Work, Energy, Power Chapter 7 in a nutshell Work is Force times Distance. The change in Kinetic Energy is equal to the work. Power is Work per unit time.

Slides:



Advertisements
Similar presentations
Chapter 8 Work & Kinetic Energy
Advertisements

Potential Energy, Conservation of Energy
ConcepTest 6.5a Kinetic Energy I
Conservation of Energy
Reading Quiz A cannonball is dropped from a tower. As it falls,
Work, Energy, And Power m Honors Physics Lecture Notes.
Work, Energy, and Power Samar Hathout KDTH 101. Work is the transfer of energy through motion. In order for work to take place, a force must be exerted.
Work, Energy and Power. Work = Force component x displacement Work = F x x When the displacement is perpendicular to the force, no work is done. When.
Work and Energy Chapter 7.
Physics 151: Lecture 15, Pg 1 Today’s Topics l Potential Energy, Ch. 8-1 l Conservative Forces, Ch. 8-2 l Conservation of mechanical energy Ch.8-4.
Physics 218, Lecture XI1 Physics 218 Lecture 11 Dr. David Toback.
Physics 218 Lecture 11 Dr. David Toback Physics 218, Lecture XI.
Conservation of Energy
Work Lecturer: Professor Stephen T. Thornton
1a. Positive and negative work
Chapter 7 Work and Kinetic Energy 7-1 Work done by a Constant Force A. Force along Displacement W = Fd Units: Nm = Joule P7.5 (p.200)
Dr. Jie Zou PHY 1151G Department of Physics1 Chapter 7 Work and Kinetic Energy.
T101Q7. A spring is compressed a distance of h = 9.80 cm from its relaxed position and a 2.00 kg block is put on top of it (Figure 3). What is the maximum.
Chapter 5 Work and Energy
Work, Power, & Efficiency
Chapter 6 Work & Energy.
Physics 6A Work and Energy examples Prepared by Vince Zaccone For Campus Learning Assistance Services at UCSB.
WORK In order for work to be done, three things are necessary:
by the normal force acting on a sliding block?
Work and Kinetic Energy Teacher: Luiz Izola
Copyright © 2010 Pearson Education, Inc. Chapter 7 Work and Kinetic Energy.
Potential Energy and Conservative Forces
Energy m m Physics 2053 Lecture Notes Energy.
Work and Energy. Work a force that causes a displacement of an object does work on the object W = Fdnewtons times meters (N·m) or joules (J)
Sect. 7-4: Kinetic Energy; Work-Energy Principle.
Work and Energy. Work, Power, & Energy Energy offers an alternative analysis of motion and its causes. Energy is transformed from 1 type to another in.
Mechanics 105 Work done by a constant force Scalar product Work done by a varying force Kinetic energy, Work-kinetic energy theorem Nonisolated systems.
Work and Energy Chapter 7 Conservation of Energy Energy is a quantity that can be converted from one form to another but cannot be created or destroyed.
Chapter 6 Work and Energy. Units of Chapter 6 Work Done by a Constant Force Work Done by a Varying Force Kinetic Energy, and the Work-Energy Principle.
Physics 1D03 - Lecture 22 Potential Energy Work and potential energy Conservative and non-conservative forces Gravitational and elastic potential energy.
Chapter 6 Work and Energy. Units of Chapter 6 Work Done by a Constant Force Kinetic Energy, and the Work-Energy Principle Potential Energy Conservative.
Work and Energy.
Work and Energy Work The work done by a constant force is defined as the product of the component of the force in the direction of the displacement and.
Work and Energy. Work Done by a Constant Force The work done by a constant force is defined as the distance moved multiplied by the component of the force.
Energy. Analyzing the motion of an object can often get to be very complicated and tedious – requiring detailed knowledge of the path, frictional forces,
Physics. Session Work, Power and Energy - 3 Session Objectives.
Work and Energy Work is the product of Force and displacement. The force needed to calculate Work is the force or component force in the direction of.
Work and Energy.
Lecture 11: Potential Energy & Energy Conservation.
Motion, Forces and Energy Lecture 7: Potential Energy & Conservation The name potential energy implies that the object in question has the capability of.
Energy and Work. Energy Energy is the ability to change or cause change. If something has no energy, there can be no change.
Lecture 10: Work & Energy.
Work –Moving an object with a force that is in the direction of the movement.  W = F ∙ d If F and displacement moved are in same direction, W is (+) If.
Physics 1D03 - Lecture 22 Potential Energy Serway and Jewett 8.1 – 8.3 Work and potential energy Conservative and non-conservative forces Gravitational.
1. Work [W] = N*m = J Units: Work done by forces that oppose the direction of motion will be negative. Work and energy A. PositiveB. NegativeC. Zero Example:
Work, Power, Energy and Motion Work, Power, Energy and Motion moving train cars moving electrons nuclear forces chemical forces gravitational force Electrical.
Work, Energy and Power Ms Houts AP Physics C Chapters 7 & 8.
A body experiences a change in energy when one or more forces do work on it. A body must move under the influence of a force or forces to say work was.
 Work  Energy  Kinetic Energy  Potential Energy  Mechanical Energy  Conservation of Mechanical Energy.
Physics 101: Lecture 9, Pg 1 Physics 101: Lecture 9 Work and Kinetic Energy  Hour Exam 1, Tomorrow! – Exam 2.
PHY 101: Lecture Work Done by a Constant Force
Chapter 7.1 and 7.7 Work and Power What is energy? Energy is defined as the ability to do work.Energy is defined as the ability to do work. But in some.
Copyright © 2010 Pearson Education, Inc. Lecture Outline Chapter 7 Physics, 4 th Edition James S. Walker.
Work, Power, and Energy. WORK  In Physics, work has a very specific definition.  This is not work in Physics.
IB Physics 11 Mr. Jean November 3 rd, The plan: Video clips of the day Work Potential energy –Gravitational potential kinetic energy.
Chapter 6 Work and Energy.
Energy.
Let’s Play! Please listen carefully and think before answering.
Work.
Work.
Work, Energy, Power Chapter 6 in a nutshell
This lesson Work done as energy transfer
Work, Energy, Power.
Forces.
Physics: Work and Energy
Presentation transcript:

Work, Energy, Power Chapter 7 in a nutshell Work is Force times Distance. The change in Kinetic Energy is equal to the work. Power is Work per unit time.

