EDEXCEL NATIONAL CERTIFICATE/DIPLOMA SCIENCE FOR TECHNICIANS OUTCOME 3 - ENERGY TUTORIAL 1 MECHANICAL WORK, ENERGY AND POWER: WORK

Similar documents
DYNAMICS MOMENT OF INERTIA

ENGINEERING COUNCIL DYNAMICS OF MECHANICAL SYSTEMS D225 TUTORIAL 4 MOMENT OF INERTIA. On completion of this tutorial you should be able to

ENGINEERING COUNCIL CERTIFICATE LEVEL MECHANICAL AND STRUCTURAL ENGINEERING C105 TUTORIAL 13 - MOMENT OF INERTIA

Energy Conservation AP

EDEXCEL NATIONAL CERTIFICATE/DIPLOMA SCIENCE FOR TECHNICIANS OUTCOME 1 - STATIC AND DYNAMIC FORCES TUTORIAL 3 STRESS AND STRAIN

EDEXCEL NATIONAL CERTIFICATE/DIPLOMA FURTHER MECHANICAL PRINCIPLES AND APPLICATIONS UNIT 11 - NQF LEVEL 3 OUTCOME 4 - LIFTING MACHINES

MECHANICAL PRINCIPLES OUTCOME 3 CENTRIPETAL ACCELERATION AND CENTRIPETAL FORCE TUTORIAL 1 CENTRIFUGAL FORCE

ENGINEERING COUNCIL DYNAMICS OF MECHANICAL SYSTEMS D225 TUTORIAL 10 NATURAL VIBRATIONS ONE DEGREE OF FREEDOM

Engineering Science OUTCOME 2 - TUTORIAL 3 FREE VIBRATIONS

Work Done by a Constant Force

EDEXCEL NATIONAL CERTIFICATE/DIPLOMA MECHANICAL PRINCIPLES AND APPLICATIONS NQF LEVEL 3 OUTCOME 2

Momentum, Impulse, Work, Energy, Power, and Conservation Laws

Chapter 6 Energy and Oscillations

Review. Kinetic Energy Work Hooke s s Law Potential Energy Conservation of Energy Power 1/91

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

40 N 40 N. Direction of travel

Chapter Work, Energy and Power. Q1. The co-efficient of restitution e for a perfectly elastic collision is [1988] (a) 1 (b) 0 (c) (d) 1 Ans: (a)

Momentum, Impulse, Work, Energy, Power, and Conservation Laws

(35+70) 35 g (m 1+m 2)a=m1g a = 35 a= =3.27 g 105

The content contained in all sections of chapter 6 of the textbook is included on the AP Physics B exam.

Suggested Problems. Chapter 1

2. What would happen to his acceleration if his speed were half? Energy The ability to do work

Solving two-body problems with Newton s Second Law. Example Static and Kinetic Friction. Section 5.1 Friction 10/15/13

PHY218 SPRING 2016 Review for Final Exam: Week 14 Final Review: Chapters 1-11, 13-14

Potential Energy. Serway 7.6, 7.7;

AP PHYSICS 1. Energy 2016 EDITION

Physics. Assignment-1(UNITS AND MEASUREMENT)

a. Change of object s motion is related to both force and how long the force acts.

DO NOT TURN PAGE TO START UNTIL TOLD TO DO SO.

Elastic Potential Energy

OUTCOME 2 KINEMATICS AND DYNAMICS

l Every object in a state of uniform motion tends to remain in that state of motion unless an

PHYSICS GUIDESHEET UNIT 5. - ENERGY SUBUNIT - ENERGY CONVERSIONS POTENTIAL AND KINETIC ENERGY ACTIVITY LESSON DESCRIPTION SCORE/POINTS

Potential and Kinetic Energy

Rotation. PHYS 101 Previous Exam Problems CHAPTER

The University of Melbourne Engineering Mechanics

CHAPTER 6: IN AN ISOLATED SYSTEM, ENERGY IS TRANSFERRED FROM ONE OBJECT TO ANOTHER WHENEVER WORK IS DONE

b) 2/3 MR 2 c) 3/4MR 2 d) 2/5MR 2

Advanced Higher Physics. Rotational motion

Section 1 Work, Power, and Machines

Chapter 6 Work and Energy

PHY218 SPRING 2016 Review for Exam#3: Week 12 Review: Linear Momentum, Collisions, Rotational Motion, and Equilibrium

ENGINEERING COUNCIL DYNAMICS OF MECHANICAL SYSTEMS D225 TUTORIAL 8 BALANCING OF ROTATING BODIES

Announcements. Principle of Work and Energy - Sections Engr222 Spring 2004 Chapter Test Wednesday

In this lecture we will discuss three topics: conservation of energy, friction, and uniform circular motion.

Quantitative Skills in AP Physics 1

Physics Exam 2 October 11, 2007

Wiley Plus. Final Assignment (5) Is Due Today: Before 11 pm!

Your Name: PHYSICS 101 MIDTERM. Please circle your section 1 9 am Galbiati 2 10 am Kwon 3 11 am McDonald 4 12:30 pm McDonald 5 12:30 pm Kwon

Physics Year 11 Term 1 Week 7

5. Plane Kinetics of Rigid Bodies

Centripetal acceleration ac = to2r Kinetic energy of rotation KE, = \lto2. Moment of inertia. / = mr2 Newton's second law for rotational motion t = la

Chapter 2 Physics in Action Sample Problem 1 A weightlifter uses a force of 325 N to lift a set of weights 2.00 m off the ground. How much work did th

Dynamics of Rotation

Physics 2211 ABC Quiz #3 Solutions Spring 2017

EDEXCEL NATIONAL CERTIFICATE/DIPLOMA SCIENCE FOR TECHNICIANS OUTCOME 3 - ENERGY TUTORIAL 2 HEAT

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

General Physics I Work & Energy

Exam 3 Practice Solutions

Lesson 8: Work and Energy

Chapter 10-Work, Energy & Power

Distance travelled time taken and if the particle is a distance s(t) along the x-axis, then its instantaneous speed is:

Physics for Scientist and Engineers third edition Rotational Motion About a Fixed Axis Problems

0J2 - Mechanics Lecture Notes 2

Chapter 5 Work and Energy

WORK & ENERGY. Work W = Fdcosα 1. A force of 25.0 Newtons is applied so as to move a 5.0 kg mass a distance of 20.0 meters. How much work was done?

Preparing for Six Flags Physics Concepts

Physics. Student Materials Advanced Higher. Tutorial Problems Mechanics HIGHER STILL. Spring 2000

Q2. A machine carries a 4.0 kg package from an initial position of d ˆ. = (2.0 m)j at t = 0 to a final position of d ˆ ˆ

Phys 106 Practice Problems Common Quiz 1 Spring 2003

VALLIAMMAI ENGINEERING COLLEGE SRM NAGAR, KATTANKULATHUR DEPARTMENT OF MECHANICAL ENGINEERING

the spring is compressed and x is the compression

Essentially, the amount of work accomplished can be determined two ways:

PHYSICS 220. Lecture 15. Textbook Sections Lecture 15 Purdue University, Physics 220 1

Topic 1: Newtonian Mechanics Energy & Momentum

Section 1: Work, Power, and Machines. Preview Key Ideas Bellringer What Is Work? Math Skills Power Machines and Mechanical Advantage

Broughton High School

WORK, ENERGY & POWER Work scalar W = F S Cosθ Unit of work in SI system Work done by a constant force

Ch 5 Work and Energy

Power: Sources of Energy

2 possibilities. 2.) Work is done and... 1.) Work is done and... *** The function of work is to change energy ***

EDEXCEL ANALYTICAL METHODS FOR ENGINEERS H1 UNIT 2 - NQF LEVEL 4 OUTCOME 3 - CALCULUS TUTORIAL 2 MAXIMA AND MINIMA

Wheel and Axle. Author: Joseph Harrison. Research Ans Aerospace Engineering 1 Expert, Monash University

Do not fill out the information below until instructed to do so! Name: Signature: Student ID: Section Number:

3. Kinetics of Particles

Today. Finish Ch. 6 on Momentum Start Ch. 7 on Energy

Physics 12. Unit 5 Circular Motion and Gravitation Part 1

Work. The quantity of work done is equal to the amount of force the distance moved in the direction in which the force acts.

AP Physics. Harmonic Motion. Multiple Choice. Test E

Lecture PowerPoints. Chapter 11. Physics for Scientists and Engineers, with Modern Physics, 4 th edition Giancoli

A uniform rod of length L and Mass M is attached at one end to a frictionless pivot. If the rod is released from rest from the horizontal position,

Lectures Chapter 10 (Cutnell & Johnson, Physics 7 th edition)

Phys 2210 S18 Practice Exam 3: Ch 8 10

Efficiency = power out x 100% power in

SECTION A. 8 kn/m. C 3 m 3m

Sample Final Exam 02 Physics 106 (Answers on last page)

Healy/DiMurro. Vibrations 2016

PHYS 1303 Final Exam Example Questions

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

Exam II. Spring 2004 Serway & Jewett, Chapters Fill in the bubble for the correct answer on the answer sheet. next to the number.

Transcription:

EDEXCEL NATIONAL CERTIFICATE/DIPLOMA SCIENCE FOR TECHNICIANS OUTCOME 3 - ENERGY TUTORIAL 1 MECHANICAL WORK, ENERGY AND POWER: WORK 3 Energy Mechanical work, energy and power: work - energy relationship, gravitational potential energy, kinetic energy, conservation of energy, work done and energy transfer, work done against friction Heat energy: elementary molecular definition of solids, liquids and gases; gas laws, transfer of heat energy, temperature, temperature scales, change of state, expansion of solids and liquids You should judge your progress by completing the self assessment exercises. These may be sent for marking at a cost (see home page). It is not clear whether the syllabus intends the student to cover angular motion also. It would seem to be a lot of material to cover so it is left to the individual to decide whether or not to study problems involving rotation. In order to do them you need to have studied angular motion and moment of inertia. D.J.Dunn freestudy.co.uk 1

1. WORK When a force F moves a distance x, the work done W is W = F x In order to do work, you must use an equal amount of energy and since energy cannot be destroyed, it must have been transferred somewhere else (Law of conservation of energy). For example if a mass is raised on a pulley, work is done and the energy of the mass increases as it is lifted. The energy used cannot have been destroyed so it must be stored in the mass as an increase in its potential (gravitational) energy. Another example is a truck being accelerated along a floor. A force is needed to accelerate the truck and as it moves more and more work is done. The energy used to accelerate the mass becomes stored in it as kinetic energy. Both the examples show that energy may be transferred to a mass by doing work. It follows that ENERGY IS STORED WORK. ENERGY FORMS POTENTIAL ENERGY This is the energy stored in a body by virtue of its altitude z and is also called gravitational energy. Consider a mass M kg raised a height z metres against the force of gravity. The weight is Mg. The work done = weight x distance moved W = Mgz Since this energy cannot be destroyed it is stored in the mass and may be recovered. The Potential energy is P.E. = mgz Note that z is the S. I. symbol for altitude but h for height and x, for distance is also commonly used. For example if a mass is raised on a simple pulley, work is done and the energy of the mass increases as it is lifted. From the law of conservation of energy, the energy used up cannot have been destroyed so it must be stored in the mass as an increase in its potential (gravitational) energy. D.J.Dunn freestudy.co.uk

