In order to calculate the static coefficient, we should place this value in the following equation:

10 The force at motion is 4.11 N. In order to calculate the kinetic coefficient, we should place this value in the following equation: In our case the total mass is 1.24 kg, therefore mg = 1.24 kg x 9.8 m/s 2 (g, gravitational acceleration) = 12.15 kg x m/s 2 = 12.15 N. To find the coefficients we divide each force value by mg (total weight). Surface Block's mass [kg] Mass on the block [kg] Total mass [kg] Max. static force [N] Static coefficie nt Kinetic force [N] Kinetic coefficie nt Rough 0.24 1 1.24 5.42 5.42 N / 12.15 N= 0.45 4.11 4.11 N / 12.15 N = 0.34 24. Fill the first row in the following table with your results and calculations. If you repeated the measurement, use the average values. Surface Block's mass [kg] Mass on the block [kg] Total mass [kg] Max. static force [N] Static coefficie nt Kinetic force [N] Kinetic coefficie nt Rough 1 Smooth 1 Rough 1.5 Smooth 1.5

11 25. Proceed in this way with the smooth side on the table (will the force be different? Will the coefficients be different?): 26. Fill the second row of the table with your results and calculations. 27. Proceed in this way with each side of the block, but now put also the 500 g mass on the block. 28. Fill the third and forth rows of the table with your results and calculations.

12 Summary questions 1. Compare the following values you received. If there is a difference between the values, explain it: a. Static vs. kinetic coefficients in each measurement. b. Friction coefficients of the rough surface vs. the smooth surface (with the 1000 g). c. Friction coefficients of the rough surface with the 1000 g mass vs. the same surface with the 1500 g mass. 2. Think about what would happen in a world without. What would happen if you tried to walk? What would happen if you slide an object across the ground?