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    Questions?

    Lecture 25Superposition of periodic motions

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    Superposed vibrations in 1d

    In linear systems resultant of more than oneharmonic displacements is the sum of individualvibrations

    x1=A

    1cos( t+

    1) x

    2=A

    2cos( t+

    2)

    Same frequency

    x=x1+x

    2=Acos( t+)

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    Complex exponential formalism

    x1=A

    1cos( t+

    1)=(A

    1e

    i ( t+1))

    x2=A2cos

    ( t+2)=(A2 ei ( t+

    2)

    )

    x=x1+x

    2=(A

    1e

    i (1

    t+1)+A

    2e

    i (2

    t+2))

    z=z1+z

    2=e i (1 t+1)(A

    1+A

    2e

    i (2

    1))

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    z

    =e

    i (1t+

    1)

    (A

    1

    +A

    2e

    i (2

    1)

    )

    z1

    z2

    Phase differencebetween the

    vibrations

    A

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    Superposition of vibrations different frequencies

    x1=A

    1cos(

    1t) x2=A2 cos(2 t)

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    Beats

    x=x1+x2=A(cos

    (1 t)+cos

    (2 t))

    Equal amplitudes, different frequencies

    = 2A cos

    1

    2

    2t cos

    1+

    2

    2t

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    Beats

    x=x1+x

    2=A(cos(

    1t)+cos(

    2t))

    Equal amplitudes, different frequencies

    =2A cos

    1

    2

    2t cos

    1+

    2

    2t

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    Questions?

    Lecture 26Superposition of periodic motions

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    Questions?

    Lecture 27Vibrations at right angles

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    Vibrations at right angles

    x=A1cos(

    1t+

    1) y=A2cos(2 t+2)

    1=2

    Possible cases

    12

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    Perpendicular motion samefrequencies

    x=A1cos( t) y=A2 cos( t+)

    Initial phase difference

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    A1=A

    2=1

    =0 =2

    =4

    The motion starts atthe dark red spot andgoes towards the lightred spot, alwaysfollowing the blue line

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    x=cos( t)

    y=cos( t+4)

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    x=cos( t)

    y=cos( t+4 )

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    Questions?

    Lecture 28Vibrations at right angles

    ( different frequencies )

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    Perpendicular motion differentfrequencies Lissajous figures

    x=cos( t)

    y=cos(2 t+4)

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    x=cos( t)

    y=cos(2 t+4) Step 1

    Identify the initial points

    on the circles.

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    x=cos( t)

    y=cos(2 t+4) Step 2

    Draw a horizontal line

    through the point onthe circle for y-axismotion

    Draw a vertical linethrough the point onthe circle for x-axismotion

    The intersection of thelines will give a pointon the Lissajous figure.

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    x=cos( t)

    y=cos(2 t+4) Step 3

    Find the positions on

    the circles after time dt

    Repeat Step 2

    Join the points foundfor the Lissajous figure

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    x=cos( t)

    y=cos(2 t+4) Step 4

    Repeat Step 3, i.e.,

    Find the positions onthe circles after time2 dt

    Repeat Step 2

    Join the points foundfor the Lissajous figure

    Note: Angle covered bythe point on the circleswill be proportional to

    the correspondingan ular s eeds.

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    x=cos( t)

    y=cos(2 t+4)

    Repeat the last stepand you will constructthe Lissajous figure.

    Any checkpoint?

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    x=cos( t)

    y=cos(2 t+4)

    Checks:

    After completing the

    Lissajous figure :

    Count how many timesthe curve reaches anextreme value of x (ory) to complete thecurve.

    Here Max[x] is reached

    once

    Max[y] is reached twice

    Notice the ratio of thefrequencies.

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    Homework

    Use this check on all the figures given in the textbook.

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    Questions?

    Lecture 29Coupled Oscillators

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    Coupled oscillators

    Two independent pendula are connected by aspring

    Set one of them in motion

    Observe the exchange of energy between thetwo

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    Coupled oscillators

    Restoring forces on each massF

    res A=m02xA+k(xAxB)

    Fres B=m0

    2xBk(xAxB)

    Due to motion ofthe pendulum

    Due to the spring

    Note the sign

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    Equations of motion

    m xA+m02xA+k(xAxB)=0

    m

    xB+m

    0

    2x

    Bk(x

    Ax

    B)=0

    q1+

    0

    2q

    1=0 q1=xA+xB

    q2+ '2 q

    2=0 q2=xAxB '

    2=02+2

    k

    m

    Add

    Subtract

    Solution ??

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    q1=xA+xB=Ccos(0 t+1)

    q2=xAxB=D cos( ' t+2)

    xA=[Ccos(0 t+1)+D cos( ' t+2)]/2

    xB=[Ccos(0 t+1)D cos( ' t+2)]/2

    C ,1, D ,2 : from the initial conditions on the masses

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    Special cases

    Initially both masses are given the same displacementfrom equilibrium (in the same direction) and releasedfrom rest

    Initially both masses are given the same displacementfrom equilibrium (in opposite directions) and releasedfrom rest

    One of the masses (say A) is displaced and releasedfrom rest (Exercise : Find Cand D).

    D=0q2=xAxB=0 at t=0

    C=0q1=xA+xB=0 at t=0