WORKED EXAMPLE No. 1 If the mass being lifted is 00 kg and it is raised 0.6 m, determine the work done and the change in P.E. of the mass. The weight is mg so the force to be overcome is F = 00 x 9.81 = 196 N W = 196 x 0.6 = 1177. J The change in P. E. is the same assuming no energy was wasted. KINETIC ENERGY This is the energy stored in a body by virtue of its velocity. Consider a mass, which is at rest. A force is applied to it and it accelerates at a m/s and after t seconds it achieves a velocity of v m/s and has travelled x metres. From the laws of motion we know that F = M a a = v/t x = vt/ The work done is W = F x = M(v/t)(vt/) = Mv/ Since the energy used up cannot be destroyed, it is stored in the mass and may be recovered. The Kinetic Energy is K.E. = Mv/ WORKED EXAMPLE No. A force of 80 N is used to pull a truck 00 m along a horizontal floor. Determine the work done and the increase in K.E. W = F x = 80 x 00 = 16000 J If there was no energy lost due to friction then this must end up as kinetic energy in the truck. D.J.Dunn freestudy.co.uk 3

ANGULAR KINETIC ENERGY A rotating wheel has kinetic energy since all parts of the wheel are moving and have a velocity in a circular path. The corresponding formula is:- K.E. = I ω / ω is the angular velocity of the wheel in radian/sec and I is the moment of inertia. For those not familiar with this concept here is a brief explanation. The mass of any wheel is spread around at various radii and so an affective radius is used called the RADIUS OF GYRATION symbol k. If this is known we can calculate I with :- I = m k For a solid plain disc, k = 0.707R where R is the outer radius. You also need to know that linear and angular velocities are linked by v = ω r where r is the radius at which v is measured. STRAIN ENERGY When an elastic body is deformed and released, it springs back to its original shape and size. In order to deform it, that is, bend it, twist it, squash it or stretch it, work is done. This work is stored in the body as strain energy. Consider a simple spring, which requires F Newton to stretch it 1 m. The stiffness is K N/m. When the spring is stretched in stages the plot of F against x is a straight line as shown. The gradient is K = F/x and this is Hooke's Law. The work done is the mean force x distance moved. The mean force = F/ W = Fx/ This work is stored in the spring as strain energy, which also has a symbol of U. U = Fx/ for a simple spring. Note that F/ is the average force needed to stretch the spring. Since F = K x then U = Kx / for a simple spring. 3. ENERGY CONVERSION Many engineering problems involve the conversion of energy from one form to another. The law of energy conservation tells us that if no energy is lost to friction then the energy before a change is the same as the energy after a change. This may be used to solve problems. In later problems we shall deal with conversions with energy loss but first let's study simple cases with no losses in the conversion process. FALLING BODIES A body, which is z metres above a point, has potential energy of mgz. As it falls, the potential energy is converted in kinetic energy mv /. If the energy conversion is perfect, then we may equate the two mgz = mv / hence v = (gz) D.J.Dunn freestudy.co.uk 4

This formula may also be applied to jet of water issuing from a hole in a tank. The water is forced out by the height of water in the tank. A mass moving from the surface of the tank to the hole will lose potential energy and gain kinetic energy so the velocity is v = (gz) The formula may also be applied to swinging hammers or pendulums. The hammer starts at height z and swings down so that at the bottom of the swing the kinetic energy is equal to the potential energy lost and again (gz). WORKED EXAMPLE No. 3 Consider a cylindrical body attached by a cord to a fixed point. The cord is wrapped around an axle of radius r. If the body falls, the cylinder spins and so it achieves linear and angular velocities. Show that the velocity of the falling mass is given by mgz v = m + I/r P.E. lost = mgz KE gained = mv / + I ω / = mv / + I ω / mgz = mv / + I ω / ω = v/r mgz = mv / + I v /r = v (m/ + I /r mgz ) v = m + I/r A wheel with a moment of inertia of 1. kg m is rotated by a falling mass of 80 g attached to a string wrapped around the axle which is 40 mm diameter. Calculate the linear and angular velocity when if falls 4 m. The inertia of the axle may be ignored. Check the answer by comparing the energy before and after. v mgz = = m + I/r x 0.08 x 9.81x 4 = 0.001 v = 0.045 m/s 0.08 + 1./0.0 ω = v/r = 0.045/0.0 =.59 rad/s (note the velocity of the mass and string is the same as the velocity at radius r). P.E. Lost = mgz = 0.08 x 9.81 x 4 = 3.139 J KE gained = mv / + Iω / = 0.08 x 0.045 / + 1. x.59 / = 3.139 J D.J.Dunn freestudy.co.uk 5

WORKED EXAMPLE No. 4 A ball of mass 0 g is dropped a height of 750 mm onto a platform resting on a spring of stiffness 50 N/m. Calculate the distance the platform will move down before the ball stops moving. Change in P. E. = mg (z + x) Change in Strain Energy is Kx / Kx / = mg (z + x) = mg z + mg x Kx = mg z + mg x Kx - mg x - mg z = 0 Use the quadratic equation a = K = 5 b = -mg = -0.394 c = -mgz = 0.943 b ± b 4ac x = a Answer x = 81 mm 0.394 ± = - 0.394 4 x 50 x 0.943 = 0.081m or 0.073m x 50 SELF ASSESSMENT EXERCISE No. 1 1. An object of mass 0 kg is dropped onto a surface from a height of 50 m. Calculate the energy and velocity just before it hits the surface. (9810 J and 31.3 m/s). A swinging hammer must have 50 Joules of energy and a velocity of m/s at the bottom of the swing. Calculate the mass and height of the hammer before it is released. (5 kg and 0.04 m) 3. A swinging hammer has a mass of kg and is raised 0. m. Calculate the energy and velocity at the bottom of the swing. (1.98 m/s) 4. A platform rests on springs with a stiffness of 00 kn/m. A mass of 4 kg is dropped on it from a height of 0 mm. Assuming that the deflection is small, what is the maximum distance the platform moves? (3 mm) 5. A drum is made to revolve about its centre by a falling mass as shown. Calculate the velocity of the falling mass and rotating drum when the mass descends 10 m with no frictional losses. (13 m/s and 65.3 rad/s) D.J.Dunn freestudy.co.uk 6

4. MECHANICAL POWER Power is the rate of using energy or doing work. Energy has units of Joules so power is Joules per second or Watts. P = Energy used/time taken Mechanical power is the power developed by a force as opposed to say the rate of using heat which is also a form of power. Power = Work Done per Second = F x/t Since x/t is the velocity v of the force then we have a definition for mechanical power. P = F v 5. FRICTION Friction always causes energy to be wasted in the form of heat. It is ever present in mechanical mechanisms. When solving problems involving energy conversion, the conversion is less than 100%, the difference being the energy wasted. EFFICIENCY Efficiency (symbol η eta) is the ratio of the energy conversion process so Energy Out η% = x 100 and the energy wasted is Energy Out Energy In Energy In In devices like friction brakes, all the energy is converted into heat by friction so the efficiency does not mean anything. WORKED EXAMPLE No. 4 A pulley is used to raise a mass of 85 kg a distance of 1 m. The efficiency is 60%. Calculate the work done. The change in P. E. = mg z = 85 x 9.81 x 1 = 10 kj The Work Done is the energy in so W = 10/60% = 10/0.6 = 16.67 kj SELF ASSESSMENT EXERCISE No. 1. 5 000 J of energy is used up in 0 seconds. What is the power? (50 W). A vehicle is propelled 5 000 m by a force of 000 N in 1 seconds. Calculate the work done and the power used. (4.17 MW) 3. A block of mass 500 kg is raised at a constant rate by a hoist at a rate of 0.15 m/s. Calculate the force in the rope and hence the power used. (4905 N and 735.8 W) 4. A load is raised by a pulley. The force in the rope is 40 N and it moves 3 m in 11 seconds. The process is 70% efficient. Calculate the mechanical power. (15.6 W) 5. A rocket flies at 10 m/s under a propulsion force of 3 000 N. Calculate the power used. (360 kw) 6. A lifting jack must raise a force of 4 kn a distance of 0.3 m. Due to friction the efficiency is only 35%. Calculate the energy used to raise the load. (349 Joules) 7. An electric hoist raises a mass of 60 kg at a rate of 0. m/s. The process is 30% efficient. Calculate the power input to the hoist. (39 W) D.J.Dunn freestudy.co.uk 7