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Unit 8 Superposition of waves AS/A Level Physics Cambridge CAIE 9702

1h 6m 11s8,493 words1,348 segmentsEnglish

FULL TRANSCRIPT

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hey everyone welcome to PL Academy hope

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you found this video

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you could subscribe like the video share

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it with your friends and maybe drop a

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comment your support really helps me

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make more

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videos in this video I covered

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everything on the syllabus like you can

0:28

see in the figure

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principle of

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superposition superposition is the

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principle that when waves of the same

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type meet at a point they individual

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displacements combined to produce a

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resultant

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displacement as a blue wave travels to

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the left and a red wave travels to the

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right initially they are in Phase

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meaning their phase difference is zero

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when these waves meet their individual

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displacements combine constructively

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resulting in a maximum resultant

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displacement that is twice the amplitude

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of either individual wave this is called

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constructive superposition which occurs

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when waves are in Phase with phase

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differences of 0 Dee creating the

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maximum

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amplitude when a blue wave travels One

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Division to the left and a red wave

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travels One Division to the right they

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individual displacements combined to

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create the resultant displacement as

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shown

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when a blue wave travels One Division to

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the left and a red wave travels One

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Division to the right the phase

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difference between two waves is pi

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radians or

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180° they are said to be in

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antiphase their individual displacements

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combined destructively resulting in a

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minimum resultant displacement which can

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be zero if the waves have equal

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amplitudes this is called destructive

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superposition which occurs when waves

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are in anti phase with phase differences

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of Pi radians or

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180° creating the zero

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amplitude when a blue wave travels One

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Division to the left and a red wave

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travels One Division to the right their

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individual displacements combined to

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create the resultant displacement as

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shown when a blue wave travels One

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Division to the left and a red wave

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travels One Division to the right the

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phase difference between two waves is 2

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pi radians or

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360° they are said to be in Phase their

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individual displacements combine

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constructively resulting in a maximum

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resultant displacement that is twice the

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amplitude of either individual wave this

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is called constructive superposition

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which occurs when waves are in Phase

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with phase differences of 2 pi radians

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or

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360° creating the maximum

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amplitude therefore we can be concluded

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that

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the constructive superposition which

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occurs when waves are in Phase with

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phase differences of 0 2 pi 4 Pi 6 pi

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and so on the destructive superposition

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which occurs when waves are antiphase

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with phase differences of Pi 3 Pi 5 Pi 7

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pi and so

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on exam style question one the three

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waves shown in each diagram have the

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same amplitude and frequency but

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different phase they are added together

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to give a resultant wave in which case

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is the resultant wave zero at this

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instant in a choice a there are three

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waves as blue violet and green coolers

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like this at this point displacements of

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three waves combined to be zero like

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this at this point displacements of

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three waves combined to be zero like

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this at at this point displacements of

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three waves combined to be zero like

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this and any positions the resultant

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displacements of three waves combined

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together to become zero like this so a

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is

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correct stationary wave stationary waves

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or standing waves are formed by the

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superposition or interference of two

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Progressive waves traveling in opposite

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directions with the the same frequency

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wavelength and speed this interference

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results in a pattern of nodes and

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antinodes at nodes are the destructive

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superposition their phase differences

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are Pi 3 Pi 5 Pi 7 pi and so on or

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180°

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540°

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900° 1,

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1260° and so on their path differences

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are Lambda over 2 3 Lambda over 2 5

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Lambda over 2 7 Lambda over 2 and so on

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at anodes are the constructive

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superposition their phase differences

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are 0 2 pi 4 Pi 6 pi and so on or 0°

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360°

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720° 1, 80° and so on their path

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differences are 0 Lambda 2 lamb LDA 3

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Lambda and so on when a blue wave

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travels to the right and a red wave

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travels to the left as shown they are

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moving in opposite directions and they

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have same frequency wavelength and speed

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at the initial they are in phase and

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phase difference is zero they superpose

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or interfere with each other to create

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the stationary wave shown in Black Wave

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After 1/8 of a period each wave travels

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1/8 of a wave length in opposite

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directions resulting in a separation of

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1/4 of a

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wavelength they superpose to form the

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stationary wave shown in Black Wave

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After 1/4 of a period each wave travels

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1/4 of a wavelength in opposite

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directions resulting in a separation of

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half the

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wavelength they superpose to form the

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stationary wave shown in Black Wave

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After 38 of a period each wave travels

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38 of a wavelength in opposite direction

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CS resulting in a 34s wavelength in

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separation they superpose to form the

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stationary wave shown in Black Wave

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after half of period each wave travels

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half a wavelength in opposite directions

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resulting in a full wavelength

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separation they superpose to form the

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stationary wave shown in Black Wave when

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two waves traveling at high speeds in

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opposite directions superpose they can

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form stationary waves which appear as a

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series of Loops as shown this creates a

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pattern of nodes and antinodes as shown

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at nodes the amplitude is at minimum in

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this diagram it is zero because the

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waves have equal

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amplitudes at antinodes the amplitude is

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maximum the distance between two Loops

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is equal to wavelength Lambda so the

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distance between consecutive nodes or

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antinodes are half of the wavelength

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exam style question two the diagram

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shows a sketch of a wave pattern over a

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short period of time which description

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of this wave is correct in the diagram

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shown the stationary wave the distance

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for two Loops is a wavelength for one

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meter has five Loops which is equivalent

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to 2.5

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wavelengths so we can determine the

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wavelength of the wave is equal to 1 m /

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2.5 which is 0.4 M or 40

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cm the transverse waves and longitudinal

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waves can be occurred the stationary

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wave in the choice a the wave is

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longitudinal has a wavelength of 20 cm

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and is

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stationary this is

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incorrect in the choice B the wave is

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transverse has a wavelength of 20 cm and

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is

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stationary this is incorrect

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in the choice C the wave is transverse

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has a wavelength of 40 cm and is

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Progressive this is

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incorrect in the choice d The Wave is

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transverse has a wavelength of 40 cm and

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is

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stationary this is

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correct stationary wave of the stretched

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string a vibrator generates an incident

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wave that travels to the left this wave

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reflects at the pulley creating a

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reflected wave traveling to the right

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the incident and reflected waves have

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the same frequency wavelength and speed

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these two waves superpose to produce a

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standing wave the simplest standing wave

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pattern with a single Loop is called the

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fundamental frequency or the first

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harmonic the fixed ends at the vibrator

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and pulley are always formed nodes

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because the string cannot free to

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vibrate

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the vibrator varies the frequency until

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a stationary wave with two Loops second

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harmonic three Loops third harmonic four

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Loops fourth harmonic and so on let L be

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the length of the stretched string

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recall that two Loops of stationary wave

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equals one

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wavelength for first harmonic has a

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single Loop indicating that L equals

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half of wavelength so the wavelength

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equals 2 L the fundamental frequency F1

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can be calculated by dividing the speed

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V by wavelength Lambda substituting

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Lambda equal 2 L so fub1 = V / 2L 4

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second harmonic has two Loops indicating

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that L equals wavelength Lambda the

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second harmonic frequency FS2 is

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calculated by dividing the speed V by

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wavelength Lambda substituting Lambda

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equals l so FS2 = V / l or 2 v/ 2 L and

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V / 2 L =

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fub1 so FS2 is twice as fub1 43d

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harmonic has three Loops indicating that

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L equals 3 Lambda / 2 so Lambda equal 2

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L over 3 the third harmonic frequency F3

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is calculated by dividing the speed V by

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wavelength Lambda substituting Lambda =

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2 L over 3 so F3 = 3 V / 2 L and V / 2 L

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equals

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FS1 so F3 is three times of fub1 for

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fourth harmonic has four Loops

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indicating that L equal 2 Lambda so

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Lambda equal L / 2 the fourth harmonic

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frequency F3 is calculated by dividing

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the speed V by wavelength Lambda

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substituting Lambda = L / 2 so F4 = 2 V

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/ l or 4 V / 2 L and V / 2 L =

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fub1 so F4 is fourth times of

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fub1 exam style question three a

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stationary wave is produced on a string

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that is stretched between two fixed

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points that are a distance of 1.35 M

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apart as shown the speed of the waves on

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the string is 450

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m/s what is the frequency of oscillation

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of the stationary wave the standing wave

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has three Loops which corresponds to 1.5

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wavelengths so 1.35 m equal 1.5

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wavelengths this means one wavelength is

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1.35 m / 1.5 is equal to 0.9 M the

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frequency of the stationary wave can be

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calculated by the equation FAL v/ Lambda

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substituting V equal 450 m/s and Lambda

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equal 0.9 M we get the frequency equals

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500

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htz so C is

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correct the stationary wave of sound

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wave in air column with close one end a

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speaker generates an incident sound wave

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that travels through a pipe closed at

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one end this wave reflects at the closed

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end creating a reflected wave traveling

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in the opposite direction the incident

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and reflected waves have the same

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frequency wavelength and speed the

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superposition of these two waves can

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produce a standing wave the simplest

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standing wave with a quarter Loop

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pattern is called the fundamental wave

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or the first

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harmonic this corresponds to the lowest

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frequency that can be heard hence the

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term fundamental frequency a closed end

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of the pipe forms a node because air

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particles cannot vibrate freely an open

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end forms an antinode because air

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particles can vibrate freely the speaker

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varies the frequency until a stationary

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wave with second her second harmonic

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three herd third harmonic and so on let

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L be the length of the air column recall

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that two Loops of stationary wave equals

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one

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wavelength for first harmonic has an

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one4 Loop pattern indicating that L

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equals 1/4 of a wavelength so the

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wavelength equals 4 L the fundamental

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frequency fub1 can be calculated by

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dividing the speed V by wavelength

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Lambda substituting Lambda equal 4 L so

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fub1 = v/ 4 L 4C harmonic has a 3/4 Loop

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pattern indicating that L equals 3/4 of

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a wavelength so the wavelength equals 4

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L over 3 the second harmonic frequency

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FS2 can be calculated by dividing the

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speed V by wavelength Lambda

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substituting Lambda equals 4 L over 3 so

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F2 = 3 V over 4 L and V over 4 L = fub1

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so FS2 = 3 * of fub1 43 harmonic has a

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54 Loop pattern indicating that L equals

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5/4 of a wavelength so the wavelength

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equals 4 L the third harmonic frequency

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F3 can be calculated by dividing the

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speed V by wavelength Lambda

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substituting Lambda equals 4 L over 5 so

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F3 = 5 V over 4 L and V over 4 L =

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fub1 so F3 = 5 * of

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fub1 exam style question four a long

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glass tube is almost completely immersed

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in a large tank of water a tuning fork

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is struck and held just above the open

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end of the tube as it is slowly raised a

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louder sound is first heard when the

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height h of the end of the tube above

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the water is 18.8

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CM a louder sound is next heard when H

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is 56.4

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cim the speed of sound in air is 330

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m/s what is the frequency of the sound

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produced by The Tuning Fork the first

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herd when H is 18.8

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CM the next herd when H is 56.4

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CM so half of wave length equal

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56.4 - 18.8 is equal to 37.6

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CM therefore 1 wavelength equal 2 *

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37.6 is equal to

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0.752 M the frequency can be calculated

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using the equation FAL V / Lambda

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substituting V = 330 m/s and Lambda

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equal 0.7 5 2

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m we get the frequency F equal 440 Hertz

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for two significant figures so B is

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correct the stationary wave of sound

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wave in air column with open both ends a

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speaker generates an incident sound wave

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that travels through an open pipe this

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wave reflects at the open end creating a

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reflected wave traveling in the opposite

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direction

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the incident and reflected waves have

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the same frequency wavelength and speed

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the superposition of these two waves can

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produce a standing wave the simplest

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standing wave with one Loop pattern is

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called the fundamental wave or the first

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harmonic this corresponds to the lowest

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frequency that can be heard hence the

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term fundamental

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frequency both open ends forms an

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antinode because air particles can

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vibrate freely

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the speaker varies the frequency until a

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stationary wave with second her second

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harmonic three herd third harmonic and

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so on let L be the length of the air

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column recall that two Loops of

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stationary wave equals one

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wavelength for first harmonic has an one

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Loop pattern indicating that L equals

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half of a wavelength so the wavelength

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equals 2 L the fundamental frequency

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fub1 can be calculated by dividing the

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speed V by wavelength Lambda

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substituting Lambda equals 2 L so fub1 =

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V / 2 L 4 second harmonic has a two

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Loops pattern indicating that L equals

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one

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wavelength the second harmonic frequency

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F2 can be calculated by dividing the

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speed V by wavelength Lambda

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substituting Lambda equals l so F2 = V /

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l or 2 V / 2 L and v/ 2 L =

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fub1 so FS2 = 2 * of fub1 43 harmonic

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has a three Hales Loops pattern

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indicating that L equals 3 halves of a

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wavelength so the wavelength equals 2 L

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over 3 the third harmonic frequency F3

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can be calculated by dividing the speed

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V by wavelength Lambda substitute Lambda

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= 2 l/ 3 so F3 = 3 V / 2 L and v/ 2 L =

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fub1 so F3 = 3 * of

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fub1 exam style question five stationary

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sound waves can be formed in the air

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Columns of pipes one type of pipe is

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closed at one end and open at the other

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end

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another of pipe is open at both ends

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which pipe can form a stationary sound

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wave with the lowest frequency let V

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represent the speed of sound in air

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Choice a consider a pipe open at both

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ends the lowest frequency or fundamental

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frequency standing wave has a half

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wavelength pattern one Loop is shown one

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Loop is equivalent to half

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wavelength so 2 L equals a half of

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Lambda and Lambda equal 4 L using the

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equation the frequency F equal speed V

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over wavelength Lambda substituting

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Lambda equals 4 L so F = 0.25 V over L

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Choice B consider a pipe is closed at

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one end the lowest frequency or

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fundamental frequency standing wave has

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a quarter wavelength pattern half Loop

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is shown a half Loop is equivalent a

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quarter

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wavelength so 2 L = 1/4 Lambda and

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Lambda equal 8 L using the equation the

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frequency F equal speed V over

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wavelength Lambda substituting Lambda

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equal 8 l so F =

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0.125 V / L Choice C consider a pipe

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open at both ends the lowest frequency

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or thund mental frequency standing wave

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has a half wavelength pattern one Loop

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is shown one Loop is equivalent to half

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wavelength so L equals a half of Lambda

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and Lambda equal 2 L using the equation

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the frequency FAL speed V over

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wavelength Lambda substituting Lambda

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equal 2 L so F equal 0.5 V / L Choice d

21:59

consider a pipe is closed at one end the

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lowest frequency or fundamental

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frequency standing wave has a quarter

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wavelength pattern half Loop is shown a

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half Loop is equivalent to quarter

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wavelength so L equal 1/4 Lambda and

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Lambda equal 4 L using the equation the

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frequency F equal speed V over

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wavelength Lambda substituting Lambda

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equals 4 L

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so F equal 0.25 V / l so B has the

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lowest

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frequency stationary wave of

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microwave an incident microwave

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traveling toward a metal reflector is

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reflected and travels in the opposite

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direction the incident and reflected

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waves have the same frequency wavelength

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and speed the superposition of the

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incident and reflected microwaves

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creates a stationary wave pattern with

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nodes and

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antinodes a detector measures the

