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DEpartment of physics

THUSHARI Jayasekera - ASSistant Professor

Classical Machanics - PHYS 310
Class Meets on MWRF 8.00 am - 8.50 am
Office Hours - WR 2.00 pm - 5.00 pm (Neckers 489)
 

       

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Lecture 10

  • In this lecture,we will discuss the effect of driving forces on the damped harmonic oscillator. We talk about the general solution to this problem, and graphicall visualize it.

10.1 Resonance Phenomena



10.1 Resonance Phenomena

In the last lecure,we discussed about the resonance phenomena. Let's work on the math now find out the condition for occuring the resonance. The system is described by a natural frequency and a damping coefficient. We need to find out the frequency of the driving force for this system such that the maximum amplitude of the position coordinate.

Resonance

that means at this resonance frequency, D is a maximum.

Let's look at the amplitude as a function of frequency, and see the resonance frequency and the maximum amplitude.



The above CDF was created by Thushari Jayasekera
Quality Factor of Resonance

As you can see from the above CDF player, the width of the resonance is charaacerized by the damping coefficient of the oscillator. So we define the Quality Factor of the Driven Oscillator as,

QualityFactor.png
As the damping coefficeint is small, we see sharper resonance. So the Q is larger for sharper resonance.

Let's do few more Problems with Simple Harmonic Oscillator
Thushari Jayasekera, Assistant Professor of Physics, Southern Illinois University - Carbondale
Tel: 618 453 1055 Fax: 618 453 1056

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