New Concept: Kinetic Energy K = ½ m V 2 Work causes a change in kinetic energy, so the units are the same. Units of Kinetic energy: Joule But, from the definition of kinetic energy, the units are also, 1 Joule = 1 Kg-m 2 /s 2

Table 7-1 Typical Values of Work Annual U.S. energy use8 x Mt. St. Helens eruption10 18 Burning one gallon of gas10 8 Human food intake/day Melting an ice cube Lighting a 100-W bulb for 1 minute6000 Heartbeat0.5 Turning page of a book10 –3 Hop of a flea10 –7 Breaking a bond in DNA10 –20 ActivityEquivalent work (J)

Work is force times distance…but! Only the force component in the direction of motion counts! Units of work: Joule

Force in direction of motion is what matters… D F F x = F cos  W = D * F cos 

Figure 7-3 Force at an Angle to Direction of Motion: Another Look

I’ve got work to do…. F = Mg yy W=F*  y=MgH This is the work done by the person lifting the box.

How about the reverse?…. F = Mg H W=F*  y = - MgH Work can be positive or negative. Lifting a box is positive work. Lowering the box is negative work.

Positive or Negative? Work done by gravity. F g = - Mg  y = - H Work “done by force of gravity” is positive when an object is dropped.

Problem 7-77 W = 50J, given v, F, x. What is theta? What is M?

Figure 7-4 Positive, Negative, and Zero Work

Raindrops are falling on my head…. V1V1 F = - Mg V2V2  y = -H

Special case: Object dropped from rest. -Mg Mass M dropped from height H. What is speed just before hitting the ground? (Neglect friction of air) H W=MgH W=  K=1/2 M v 2

Thought provoking: The inclined plane. Distance = h Force = mg W = mgh Distance = L = h/sin  Force = mg sin  W = mgh The work is the same in both cases. This is an example of conservation of energy, which we will see much more of in the future.

How about the speed? H If Block fell straight down through height H, its speed would be:  Use F=Ma to find speed down the ramp. F=Mg sin  V=at L=1/2 a t 2 so But a = g sin  And L = H/sin  So… Same magnitude of speed, but DIFFERENT DIRECTION!

Figure 7-6 Graphical Representation of the Work Done by a Constant Force

Figure 7-7 Work Done by a Non-Constant Force

Figure 7-8a Work Done by a Continuously Varying Force

Figure 7-8b Work Done by a Continuously Varying Force

Figure 7-8c Work Done by a Continuously Varying Force

When force is not constant. The area under a force-distance curve is the work, W. Distance Force The average force times the distance gives the work. This is the same as the area under the curve.

Back to our Spring Flings. F = -K  x How much work is done to move the block? Be careful with the signs of the forces! The force to move the block must be equal and opposite to the force of the spring on the block. F = K  x Force DistanceX F=Kx W = ½ F X W = ½ K X 2 Work done to move a mass on a spring a distance “x”:

Conceptual Checkpoints What is work, in physics terms? What is kinetic energy? What is power? Work is force in the direction of motion. Kinetic energy is ½ Mv 2 Power is Work (or Energy) per Unit time.

Work and the Weightlifter A weightlifter performs three steps. What is the work done for each of the steps? Assume the weight is 100 Kg, the height of the lift is 1 M, and the acceleration of gravity is 10 M/s^2. Work done against gravity to lift an object a height H is W = MgH W1: The weight is lifted up to the height of 1 M. W2: The weight is held at 1M for 5 seconds. W3: The weight is lowered down to the ground. Cheryl Hawarth, USA gold medal.

Weightlifting Work J, 5000J, 1000J J, 0J, -1000J J, 5000J, -1000J W1: The weight is lifted up to the height of 1 M. W2: The weight is held at 1M for 5 seconds. W3: The weight is lowered down to the ground. The work done W1, W2, W3 is:

The energy is kinetic, relatively speaking…. V = + 5 m/s V = -5 m/s Train moves to the right with speed V. A baseball is thrown to the left with the same speed. What is the kinetic energy of the baseball? Its mass is 1 kg.

What is the kinetic energy? J 2. 5 J 3. Zero 4. Either zero or 12.5J, depends on your frame of reference. V = + 5 m/s V = -5 m/s K = ½ M V 2 M = 1 kg

The Power to overcome Friction. Work is Force times distance. Power is Work per unit time. F Frictional Force, F f =  N Block moves with STEADY SPEED under influence of applied force that EXACTLY balances friction, so V is CONSTANT. AN IMPORTANT SPECIAL CASE Force of friction Under these conditions, THIS IS A SPECIAL CASE IN WHICH AN APPLIED FORCE RESULTS IN CONSTANT SPEED. IT OCCURS BECAUSE THE NET FORCE IS ZERO (SUM OF ALL APPLIED FORCES).

How about this case? Total work is just the sum of the work for each spring.

And this one? This is harder. The two springs DO NOT stretch the same distance (they have different K values). But F 1 = F 2 (why?), so let it be called F. So, can create an effective spring constant, K eff, Then, we can apply the usual formula: