A PRESENTATION ON VIBRATION

Slides:



Advertisements
Similar presentations
Oscillations and Simple Harmonic Motion:
Advertisements

Coulomb or Dry Friction Damping.
Revision Previous lecture was about Harmonic Oscillator.
Ch 3.8: Mechanical & Electrical Vibrations
Lecture 2 Free Vibration of Single Degree of Freedom Systems
FCI. Prof. Nabila.M.Hassan Faculty of Computer and Information Basic Science department 2013/ FCI.
Mechanical Vibrations
Phy 212: General Physics II Chapter 15: Oscillations Lecture Notes.
The simple pendulum Energy approach q T m mg PH421:Oscillations F09
Copyright © Cengage Learning. All rights reserved. 17 Second-Order Differential Equations.
Copyright © 2009 Pearson Education, Inc. Lecture 1 – Waves & Sound a) Simple Harmonic Motion (SHM)
Oscillations An oscillation is a repetitive to-and- fro movement. There are two types of vibration: free and forced. A forced vibration is produced when.
Chapter 13 Oscillatory Motion.
Chapter 15 Oscillatory Motion.
Mechanical Vibrations
Harmonic Oscillation 1. If a force F acts on a spring, the length x changes. The change is proportional to the restoring force (Hooke’s Law). A spring.
Chapter 19 MECHANICAL VIBRATIONS
Mechanical Vibrations
Energy of the Simple Harmonic Oscillator. The Total Mechanical Energy (PE + KE) Is Constant KINETIC ENERGY: KE = ½ mv 2 Remember v = -ωAsin(ωt+ ϕ ) KE.
SIMPLE HARMONIC MOTION Chapter 1 Physics Paper B BSc. I.
Chapter 14 Periodic Motion.
16.1 Simple Harmonic Motion
Copyright © 2010 Pearson Education, Inc. Lecture Outline Chapter 13 Physics, 4 th Edition James S. Walker.
Oscillations – motions that repeat themselves Period ( T ) – the time for one complete oscillation Frequency ( f ) – the number of oscillations completed.
SECOND ORDER LINEAR Des WITH CONSTANT COEFFICIENTS.
SECOND-ORDER DIFFERENTIAL EQUATIONS
Chapter 15 Oscillations. Periodic motion Periodic (harmonic) motion – self-repeating motion Oscillation – periodic motion in certain direction Period.
Oscillatory motion (chapter twelve)
Oscillations – motions that repeat themselves Period ( T ) – the time for one complete oscillation Frequency ( f ) – the number of oscillations completed.
Vibrations and Waves Hooke’s Law Elastic Potential Energy Simple Harmonic Motion.
APHY201 1/30/ Simple Harmonic Motion   Periodic oscillations   Restoring Force: F = -kx   Force and acceleration are not constant  
Copyright © 2010 Pearson Education, Inc. Chapter 13 Oscillations about Equilibrium.
1 Teaching Innovation - Entrepreneurial - Global The Centre for Technology enabled Teaching & Learning M G I, India DTEL DTEL (Department for Technology.
Oscillations Readings: Chapter 14.
Oscillations. Periodic Motion Periodic motion is motion of an object that regularly returns to a given position after a fixed time interval A special.
Damped harmonic oscillator
Whenever the force acting on an object is: Whenever the force acting on an object is: 1. Proportional to the displacement 2. In the opposite direction,
1 10. Harmonic oscillator Simple harmonic motion Harmonic oscillator is an example of periodic motion, where the displacement of a particle from.
PHY 151: Lecture Motion of an Object attached to a Spring 12.2 Particle in Simple Harmonic Motion 12.3 Energy of the Simple Harmonic Oscillator.
SIMPLE HARMONIC OSCILLATION
SIMPLE HARMONIC OSCILLATION
Chapter 13: Oscillatory Motion
Physics Vibrations and Waves ....
Mechanical Vibrations
10. Harmonic oscillator Simple harmonic motion
Voronkov Vladimir Vasilyevich
Periodic Motion Oscillations: Stable Equilibrium: U  ½kx2 F  kx
Lecture No. 2: Damped Oscillations, Driven Oscillations and Resonance
Solving the Harmonic Oscillator
Oscillations AP Physics C.
Theoretical Mechanics DYNAMICS
A spring with a 4-kg mass has natural length 0
Chapter 15 Oscillatory Motion
Oscillations Readings: Chapter 14.
Oscillatory Motion Periodic motion Spring-mass system
The Simple Pendulum A simple pendulum consists of a mass at the end of a lightweight cord. We assume that the cord does not stretch, and that its mass.
Simple Harmonic Motion
Lecture Outline Chapter 13 Physics, 4th Edition James S. Walker
LECTURE 1 – FUNDAMENTAL OF VIBRATION
Oscillations and Harmonic Motion
ENGINEERING MECHANICS
Chapter 14 Periodic Motion.
VIBRATION.
VIBRATION.
Chapter 15 Oscillations.
Copyright © 2014 John Wiley & Sons, Inc. All rights reserved.
Principles of Dynamics
Simple Harmonic Motion and Wave Interactions
PHYS 1443 – Section 501 Lecture #25
Presentation transcript:

