Kinetics of a particle: Work & Energy

Slides:



Advertisements
Similar presentations
Topics in textbook Actual Work Definition of Work Potential Energy
Advertisements

Work & Energy Principles
Work Done by a Constant Force
Work & Energy Principles
Kinetics of Particles: Energy and Momentum Methods
Conservative Forces and Potential Energy The force is called a conservative force when; The work done by a force in moving a particle from a one point.
King Fahd University of Petroleum & Minerals Mechanical Engineering Dynamics ME 201 BY Dr. Meyassar N. Al-Haddad Lecture # 16.
ENGR 215 ~ Dynamics Sections Impulse and Linear Momentum In this section we will integrate the equation of motion with respect to time and.
ENGR 215 ~ Dynamics Sections 14.1 – Conservation of Energy Energy can neither be created nor destroyed during a process, it can only change forms.
King Fahd University of Petroleum & Minerals Mechanical Engineering Dynamics ME 201 BY Dr. Meyassar N. Al-Haddad Lecture # 38.
King Fahd University of Petroleum & Minerals Mechanical Engineering Dynamics ME 201 BY Dr. Meyassar N. Al-Haddad Lecture # 16.
Kinetics of a Particle:
CHAPTER 13 Kinetics of a Particle:
General Physics 1, Additional questions By/ T.A. Eleyan
1a. Positive and negative work
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.
Elastic Potential Energy: More Practice. Conservation of Mechanical Energy: Learning Goal The student will investigate a simple energy transformation,
Dynamics: POWER AND EFFICIENCY Today’s Objectives: 1.Determine the power generated by a machine, engine, or motor. 2.Calculate the mechanical efficiency.
Chapter 5 Energy Phy 2053 Conceptual Questions
Give the expression for the velocity of an object rolling down an incline without slipping in terms of h (height), M(mass), g, I (Moment of inertia) and.
Kinetic Energy, Work, Power, and Potential Energy
Kinetic Energy, Work, Power, and Potential Energy
POWER AND EFFICIENCY Today’s Objectives: Students will be able to:
Potential Energy and Conservative Forces
Power, Efficiency, and Potential Energy Class Lectures 11: 3.6 & 7 Today’s Objective 1.Power and Efficiency 2.Potential Energy 3.Conservation of 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)
Sub title Potential Energy Work Work- Energy Theorem Kinetic Energy Power 200 Work-Power-Energy.
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.
POWER AND EFFICIENCY. APPLICATIONS Engines and motors are often rated in terms of their power output. The power output of the motor lifting this elevator.
Physics. Session Work, Power and Energy - 3 Session Objectives.
Today’s Objectives: Students will be able to:
Energy Examples Serway and Jewett 8.1 – 8.3 Physics 1D03 - Lecture 22.
POWER AND EFFICIENCY Today’s Objectives: Students will be able to:
APPLICATIONS A roller coaster makes use of gravitational forces to assist the cars in reaching high speeds in the “valleys” of the track. How can we design.
Work has a specific definition in physics
Work = Force x Displacement …when F and D are in the same direction (The block would be accelerating !)
 Work  Energy  Kinetic Energy  Potential Energy  Mechanical Energy  Conservation of Mechanical Energy.
Energy Energy Universe is made up of matter and energy. Energy is the mover of matter. Energy has several forms: –Kinetic –Potential –Electrical –Heat.
Conservative and Nonconservative Forces. A Force is “Conservative” if: The work it does on an object is available for kinetic energy. These forces store.
Work & Energy Principles
EnergyDefinitions 1 Different kinds of energy Kinetic energy Kinetic energy is motion energy. The faster it moves the more kinetic energy it possesses.
IB Physics 11 Mr. Jean November 3 rd, The plan: Video clips of the day Work Potential energy –Gravitational potential kinetic energy.
Work is only done by a force on an
Calculate the work of a force.
Conservation of Mechanical Energy: Learning Goal
Work & Energy Principles
KINETICS of PARTICLES Newton’s 2nd Law & The Equation of Motion
Aplications.
1a. Positive and negative work
Work Done by a Constant Force
Different kinds of energy
WORK And Energy and Power.
Work Done by a Constant Force
Chapter 5 Work and Energy
POWER AND EFFICIENCY Today’s Objectives: Students will be able to:
11/29/2018 Physics 253.
POWER AND EFFICIENCY Today’s Objectives: Students will be able to:
Potential Energy Problems
Work and Energy 2/4/2019 SHOW WORK DONE BY A COMPRESSED SPRING
POWER AND EFFICIENCY Today’s Objectives: Students will be able to:
Potential Potential Energy
King Fahd University of Petroleum & Minerals
PE, KE Examples Answers 1. A shotput has a mass of 7.0 kg. Find the potential energy of a shotput raised to a height of 1.8 m. m = 7.0 kg h.
What do we want to do today?! Sunday:
Chapter 14 : Kinematics Of A Particle – Work and Energy
Work, Energy, Power.
DEPARTMENT OF MECHANICAL ENGINEERING
POWER AND EFFICIENCY Today’s Objectives: Students will be able to:
T101-Q-1 Figure 1 shows the spring force as a function of position x for a spring-block system resting on a frictionless table. The block is released at.
Presentation transcript:

Kinetics of a particle: Work & Energy

Objectives To develop the principle of work and energy and apply it to solve problems that involve force, velocity, and displacement. To study problems that involve power and efficiency. To introduce the concept of a conservative force and apply the theorem of conservation of energy to solve kinetic problems. 14/11/61 MEE214 – Dynamics

Work of a Force A force F does work on a particle only when the particle undergoes a displacement in the direction of the force. 14/11/61 MEE214 – Dynamics

Work of a Force If the particle undergoes a finite displacement along its path from r1 to r2 or s1 to s2, the work is determined by integration. 14/11/61 MEE214 – Dynamics

Work of a Weight 14/11/61 MEE214 – Dynamics

Work of a Spring Force Work done on a spring Force and Displacement are in the same direction. 14/11/61 MEE214 – Dynamics

Work of a Spring Force Work done on a particle or body Force and Displacement are in the different direction. 14/11/61 MEE214 – Dynamics

Example 14.1 The 10-kg block rest on a smooth incline. If the spring is originally stretched 0.5 m, determine the total work done by all forces acting on the block when a horizontal force P = 400 N pushes the block up the plane s = 2 m. 14/11/61 MEE214 – Dynamics

Principle of Work and Energy Consider a particle P, which at the instant considered located on the path as measured from an inertial coordinate system. For the particle in the tangential direction, ∑Ft = mat 14/11/61 MEE214 – Dynamics

Principle of Work and Energy 14/11/61 MEE214 – Dynamics

Problem 14-13 The 2-lb brick slides down a smooth roof, such that when it is at A it has a velocity of 5 ft/s Determine the speed of the brick just before it leaves the surface at B, the distance d from the wall to where it strikes the ground, and the speed at which it hits the ground. 14/11/61 ME212 ดร. พิภัทร

Example 14.6 The block A and B have a mass of 10-kg and 100-kg respectively. Determine the distance B travels from the point where it is released from rest to the point its speed become 2 m/s. 14/11/61 MEE214 – Dynamics

Example 14.4 The platform P is tied down so that the 0.4-m-long cords keep a 1-m-long spring compressed 0.6-m when nothing is on the platform. If a 2-kg platform is placed on the platform and released from rest after the platform is pushed down 0.1 m, determine the max height h the block rises in the air, measure from the ground. 14/11/61 MEE214 – Dynamics

Power v Power It is defined as the amount of work performed per unit of time. The power generated by a machine or engine that performs an amount of work dU within a time interval dt is 14/11/61 MEE214 – Dynamics

Efficiency Efficiency It is defined as the ratio of the output of useful power produced by the machine to the input of power supplied to the machine 14/11/61 MEE214 – Dynamics

Example 14.8 The motor M of the hoist operates with an efficiency of ε = 0.85. Determine the power that must be supplied to the motor to lift the 375-N crate C at the instant point P on the cable has an acceleration of 1.2m/s2, and a velocity of 0.6 m/s 14/11/61 MEE214 – Dynamics

Conservative Force Work done is independent of the path Examples: Weight of a particle Elastic force of a spring 14/11/61 MEE214 – Dynamics

Potential Energy Amount of work done by a conservative force from moving from a given position to datum. Capacity of work stored in a particle. 14/11/61 MEE214 – Dynamics

Potential Energy 14/11/61 MEE214 – Dynamics

Conservation of Energy If a particle is subject to both conservative and non-conservative forces: No non-conservative forces: 14/11/61 MEE214 – Dynamics