An Introduction to the Behavior of Waves

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  • 8/14/2019 An Introduction to the Behavior of Waves

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    Sanjitha N. Adikari

    An introduction to the

    behavior of waves

    Advanced level Physics AS

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    Sanjitha N. Adikari

    Principle of superposition

    Where two or more waves meet , the totaldisplacement at any point is the vector sum ofthe displacement that each individual waveswould cause at that point.

    Resultant wave

    Individual waves

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    Principle of superposition theorem

    Vector sum means

    Waves in turn depends upon the path

    different between the waves involved.

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    Sanjitha N. Adikari

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    Classifying waves Progressive waves

    The position of its perks and troughs are moving. These waves have a property to carry energy ( action

    at a distance)

    Eg: pebble thrown in to the water cause a water wavesspared out over the surface of water container.

    Stationary waves ( standing waves)

    The wave is not progressive. Its perks and troughsaren't moving. These waves have a property to create oscillation.

    Eg: guitar string, understanding the behavior of electronsand sub atomic particles

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    Stationary waves

    As the frequency of the cord is increasedresonance (the tendency of a system tooscillate at maximum amplitude at certainfrequencies) occurs.

    vibrator

    Wight to make a

    tension on string

    1

    Rubber cord

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    Stationary waves in a pipe.

    Open end pipe

    closed end pipe

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    Reflection at the end of string Setting up waves on a rope

    Fixedend Free end

    As the pulse reaches the end of the string the string exerts a force on

    the support. the support exerts a force equal in size but opposite in

    direction on the string.

    The phase change on reflection occurs where a hard reflection

    occurs. Fixed End)

    No phase change on reflection occurs where a hard reflection

    occurs. Fixed End)

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    air

    glass

    glass

    air

    If a wave traveling form a less

    dense medium to a more dense

    medium there is a PHASE

    CHANGE OF 180o

    If a wave traveling form a more

    dense medium to a less dense

    medium there is a NO PHASE

    CHANGE.

    D1 D2 D2 D1

    D2>D1

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    Reflection at a Point where the

    Wave Velocity Changesv2 > v1

    v2< v1

    Transmitted wave, no phase change.

    Reflected wave, phase change.

    Transmitted wave, no phase change.

    Reflected wave, no phase change.

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    Harmonics

    There are several frequencies with which

    the snaky can be vibrated to produce the

    patterns. Each frequency is associatedwith a different standing wave pattern.

    These frequencies and their associated

    wave patterns are referred to asharmonics.

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    First Harmonic (Fundamental

    Frequency of Resonance)

    All points oscillate in phase but with different amplitudes of oscillation.

    Consider the string to be disturbed at A (the centre).

    Waves travel towards B (and C) and are reflected with a 180 phase change.

    If the "effective distance" travelled by the waves is l, then resonance occurs.

    This means that, for the first resonance, the distance A B A (or A C A) must be

    equal to l/2.

    second Harmonic (Frequency ofResonance)

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    Organ

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    Nodes -The crests and troughs of a standing wave donot travel, or propagate, down the string. Instead, a

    standing wave has certain points, called nodes, thatremain fixed at the equilibrium position.

    Antinodes These are points where the original waveundergoes complete destructive interference with its

    reflection. In between the nodes, the points that oscillatewith the greatest amplitudewhere the interference iscompletely constructiveare called antinodes.

    NodesAntinodes

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    Finding the frequencies of the

    harmonics To find the frequencies of the harmonics

    for a stretched string. We can use the fact

    that the speed at which a transverse waveis propagated along a string.

    V = T/

    -Mass per unit length

    T- tension

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    We knowV = f

    And also we know = 2l/n

    Form these two equations we can have f = n/2 x v

    Form the equation for string

    fn = n/2l T/ where n = 1,2,3..

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    we can solve for the frequency, fn , for any term, n, in the harmonicseries. A higher frequency means a higher pitch.

    The equation tells you that a higher frequency is produced by a taut string, a string with low mass density, a string with a short wavelength.

    If you tighten a string, the pitch goes up

    the strings that play higher pitches are much thinner than the fatstrings for low notes

    by placing your finger on a string somewhere along the neck of theinstrument, you shorten the wavelength and raise the pitch .

    Theories behind the Guitar (musical instruments)

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    Sound waves and microwaves

    Sound Need a medium to travel..

    Speed approximately 342 m/s

    microwaves No medium required to travel it is a

    electromagnetic wave

    Speed approximately 100000000 m/s

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    Electromagnetic waves

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    Questions..