Unit 3 Energy, Work, and Power Energy is the ability to do work Work occurs when an object moves in the direction of an applied force (or component)

Slides:



Advertisements
Similar presentations
Work and Energy.
Advertisements

-PotentialEnergy -Conservation of Mechanical Energy in an isolated system, without friction. AP Physics C Mrs. Coyle.
Conservation of Energy
1a. Positive and negative work
Mechanical Work: More Practice. Gravitational Potential Energy: More Practice.
Physics 3050 Energy Lecture Slide 1 Energy. Physics 3050 Energy Lecture Slide 2 Work Work = (Force in direction of motion)*distance W, Joule (J) = N-m.
Work and Energy Definition of Work Kinetic Energy Potential Energy
Example: A 20 kg block is fired horizontally across a frictionless surface. The block strikes a platform that is attached to a spring at its equilibrium.
Work, energy and power You should be able to: state the definition of work done by a constant force; understand the work done by a varying force; state.
WORK In order for work to be done, three things are necessary:
Chapter 6 Energy and Oscillations
WORK AND ENERGY 1. Work Work as you know it means to do something that takes physical or mental effort But in physics is has a very different meaning.
Chapter 8: Potential Energy and Conservation of Energy
Ch 6 Work and Energy.
Mechanical Energy Ch. 4. Energy Is the ability to do work. Energy = work Units = Joules (J) James Prescott Joule.
Welastic = 1/2 kx02 - 1/2 kxf2 or Initial elastic potential energy minus Final elastic potential energy.
Chapter 5 Work and Energy. 6-1 Work Done by a Constant Force The work done by a constant force is defined as the distance moved multiplied by the component.
Mechanics Work and Energy Chapter 6 Work  What is “work”?  Work is done when a force moves an object some distance  The force (or a component of the.
Energy m m Physics 2053 Lecture Notes Energy.
Physics 3.3. Work WWWWork is defined as Force in the direction of motion x the distance moved. WWWWork is also defined as the change in total.
Energy and Power.
Chapter 7 Energy of a System. Introduction to Energy A variety of problems can be solved with Newton’s Laws and associated principles. Some problems that.
Work IN, Work OUT The Work/Energy Principle. Kinetic Energy KE depends on mass and velocity Work done on an object will change KE.
Mechanical Energy. Kinetic Energy, E k Kinetic energy is the energy of an object in motion. E k = ½ mv 2 Where E k is the kinetic energy measured in J.
Work Done by a Varying Force (1D). Force Due to a Spring – Hooke’s Law.
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)
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.
Conservative Forces: The forces is conservative if the work done by it on a particle that moves between two points depends only on these points and not.
Chapter 6 Notes. Chapter Work  Work is equal to the product of the magnitude of the displacement times the component of the force parallel to the.
Conservative and non-conservative forces Potential energy Total mechanical energy Energy conservation Lecture 11: Potential energy.
Conservation of Energy
Energy. WORK ENERGY THEOREM For an object that is accelerated by a constant force & moves in the same direction… Lets derive this…
Energy The ability to do work. Kinetic Energy (KE) The energy that an object has due to its motion. KE = ½ m v 2 –KE  m and KE  v 2 –Kinetic energy.
Motion, Forces and Energy Lecture 7: Potential Energy & Conservation The name potential energy implies that the object in question has the capability of.
Chapter 7 Conservation of Energy (cont’d) Mechanical energy conservation Examples Work by non-conservative forces March 4, 2010.
Work and Energy x Work and Energy 06.
Chapter 8: Conservation of Energy. In Ch. 7, we learned The Work-Energy Principle: W net = (½)m(v 2 ) 2 - (½)m(v 1 ) 2   K W net ≡ The TOTAL work done.
Ideas about Work and Energy What exactly is energy?
Physics 1D03 - Lecture 22 Potential Energy Serway and Jewett 8.1 – 8.3 Work and potential energy Conservative and non-conservative forces Gravitational.
WORK A force that causes a displacement of an object does work on the object. W = F d Work is done –if the object the work is done on moves due to the.
Work = Force x Displacement …when F and D are in the same direction (The block would be accelerating !)
Potential and Kinetic Energy…
Work and Energy Physics 1. The Purpose of a Force  The application of a force on an object is done with the goal of changing the motion of the object.
Work&EnergyWork&Energy. 4.1 Work Done by a Constant Force.
Work Readings: Chapter 11.
Conservation of Energy
Chapter 5 Work and Energy. Mechanical Energy  Mechanical Energy is the energy that an object has due to its motion or its position.  Two kinds of mechanical.
1 PPMF102 – Lecture 2 Work & Energy. 2 Work = force x displacement x cos  Work = force x displacement x cos  W = Fs cos  W = Fs cos  Scalar quantity.
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 in the direction.
Energy Notes Energy is one of the most important concepts in science. An object has energy if it can produce a change in itself or in its surroundings.
Energy and its Conservation Physics Mrs. Coyle. Part I Mechanical Energy – Potential – Kinetic Work Energy Theorem.
Potential Energy Stored energy due to the relative position of an object In the field of a field force (i.e., gravity, electrostatic, magnetic) In relation.
Work-Energy Relationship Already understand that lifting an object will increase the object’s gravitational potential energy. W=ΔPE= mgΔh No friction.
Conservation of Energy Or the More things change the more they stay the same.
PHYSICS 103: Lecture 12 Review of Example Problems Energy and Work Agenda for Today:
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.
Conservative and Nonconservative Forces
Springs And pendula, and energy.
Work, energy and power.
Energy.
Topic VII Work and Energy
Potential Energy and Conservation of Energy.
Chapter 13 Work and Energy.
Work-Energy Theorem Energy is the ability to do work.
Aim: How do we explain conservation of energy?
Forms of mechanical energy
Simple Harmonic Motion and Wave Interactions
Ch 4 Energy Kinetic Energy (KE) – the energy a moving object has because of its motion; depends on mass and speed of object KE = mv2/2 Joule – SI unit.
Physics and The Mousetrap Car
Presentation transcript:

Unit 3 Energy, Work, and Power

Energy is the ability to do work Work occurs when an object moves in the direction of an applied force (or component) Power is the rate at which work is done

Types of energy 1)Potential (U) a)Gravitational b)Elastic 2)Kinetic (K) 3)Mechanical (E)

Work and potential energy Gravitational potential energy change – Raise or lower object – Requires force – Requires a distance – Work is done Elastic potential energy change – Compress or stretch a “spring” – Requires force – Requires a distance – Work is done

Work and kinetic energy Kinetic energy change – Increase or decrease speed – Acceleration – Acceleration requires force – Acceleration and/or speed means distance – Work is done

W = ΔU* W = ΔK* ΔU = ΔK* *Sometimes A change in energy means work is done Work does not mean a change in kinetic and/or potential energy

Nonconservative forces cause a change in the energy of the system Work may be done to overcome friction In the absence of nonconservative forces W = ΔK + ΔU Energy is conserved in the absence of nonconservative forces

Kinetic energy K = ½mv 2

Mechanical energy is kinetic plus potential E = K + U

h x θ

A pendulum with l = 3.7 m and m = 7.2 kg is released from the horizontal. Determine the tension in the string when it makes an angle θ = 25º with the vertical. θ mg T θ