Work, Energy & Power Honors Physics. There are many different TYPES of Energy. Energy is expressed in JOULES (J) 4.19 J = 1 calorie Energy can be expressed.

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Presentation transcript:

Work, Energy & Power Honors Physics

There are many different TYPES of Energy. Energy is expressed in JOULES (J) 4.19 J = 1 calorie Energy can be expressed more specifically by using the term WORK(W) Work = The Scalar Dot Product between Force and Displacement. So that means if you apply a force on an object and it covers a displacement you have supplied ENERGY or done WORK on that object.

Scalar Dot Product? A product is obviously a result of multiplying 2 numbers. A scalar is a quantity with NO DIRECTION. So basically Work is found by multiplying the Force times the displacement and result is ENERGY, which has no direction associated with it. A dot product is basically a CONSTRAINT on the formula. In this case it means that F and x MUST be parallel. To ensure that they are parallel we add the cosine on the end. FORCE Displacement

Work FORCE Displacement

Work FORCE Displacement

Work In the figure above, we see the woman applying a force at an angle theta. Only the HORIZONTAL COMPONENT actually causes the box to move and thus imparts energy to the box. The vertical component (Fsin  ) does NO work on the box because it is NOT parallel to the displacement.

The Work Energy Theorem Up to this point we have learned Kinematics and Newton's Laws. Let 's see what happens when we apply BOTH to our new formula for WORK! 1.We will start by applying Newton's second law! 2.Using Kinematic #3! 3.An interesting term appears called KINETIC ENERGY or the ENERGY OF MOTION!

The Work Energy Theorem And so what we really have is called the WORK-ENERGY THEOREM. It basically means that if we impart work to an object it will undergo a CHANGE in speed and thus a change in KINETIC ENERGY. Since both WORK and KINETIC ENERGY are expressed in JOULES, they are EQUIVALENT TERMS! " The net WORK done on an object is equal to the change in kinetic energy of the object."

Example Suppose the woman in the figure above applies a 50 N force to a 25-kg box at an angle of 30 degrees above the horizontal. She manages to pull the box 5 meters. a)Calculate the WORK done by the woman on the box b)The speed of the box after 5 meters if the box started from rest J 4.16 m/s

Lifting mass at a constant speed Suppose you lift a mass upward at a constant speed,  v = 0 &  K=0. What does the work equal now? Since you are lifting at a constant speed, your APPLIED FORCE equals the WEIGHT of the object you are lifting. Since you are lifting you are raising the object a certain “y” displacement or height above the ground. When you lift an object above the ground it is said to have POTENTIAL ENERGY

Potential Energy mg h Since this man is lifting the package upward at a CONSTANT SPEED, the kinetic energy is NOT CHANGING. Therefore the work that he does goes into what is called the ENERGY OF POSITION or POTENTIAL ENERGY. All potential energy is considering to be energy that is STORED!

Potential Energy h The man shown lifts a 10 kg package 2 meters above the ground. What is the potential energy given to the package by the man? 196 J

Suppose you throw a ball upward What does work while it is flying through the air? Is the CHANGE in kinetic energy POSITIVE or NEGATIVE? Is the CHANGE in potential energy POSITIVE or NEGATIVE? GRAVITY NEGATIVE POSITIVE

ENERGY IS CONSERVED The law of conservation of mechanical energy states: Energy cannot be created or destroyed, only transformed! Energy BeforeEnergy After Am I moving? If yes, K o Am I above the ground? If yes, U o Am I moving? If yes, K Am I above the ground? If yes, U

Conservation of Energy In Figure A, a pendulum is released from rest at some height above the ground position. It has only potential energy. In Figure B, a pendulum is still above the ground position, yet it is also moving. It has BOTH potential energy and kinetic energy. In Figure C, a pendulum is at the ground position and moving with a maximum velocity. It has only kinetic energy. In Figure D, the pendulum has reached the same height above the ground position as A. It has only potential energy.

Conservative vs Nonconservative Forces As you saw when lifting a book, the work that you do "against gravity" in lifting is stored (somewhere... Physicists say that it is stored "in the gravitational field" or stored "in the Earth/book system".) and is available for kinetic energy of the book once you let go. Forces that store energy in this way are called conservative forces. Gravity is a conservative force, and there are many others. Elastic (Hooke's Law) forces, electric forces, etc. are conservative forces. These are sometimes called internal forces and they conserve the total mechanical energy of an object. They change the type of energy of the object/system. As you saw when pushing a book, the work that you do "against friction" is apparently lost - it is certainly not available to the book as kinetic energy! Forces that do not store energy are called nonconservative or dissipative forces. Friction is a nonconservative force, and there are others. Any friction-type force, like air resistance, is a nonconservative force. The energy that it removes from the system is no longer available to the system for kinetic energy. Some books consider all external forces nonconservative since they change the energy of the system (depending upon whether positive or negative work is done). Of course, if energy is a "real thing," the energy removed by a nonconservative force can't just disappear! Where does it go?

Energy consistently changes forms

PositionmvUKME 160 kg8 m/s Am I above the ground? Am I moving? NO, h = 0, U = 0 J 0 J Yes, v = 8 m/s, m = 60 kg 1920 J (= U+K) 1920 J

Energy consistently changes forms PositionmvUKME 160 kg8 m/s0 J1920 J 260 kg Energy Before = Energy After KOKO = U + K 1920= (60)(9.8)(1) + (.5)(60)v = v J 1332 = 30v = v 2 v = 6.66 m/s 6.66 m/s 1920 J 1332 J

Energy consistently changes forms PositionmvUKME 160 kg8 m/s0 J1920 J 260 kg6.66 m/s588 J1332 J1920 J 360 kg1920 J Am I moving at the top?No, v = 0 m/s 0 m/s0 J1920 J E B = E A Using position 1 K o = U 1920 = mgh 1920 =(60)(9.8)h h = 3.27 m

Spring Constants and Energy Conservation Objective: Determine the spring constant k of a spring using energy conservation principles. Materials: meter stick, pop-up toy, balance Procedure: You decide

Power One useful application of Energy is to determine the RATE at which we store or use it. We call this application POWER! As we use this new application, we have to keep in mind all the different kinds of substitutions we can make. Unit = WATT or Horsepower