A PRESENTATION ON VIBRATION PREPARED BY: CHANDAN PAL ROLL NO-10800711025 DEPT- ME SEM/YEAR- 5th/3rd PREPARED FOR: SEMINAR –I (ME 581 SESSIONAL) ASANSOL ENGINEERING COLLEGE DEPARTMENT OF MECHANICAL ENGINEERING ASANSOL

A Presentation on Mechanical Vibrations

Introduction Mechanical vibration is the motion of a particle or body which oscillates about a position of equilibrium. Time interval required for a system to complete a full cycle of the motion is the period of the vibration. Number of cycles per unit time defines the frequency of the vibrations. Maximum displacement of the system from the equilibrium position is the amplitude of the vibration. When the motion is maintained by the restoring forces only, the vibration is called free vibration. When a periodic force is applied to the system, the motion is described as forced vibration. When the frictional dissipation of energy is neglected, the motion is said to be undamped. Actually, all vibrations are damped to some degree.

Free Vibrations of Particles-Simple Harmonic Motion If a particle is displaced through a distance xm from its equilibrium position and released with no velocity, the particle will undergo simple harmonic motion, General solution is the sum of two particular solutions, x is a periodic function and wn is the natural circular frequency of the motion. C1 and C2 are determined by the initial conditions:

amplitude phase angle period natural frequency Displacement is equivalent to the x component of the sum of two vectors which rotate with constant angular velocity amplitude phase angle period natural frequency

Velocity-time and acceleration-time curves can be represented by sine curves of the same period as the displacement-time curve but different phase angles.

Simple Pendulum (Approximate Solution) Results obtained for the spring-mass system can be applied whenever the resultant force on a particle is proportional to the displacement and directed towards the equilibrium position. Consider tangential components of acceleration and force for a simple pendulum, for small angles,

Simple Pendulum (Exact Solution) An exact solution for leads to which requires numerical solution.

Free Vibrations of Rigid Bodies If an equation of motion takes the form the corresponding motion may be considered as simple harmonic motion. Consider the oscillations of a square plate Analysis objective is to determine wn. For an equivalent simple pendulum,

Principle of Conservation of Energy Resultant force on a mass in simple harmonic motion is conservative - total energy is conserved. Consider simple harmonic motion of the square plate,

Forced Vibrations Forced vibrations - Occur when a system is subjected to a periodic force or a periodic displacement of a support. forced frequency

Substituting particular solution into governing equation, At wf = wn, forcing input is in resonance with the system.

Damped Free Vibrations All vibrations are damped to some degree by forces due to dry friction, fluid friction, or internal friction. With viscous damping due to fluid friction, Substituting x = elt and dividing through by elt yields the characteristic equation, Define the critical damping coefficient such that

Characteristic equation, critical damping coefficient Light damping: c < cc damped frequency Heavy damping: c > cc - negative roots - nonvibratory motion Critical damping: c = cc - double roots - non-vibratory motion

Damped Forced Vibrations magnification factor phase difference between forcing and steady state response

Electrical Analogues Consider an electrical circuit consisting of an inductor, resistor and capacitor with a source of alternating voltage Oscillations of the electrical system are analogous to damped forced vibrations of a mechanical system.

Electrical Analogues The analogy between electrical and mechanical systems also applies to transient as well as steady state oscillations - With a charge q = q0 on the capacitor, closing the switch is analogous to releasing the mass of the mechanical system with no initial velocity at x = x0. If the circuit includes a battery with constant voltage E, closing the switch is analogous to suddenly applying a force of constant magnitude P to the mass of the mechanical system.

Electrical Analogues The electrical system analogy provides a means of experimentally determining the characteristics of a given mechanical system. For the mechanical system, For the electrical system, The governing equations are equivalent. The characteristics of the vibrations of the mechanical system may be inferred from the oscillations of the electrical system.

Thank You Chandan Pal Roll-10800711025 Reg. No.- 111080110392