Aim: How do we apply conservation of energy to solving problems?

Slides:



Advertisements
Similar presentations
Castigliano’s theorems
Advertisements

Solving Equations = 4x – 5(6x – 10) -132 = 4x – 30x = -26x = -26x 7 = x.
College and Engineering Physics Potential Energy 1 TOC Definition of Potential Energy Examples of Potential Energy Types of Potential Energy.
09-1 Physics I Class 09 Potential Energy and Conservation of Energy.
King Fahd University of Petroleum & Minerals Mechanical Engineering Dynamics ME 201 BY Dr. Meyassar N. Al-Haddad Lecture # 16.
CHAPTER 14 Kinetics of a particle:Work and Energy 14.1 The Work of a Force 1. Definition of Work A force does work in a particle only when the particle.
12-1 Physics I Class 12 Conservative Forces and Potential Energy.
Fall wk 7 – Thus.11.Nov.04 Welcome, roll, questions, announcements Energy, work, and forces Review derivatives Spring workshop Energy Systems, EJZ.
King Fahd University of Petroleum & Minerals Mechanical Engineering Dynamics ME 201 BY Dr. Meyassar N. Al-Haddad Lecture # 16.
Physics 218: Mechanics Instructor: Dr. Tatiana Erukhimova Lecture 20.
Potential Energy and Conservation of Energy Work and Potential Energy Path Independence of Conservative Forces Determining Potential Energy Conservation.
AP PHYSICS REVIEW Energy. Work  Work is when a force is applied to an object to move it a distance.  W = Fd cos( Ɵ )  Work can be done by many forces.
Chapter 8 Conservation of Energy 8.2 Gravitational Potential Energy 8-3 Mechanical Energy and Its Conservation 8-4 Problem Solving Using Conservation of.
Central Force Motion Chapter 8
5.4 Exponential Functions: Differentiation and Integration The inverse of f(x) = ln x is f -1 = e x. Therefore, ln (e x ) = x and e ln x = x Solve for.
Motion Summary.  Vectors & Scalars  Displacement, Velocity, Acceleration  Equations of motion  Relative motion.
1 7.4 Conservative Forces and Potential Energy Define a potential energy function, U, such that the work done by a conservative force equals the decrease.
Work Done by a Varying Force (1D). Force Due to a Spring – Hooke’s Law.
Kinetic Energy and the Work/Energy Principle Energy is the ability to do work. Total energy is always conserved. A moving object can do work on another.
Aim: Differentiating & Integrating Expo Functions Course: Calculus Do Now: Aim: How do we differentiate and integrate the exponential function?
Mechanics Topic 2.3 Work, Energy and Power. Work A simple definition of work is the force multiplied by the distance moved However this does not take.
Equation y + 5 y + 5 = 20 Expressions
Chapter 7 Outline Potential Energy and Energy Conservation Gravitational potential energy Conservation of mechanical energy Elastic potential energy Springs.
Chapters 7, 8 Energy. What is energy? Energy - is a fundamental, basic notion in physics Energy is a scalar, describing state of an object or a system.
Indefinite Integrals. Find The Antiderivatives o Antiderivatives- The inverse of the derivative o Denoted as F(x) o Leibniz Notation: (indefinite integral)
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.
Solving equations with polynomials – part 2. n² -7n -30 = 0 ( )( )n n 1 · 30 2 · 15 3 · 10 5 · n + 3 = 0 n – 10 = n = -3n = 10 =
Work = Force x Displacement …when F and D are in the same direction (The block would be accelerating !)
Work and Energy. Scalar (Dot) Product When two vectors are multiplied together a scalar is the result:
Work Readings: Chapter 11.
CHS: M.Kelly Potential Energy and Conservation of Energy.
2.1 The Derivative and The Tangent Line Problem Slope of a Tangent Line.
The Fundamental Theorem for Line Integrals
In this chapter we will introduce the following concepts:
Work, Energy and Power. Energy: Energy can neither be created nor destroyed. It comes in many forms: Kinetic Potential (gravitational, chemical, elastic)
-Relating Conservative Force and Potential Energy -Energy diagrams and Equilibrium AP Physics C Mrs. Coyle.
Ch. 8: Summary So Far We’re doing the “2 body”, conservative central force problem! 2 bodies (m 1 & m 2 ) with a central force directed along the line.
Work The work done on an object by a constant force is given by: Units: Joule (J) The net work done on an object is the sum of all the individual “works”
Solution: Physics 1710 Chapter 8—Potential Energy Power = dW/dt = (Fdx)/dt = F dx/dt = F v (for F constant) = (20.0 N )(36 x 10 3 m/ 3600 sec) = 200. N.
Revision and Consolidation 08/09/2002By Mr. NGAN HON SHING1 Revision and Consolidation.
Table of Contents 8.2 What Is Energy? Energy and Motion.
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.
 Derive and use the equation for gravitational potential energy close to the Earth’s surface.  Use the equation for kinetic energy.  Solve problems.
Work/Energy Potential Energy 1 Definition of Potential Energy Examples of Potential Energy Types of Potential Energy.
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.
Solving and Graphing Absolute Value Inequalities
Topic VII Work and Energy
Section 3.7 – Potential Energy
Conservation of energy
Announcements M: Power T: Internal Energy + Student Questions W: Lab
Work, Power, & Energy.
Homework Questions.
Potential Energy and Conservation of Energy
Chapter 13 Work and Energy.
Topic: Energy Physics 231.
What is energy? Chapter 5 section 1.
Conservation of Energy
Aim: How do we analyze energy diagrams and stability of equilibrium?
Initial: On the floor Final: On the table System: Ball and Earth
Derivative or Integral
Derivation of the Exchange of Velocities
Chapter 17 Electric Potential.
Downslope Wind Events.
Potential Energy.
Physical Science: Chapter 13 Section 3: Energy
Mechanical Energy.
Integrated Science Unit 7 - Physics
Chapter 5 Work and energy.
Electric Potential Energy
Potential Energy and Conservation of Energy
Presentation transcript:

Aim: How do we apply conservation of energy to solving problems?

Conservative Forces We have only spoken about two forms of potential energy; gravitational potential energy and elastic potential energy. However, we know that there must exist other forms of potential energy. What is the link between the force and its associated potential energy function?

F=-dU/dx Since the work done by a conservative force is equal to negative the change in potential energy and the work done by a conservative force is equal to the integral of the force with respect to position, we can derive that WC=-ΔU and W=∫Fdx F=-dU/dx

Derive an equation for the force function of the following potential energy function 1) U(x) = 4x3 -7x dU/dx=12x2-7 F=-12x2 + 7 2) U(x) = -10x2 + 4 dU/dx=-20x F=20x 3) U(x) = 10/x5 +8/x4 dU/dx=-50x-6 -32x-5 F=50x-6 +32x-5 4) U(r) = -5r7 dU/dr= -35r6 F=35r6 5) U(r) = 2/r3 – 11/r dU/dr = -2r-4 + 22r-2 F=2r-4 -22r-2