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microwave signal intensity of

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microwave this detector can be used to

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locate the nodes and anten noes of this

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standing wave by moving the detector

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between the microwave source and the

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reflector the alternating points of

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minimum and maximum signal intensity can

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be observed the points of minimum signal

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intensity correspond to the nodes the

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points of Maximum signal intensity

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correspond to the ant noes the distance

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between successive nodes or antinodes is

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equal to half of a

23:44

wavelength exam style question six in an

23:48

experiment to demonstrate a stationary

23:50

wave two microwave transmitters emitting

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waves of wavelength for cmers are set

23:56

facing each other as shown a detector is

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moved along a straight line between the

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transmitters it detects positions of

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Maximum and minimum signal the detector

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is a distance D from the leftand

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transmitter assume that both

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transmitters are at antinodes of the

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stationary wave which row gives a value

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of D for a maximum and for a minimum at

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the maximum signals is the

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antinodes at the minimum signals is the

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nodes the the question given the

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wavelength of microwave is 4 cm so half

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of a wavelength is 2

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cm the distance between consecutive

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antinodes or nodes is 2

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cm and the distance between consecutive

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antinodes and nodes is 1

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cenm from the diagram shows that the

24:48

value of D for a maximum signals or

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antinodes occur to be 0 2 4 6 8 and so

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on which are even numbers the value of D

24:59

for minimum signals or nodes occur to be

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1 3 5 7 and so on which are odd numbers

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so the value of D for a maximum can be

25:09

46 and 48

25:12

CM the value of D for a minimum can be

25:15

47

25:16

CM so C is

25:23

correct difference between the

25:25

stationary wave and the progressive wave

25:28

the progressive wave can be transferred

25:30

the energy from one place to another the

25:33

progressive wave transfers the energy in

25:36

this direction the stationary wave

25:39

cannot be transferred the energy from

25:41

one place to

25:42

another however the energy is stored in

25:45

the vibrating particles like this all

25:48

the points along the progressive wave

25:50

have the same

25:51

amplitude these amplitude is the maximum

25:54

displacement that all point in wave can

25:56

be oscillated

25:58

the stationary wave has the amplitude of

26:00

different point to vary from a maximum

26:03

to zero the zero amplitude is at nodes

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the maximum amplitude is at

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antinodes all the points over one

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wavelength in Progressive wave have

26:14

different phases all the points between

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successive nodes are in phase for

26:20

example all points in same color section

26:23

her phase difference is zero all points

26:26

in pink and yellow region have phase

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difference equals

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360° which is also in Phase all points

26:35

in red and yellow regions have phase

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difference equals

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720° which is also in Phase all points

26:43

in blue and yellow regions have phase

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difference equals

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180° which is

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antiphase all points in green and yellow

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regions have phase difference equals

26:55

540° which is antiphase

27:01

exam style question seven which

27:04

statement concerning a stationary wave

27:07

is correct Choice a all the particles

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between two adjacent nodes oscillate in

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Phase this is correct Choice B the

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amplitude of the stationary wave is

27:19

equal to the amplitude of one of the

27:21

Waves creating it this is

27:24

incorrect the amplitude of a standing

27:27

wave varies from0 Z at the nodes to a

27:29

maximum which can be twice the amplitude

27:31

of the individual waves at the anten

27:34

noes Choice C the wavelength of the

27:37

stationary wave is equal to the

27:39

separation of two adjacent

27:41

nodes this is

27:43

incorrect the distance between two

27:45

adjacent nodes is half a

27:47

wavelength Choice D there is no

27:50

displacement of a particle at an

27:52

antinode at any time this is

27:55

incorrect at antinodes it's displacement

27:58

is maximum while no displacement at

28:07

[Music]

28:10

nodes hey everyone welcome to PL Academy

28:14

hope you found this video

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useful if you did it would be awesome if

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you could subscribe like the video share

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it with your friends and maybe drop a

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comment your support really helps me

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make more videos

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in this video I covered everything on

28:31

the syllabus like you can see in the

28:37

figure defraction of wave defraction is

28:42

the spreading out of a wave as it passes

28:44

through a narrow Gap aperture or around

28:46

an obstacle the amount of defraction

28:49

depends on the wavelength of the wave

28:51

compared with the size of the Gap

28:53

aperture or the size of the obstacle

28:56

when straight wave fronts in encounter a

28:58

gap or aperture in a barrier they pass

29:01

through and defract spreading out into

29:04

the region Beyond The Wave fronts curve

29:06

at the edges of the Gap while the

29:08

central portion remains relatively

29:11

straight this shown that these area are

29:14

diffracted this area is not

29:17

defract as the size Gap decreases to

29:20

approach the wavelength defraction

29:22

becomes more resulting in Greater

29:24

spreading and curvature of the wave

29:26

fronts as shown as the size Gap

29:29

decreases to very smaller than the

29:30

wavelength defraction increases

29:33

resulting in Greater spreading and

29:35

curvature of the wave fronts but the

29:37

defraction pattern may be become less

29:39

distinct as shown so we can conclude as

29:43

follows when the aperture is much larger

29:46

than the wavelength defraction is

29:48

minimal Little Wave forms curvature when

29:51

the aperture size is comparable to the

29:53

wavelength defraction increases greater

29:56

curvature of wave fronts

29:59

when the aperture is much smaller than

30:01

the wavelength defraction is significant

30:04

but the defraction pattern may become

30:06

less

30:11

distinct when a wave encounters an

30:13

obstacle defraction occurs around the

30:16

edges when straight wave fronts with a

30:19

wavelength much smaller than the width

30:21

of the obstacle defraction is minimal

30:23

resulting in slight curvature of the

30:25

wave fronts at the edges as shown

30:28

this creates a shadow region behind the

30:30

obstacle where the wave is blocked as

30:34

wavelength increases defraction

30:36

increases leading to Greater curvature

30:38

of the wave fronts at the edges as shown

30:42

this results in a less distinct or no

30:44

Shadow region behind the obstacle as the

30:47

wave bends around it when a sound wave

30:50

passes through a doorway the size of the

30:52

doorway is comparable to the wavelength

30:54

of the sound causing the defraction to

30:56

occur when light passes through a

30:59

doorway the size of the doorway is

31:01

typically much larger than the

31:03

wavelength of light resulting in no

31:10

defraction to investigate the defraction

31:13

of the visible light using a single slit

31:16

the slit width should be less than

31:18

approximately 10 power -4 M or 0.1

31:23

mm this is because the wavelength of

31:26

visible light ranges from about 10^ -6

31:29

to 10 power -7 M when monochromatic

31:33

light from a laser Source passes through

31:35

a single slit it diffracts as shown the

31:39

central Fringe of the defraction pattern

31:41

has the highest intensity and greatest

31:44

width decreasing the slit width

31:46

increases defraction leading to Greater

31:49

spreading of the light and a decrease in

31:51

intensity this increased defraction also

31:54

results in a wider Central Fringe the

31:58

defraction pattern of white light

32:00

through a single slit is shown the

32:02

central Fringe is white while the other

32:04

fringes display a spectrum of colors

32:07

with blue light closer to the center and

32:09

red light further away this occurs

32:12

because red light has a longer

32:14

wavelength than blue light and longer

32:16

wavelengths defract more spread out more

32:20

the defraction patterns of red green and

32:23

blue light through a single slit are

32:25

also shown the red lights Central Fringe

32:28

is the widest while the blue lights

32:30

Central Fringe is the

32:32

narrowest this is consistent with red

32:34

lights longer wavelength which causes

32:37

greater defraction than green or blue

32:43

light to investigate the defraction of

32:46

water waves using a single slit in a

32:48

ripple tank the wave fronts of waves are

