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Subject: Physics

Lesson 3: Mechanical Oscillator

Class: Grade 12-LS

Section: A & B

Done By Mr. Nawaf AL Souheil

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Objectives

-Quick review for the trigonometric functions

-Quick review for the differential equation

-Define the horizontal oscillator

-Energetic study for the Simple Harmonic motion (SHM)

-Define the periodic motion

-Dynamic study for the simple harmonic motion (SHM)

-Solution for the differential equation

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Trigonometric Function

Sin(x) & Cos(x)

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Graph of the Sine Function

To sketch the graph of y = sin x first locate the key points.�These are the maximum points, the minimum points, and the intercepts.

0

-1

0

1

0

sin x

0

x

Then, connect the points on the graph with a smooth curve that extends in both directions beyond the five points. A single cycle is called a period.

y

x

y = sin x

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Graph of the Cosine Function

To sketch the graph of y = cos x first locate the key points.�These are the maximum points, the minimum points, and the intercepts.

1

0

-1

0

1

cos x

0

x

Then, connect the points on the graph with a smooth curve that extends in both directions beyond the five points. A single cycle is called a period.

y

x

y = cos x

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y

x

Example: Sketch the graph of y = 3 cos x on the interval [–π, 4π].

Partition the interval [0, 2π] into four equal parts. Find the five key points; graph one cycle; then repeat the cycle over the interval.

max

x-int

min

x-int

max

3

0

-3

0

3

y = 3 cos x

π

0

x

(0, 3)

( , 0)

( , 0)

( , )

( , – )

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The amplitude of y = a sin x (or y = a cos x) is half the distance between the maximum and minimum values of the function.

amplitude = |a|

If |a| > 1, the amplitude stretches the graph vertically.

If 0 < |a| > 1, the amplitude shrinks the graph vertically.

If a < 0, the graph is reflected in the x-axis.

y

x

y = – 4 sin x

reflection of y = 4 sin x

Is y= - 4sinx

y = 4 sin x

y = 2sin x

y = sin x

y = sin x

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Differential equation

A differential equation is any equation with a variable and its either first derivative or second derivative, or higher order derivative.

 

 

 

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Mathematical study of a second order differential equation:

 

 

 

 

 

 

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In physics all quantities of motion are studied with respect to time, and the position is denoted by x, thus the differential equation that we will study will have the form:

 

 

 

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Horizontal Oscillator

A horizontal oscillator is formed of a horizontal spring of stiffness K (in N/m), fixed at one end, while the other end a mass m is attached to it. (see the figure)

The motion of this oscillator is called: Simple Harmonic motion (SHM)

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Simple Harmonic Motion (SHM):

 

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Periodic motion:

Is the motion that repeats itself within a specific time interval called the period T of the motion.

Example: the second’s arm in the clock repeats its cycle each 1 minute, thus its period is T=1 min=60 s

 

Example: the harmonic motion repeats itself within its period that is defined by:

 

(This relation will be derived later)

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Energetic study of Horizontal Oscillator

Consider a horizontal oscillator formed of a spring with force constant K, and a block of mass m, placed as shown in the figure (Assume that the friction force is neglected):

 

At t=0, the system is released, and thus it begins to oscillate as shown in the figure.

The Motion of the system is called: Simple Harmonic motion (SHM)

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At t=0, the system is storing a pure elastic energy when the reference for the gravitational potential energy is taken along the horizontal axis of the oscillator.

Thus at t=0, the mechanical energy of the system (Spring,block,Earth) is given by:

 

 

At any instant t, the system is oscillating, and it possesses both kinetic and elastic potential energies.

Thus at any instant t, the mechanical energy of the system is given by:

 

 

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Since the friction force is neglected, so the mechanical energy is conserved, then:

 

 

Derive the obtained equation with respect to time t:

 

 

 

 

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Relation between oscillations and sinusoidal functions

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Dynamic Study:

Forces acting on the system during its motion in the absence of friction force are:

 

 

 

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Applying Newton’s Second law: