Systems of Masses. 1. Ignoring friction, calculate the acceleration of the system below and the tension in the rope. and (4.0)(9.80) 39.

Similar documents
PHYSICS - CLUTCH CH 05: FRICTION, INCLINES, SYSTEMS.

For a situation involving gravity near earth s surface, a = g = jg. Show. that for that case v 2 = v 0 2 g(y y 0 ).

Physics 140 D100 Midterm Exam 2 Solutions 2017 Nov 10

Chapter 5, Conceptual Questions

Question 1. [14 Marks]

Physics 20 Lesson 18 Pulleys and Systems

NAME NUMBER SEC. PHYCS 101 SUMMER 2001/2002 FINAL EXAME:24/8/2002. PART(I) 25% PART(II) 15% PART(III)/Lab 8% ( ) 2 Q2 Q3 Total 40%

Lesson 24: Newton's Second Law (Motion)

Chapter 4 FORCES AND NEWTON S LAWS OF MOTION PREVIEW QUICK REFERENCE. Important Terms

NB1140: Physics 1A - Classical mechanics and Thermodynamics Problem set 2 - Forces and energy Week 2: November 2016

XI PHYSICS M. AFFAN KHAN LECTURER PHYSICS, AKHSS, K.

2. Which of the following best describes the relationship between force and potential energy?

1. The property of matter that causes an object to resist changes in its state of motion is called:

Name Period. What force did your partner s exert on yours? Write your answer in the blank below:

TUTORIAL 1 SIMPLE HARMONIC MOTION. Instructor: Kazumi Tolich

F = 0. x o F = -k x o v = 0 F = 0. F = k x o v = 0 F = 0. x = 0 F = 0. F = -k x 1. PHYSICS 151 Notes for Online Lecture 2.4.

Flipping Physics Lecture Notes: Free Response Question #1 - AP Physics Exam Solutions

Review: Advanced Applications of Newton's Laws

15 Newton s Laws #2: Kinds of Forces, Creating Free Body Diagrams

Chapter 3 Dynamics: Motion and Force 3.1 Newton's 2nd Law-1D Acceleration-Horizontal Motion Homework # 19

Inclined Planes Worksheet Answers

= 1.49 m/s m. 2 kg. 2 kg

A 30 o 30 o M. Homework #4. Ph 231 Introductory Physics, Sp-03 Page 1 of 4

Figure 5.1a, b IDENTIFY: Apply to the car. EXECUTE: gives.. EVALUATE: The force required is less than the weight of the car by the factor.

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

You may use g = 10 m/s 2, sin 60 = 0.87, and cos 60 = 0.50.

FREE BODY DIAGRAMS! For each of the layouts, draw the f.b.d.s for the bodies in the system. (The solutions follow--try each before looking!)! 3.)!

Unit 5 Forces I- Newtonʼ s First & Second Law

(a) On the dots below that represent the students, draw and label free-body diagrams showing the forces on Student A and on Student B.

Application of Newton s Laws. F fr

Webreview practice test. Forces (again)

Fraser Heights Secondary Physics 11 Mr. Wu Practice Test (Dynamics)

Honors Lab 4.5 Freefall, Apparent Weight, and Friction

Student AP Physics 1 Date. Newton s Laws B FR

What is a Force? Free-Body diagrams. Contact vs. At-a-Distance 11/28/2016. Forces and Newton s Laws of Motion

Chapter 4. Dynamics: Newton s Laws of Motion

Phys101 Second Major-162 Zero Version Coordinator: Dr. Kunwar S. Saturday, March 25, 2017 Page: 1

The Laws of Motion. Newton s first law Force Mass Newton s second law Gravitational Force Newton s third law Examples

Physics 120 Final Examination

Particle Kinetics Homework

Problem Set 14: Oscillations AP Physics C Supplementary Problems

m A 1 m mgd k m v ( C) AP Physics Multiple Choice Practice Oscillations

Isaac Newton ( ) 1687 Published Principia Invented Calculus 3 Laws of Motion Universal Law of Gravity

Page 1. Physics 131: Lecture 16. Today s Agenda. Collisions. Elastic Collision

8.01x Classical Mechanics, Fall 2016 Massachusetts Institute of Technology. Problem Set 2

9. h = R. 10. h = 3 R

3. In the figure below, the coefficient of friction between the center mass and the surface is

Q16.: A 5.0 kg block is lowered with a downward acceleration of 2.8 m/s 2 by means of a rope. The force of the block on the rope is:(35 N, down)

Physics Dynamics: Forces. Science and Mathematics Education Research Group

2. If a net horizontal force of 175 N is applied to a bike whose mass is 43 kg what acceleration is produced?

PhysicsAndMathsTutor.com

5.1 m is therefore the maximum height of the ball above the window. This is 25.1 m above the ground. (b)

Physics 2211 ABC Quiz #3 Solutions Spring 2017

Particle dynamics Physics 1A, UNSW

F on stone by rope F on box by rope. F on stone by Earth

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

PHYSICS 220 Lecture 04 Forces and Motion in 1 D Textbook Sections

Frictional Force ( ): The force that occurs when two object rub against one another and always OPPOSES motion. It's not dependent on area of contact.

FOUNDATION STUDIES EXAMINATIONS January 2016

Example 1: Example 1: Example 2: a.) the elevator is at rest. Example 2: Example 2: c.) the elevator accelerates downward at 1.

HATZIC SECONDARY SCHOOL

m potential kinetic forms of energy.

Reading Quiz. Chapter 5. Physics 111, Concordia College

= 40 N. Q = 60 O m s,k

SPH3U1 - Dynamics Problems Set 3

Experiment 2: Hooke s Law

A force is a push or a pull.

Examples Newton's Laws and Friction

Unit 2: Vector Dynamics

SRI LANKAN PHYSICS OLYMPIAD MULTIPLE CHOICE TEST 30 QUESTIONS ONE HOUR AND 15 MINUTES

Forces and Newton s Laws Reading Notes. Give an example of a force you have experienced continuously all your life.

A. B. C. D. E. v x. ΣF x

Chapter 4. Dynamics: Newton s Laws of Motion. That is, describing why objects move

WS-CH-4 Motion and Force Show all your work and equations used. Isaac Newton ( )

Topic: Force PHYSICS 231

CHAPTER 4 NEWTON S LAWS OF MOTION

Physics 11 HW #6 Solutions

Physics 101 Lecture 5 Newton`s Laws

variable Formula S or v SI variable Formula S or v SI 4. How is a Newton defined? What does a Newton equal in pounds?

For more Study Material and Latest Questions related to IIT-JEE visit

d. Determine the power output of the boy required to sustain this velocity.

PHYS 101 Previous Exam Problems. Force & Motion I

Chapter 5 Applying Newton s Laws

Sara Rwentambo. PHYS 1007 AB

Tutorial Exercises: Incorporating constraints

MULTIPLE CHOICE. Choose the one alternative that best completes the statement or answers the question. Diagram 1 A) B - A. B) A - B. C) A + B. D) A B.

Created by T. Madas WORK & ENERGY. Created by T. Madas

AP Physics C: Mechanics Practice (Newton s Laws including friction, resistive forces, and centripetal force).

Every object remains in a state of rest or move with constant velocity in a straight line unless forces acts on it to change that state

SPH4U/SPH3UW Unit 2.3 Applying Newton s Law of Motion Page 1 of 7. Notes

2009 Academic Challenge

Random sample problems

Physics B Newton s Laws AP Review Packet

The Concept of Force Newton s First Law and Inertial Frames Mass Newton s Second Law The Gravitational Force and Weight Newton s Third Law Analysis

Student Book pages

PHYSICS 231 Laws of motion PHY 231

Chapter 3 The Laws of motion. The Laws of motion

Question 01. A. Incorrect! This is not Newton s second law.

Bell Ringer: What is Newton s 3 rd Law? Which force acts downward? Which force acts upward when two bodies are in contact?

Unit 5 Forces I- Newton s First & Second Law

Transcription:

Systes of Masses. Ignoring friction, calculate the acceleration of the syste below and the tension in the rope. Drawing individual free body diagras we get 4.0kg 7.0kg g 9.80 / s a?? g and g (4.0)(9.80) 39.N g g (7.0)(9.80) 68.6N or the 4.0 kg ass, the only force parallel to the acceleration (which is horizontal) is the tension force in the rope; the forces and g are perpendicular to the acceleration and should not be included. or the 7.0 kg ass, both of the forces and g are parallel to the acceleration (which is vertical). N When looking at the forces causing the syste to accelerate, tension is not included since this is an internal force. he only reaining force is therefore g. his would be the only horizontal force (or the only force parallel to the otion) in our linearized free body diagra for the whole syste: RRHS Physics

Using clockwise (or toward the 7.0 kg ass) as positive, a a t a t g g.0a 68.6 a 6. / s o find the tension it is necessary to set up an equation for one of the asses individually. If we do this for the 4.0 kg ass, we get a a (4.0)(6.) 5N. A.00 kg ass and a 3.00 kg ass are attached to a lightweight cord that passes over a pulley. he hanging asses are free to ove. (a) What is its acceleration? RRHS Physics

.00kg 3.00kg g 9.80 / s a? g g (.00)(9.80) 9.6N g g (3.00)(9.80) 9.4N reating the syste as one object and using the 3.00 kg ass as the positive end (clockwise) a a t g g a t g g 5.00a 9.4 9.6 a.96 / s (b) What is the tension force acting in the cord? o find the tension it is necessary to look at just one of the objects. Looking at the 3.00 kg object, a g g 3.00(.96) 9.4 a a 3.5N 3. Do Question # question again if the coefficient of friction between the top box and the table is 0.3. RRHS Physics 3

4.0kg 7.0kg 0.3 a?? g g (4.0)(9.80) 39.N We also need the force of friction on : f N g (0.3)(39.).N g g (7.0)(9.80) 68.6N Using the 7.0 kg ass end of the rope as positive, a a t g f a t g f.0a 68.6. a 5. / s o find the tension, we need to look at just one object. Looking at the 4.0 kg object, a f f 4.0(5.). a a 33N 4. What coefficient of static friction is necessary to prevent otion in the diagra below? 4 RRHS Physics

3.0kg g g g g 5.0kg (3.0)(9.80) (5.0)(9.80) s? 9.4N 49N a 0 Since there is no otion, the acceleration ust be zero. a t g f 0 g f g f g s N g s g 49 (9.4) s.7 s a 5. What coefficient of kinetic friction is needed in the last question for a constant speed? 3.0kg 5.0kg? k a 0 Since the acceleration is again zero, the sae forces have to balance as in the previous question, so the ath is the exact sae as the previous question. he only RRHS Physics 5

difference is that this tie we are finding the coefficient of kinetic friction since the syste is in otion. k.7 6. ind the acceleration of the following syste (a) if there is no friction..0kg g g g g g g 5.0kg (.0)(9.80) (5.0)(9.80) (6.0)(9.80) 3 6.0kg 9.6N 49N 58.8N a? Since all of the tension forces are internal forces, the only forces that contribute to the otion are g and g. We will use the 6.0 kg end of the rope as the positive direction: a a t g g a t g g 3.0a 9.6 58.8 a 3.0 / s (b) if the coefficient of friction between the box and the table is 0.. 6 RRHS Physics

.0kg 3 5.0kg 6.0kg 0. a? g g (.0)(9.80) 9.6N g g (5.0)(9.80) 49N g g (6.0)(9.80) 58.8N f N g (0.)(49) 5.9N Since all of the tension forces are internal forces, the only forces that contribute to the otion are g, f and g. We will use the 6.0 kg end of the rope as the positive direction: a a t g f g3 a t g f g3 3.0a 9.6 5.9 58.8 a.6 / s 7. A.5 kg counterweight is connected (over a pulley) to a 4.5 kg window that slides vertically in its frae. How uch force ust you exert to start the window opening with an upward acceleration of 0.8 /s? RRHS Physics 7

4.5kg.5kg g 9.80 / s a 0.8 / s p? g g (4.5)(9.80) 44.N g g (.5)(9.80) 4.5N Looking at the syste as one object (so we will ignore the internal tension forces) and using the counterweight end of the rope as the positive end, a t g g p t g g p 7.0(0.8) 44. 4.5 p a a N p 8. A. kg ass and a 3. kg ass are attached by a assless rope hanging over a pulley. he two asses are initially.60 above the ground and the pulley is 4.0 above the ground. What axiu height does the. kg object reach after the syste is released fro rest? 8 RRHS Physics

he 3. kg ass will fall.6 to the floor; during this tie, the. kg ass will be accelerating upward. We ust find this acceleration so that we can deterine the speed of the. kg ass when it stops accelerating upward (at a height of 3. fro the floor)..kg 3.kg g 9.80 / s a? g g (.)(9.80).8N g g (3.)(9.80) 3.4N reating the syste as one object and using the 3. kg ass as the positive end (clockwise) a a t g g a t g g 4.4a 3.4.8 a 4.45 / s We can now find the upward velocity of the. kg ass when it is at a height of 3.: v 0 v i f? a 4.45 / s d.6 vf vi d a v f 0.6 (4.45) v f 3.77 / s We can now calculate how uch higher it goes before gravity brings it to a stop: RRHS Physics 9

v 3.77 / s v i f 0 a 9.80 / s d? So the. kg ass will be d vf vi a 0 3.77 ( 9.80) 0.73.6.6 0.7 3.9 above the floor (and still below the 4.0 high pulley) 0 RRHS Physics