32:51

generated using a vibrating bar and move

32:54

towards a gap in a barrier where the

32:57

Ripple stri strike the barrier they are

32:59

reflected back where they arrive at the

33:02

Gap however they pass through and spread

33:04

out into the space beyond it is this

33:07

spreading out of waves as they travel

33:09

through a gap or past the edge of a

33:12

barrier a ripple tank is a shallow tray

33:15

of water with a light source shining

33:17

down through it the light illuminates

33:19

the wave fronts making them visible a

33:23

straight Dipper can be used to create

33:25

straight wave fronts in a ripple tank

33:28

when the Dipper is vibrated up and down

33:30

it creates a series of parallel wave

33:32

fronts passing through a gap to observe

33:35

the defraction of the water wave on a

33:38

screen the stroboscope or video camera

33:41

is used to make the slow motion of the

33:43

wave fronts of water wave on the

33:49

screen exam style question one the speed

33:53

of sound in air is 330

33:56

m/s which size of architectural features

33:59

in a large Concert Hall would best

34:01

defract sound waves of frequency 0.44

34:05

khz the size of architecture features

34:08

should be comparable to wavelength of

34:10

the sound waves resulting in the best

34:13

defraction so we can calculate the

34:16

wavelength of the sound first using the

34:18

equation wavelength Lambda equals speed

34:21

V over frequency F substituting V equal

34:26

330 m/ second and f = 0.44 * 10^ 3 Hertz

34:33

we get the wavelength Lambda equal 0.75

34:37

m or 750

34:40

mm so the size of architecture features

34:43

should be 750

34:46

mm exam style question two in an

34:50

experiment water waves in a ripple tank

34:52

are incident on a gap as shown some

34:55

defraction of the water waves is

34:58

observed which change to the experiment

35:00

would provide a better demonstration of

35:03

defraction the best defraction occurs

35:06

when the size of Gap is comparable to

35:08

the

35:08

wavelength Choice a increase the

35:11

amplitude of the

35:12

Waves this is incorrect because the

35:15

amplitude does not affect

35:17

defraction Choice B increase the

35:20

frequency of the

35:21

Waves this is incorrect because

35:24

increasing the frequency decreases the

35:26

wavelength which would reduce

35:28

defraction Choice C increase the

35:30

wavelength of the Waves this is correct

35:34

because increasing the wavelength makes

35:36

it closer to the gap size leading to

35:38

more

35:39

defraction Choice D increase the width

35:42

of the Gap this is incorrect because

35:45

increasing the Gap width decreases the

35:47

amount of defraction

35:53

[Music]

35:57

hey everyone welcome to PL Academy hope

36:01

you found this video

36:02

useful if you did it would be awesome if

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you could subscribe like the video share

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it with your friends and maybe drop a

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comment your support really helps me

36:13

make more

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videos in this video I covered

36:17

everything on the syllabus like you can

36:19

see in the

36:24

figure interference of wave inter

36:27

interference occurs when two coherent

36:29

waves meet at a point they superpose

36:33

producing a pattern of nodes and

36:35

antinodes at the antinodes have the

36:37

phase differences to be 0er 2 pi 4 Pi 6

36:42

pi and so on or 0

36:46

360°

36:48

720° and so on and their patch

36:51

differences are zero Lambda 2 Lambda 3

36:54

Lambda and so on at the nodes have the

36:58

phase differences to be Pi 3 Pi 5 Pi 7

37:02

pi and so on or

37:05

180°

37:07

540° 900° and so on and their patch

37:12

differences are half a Lambda 3 half

37:14

Lambda 5 half Lambda and so on waves are

37:18

considered coherent when they satisfy

37:21

the following conditions they have a

37:23

constant phase

37:25

difference this is the most important

37:28

condition they are the same type of wave

37:31

they have the same frequency and

37:34

wavelength for example green and blue

37:37

waves are

37:38

coherent this is because both waves

37:40

maintain a constant phase difference of

37:43

180° and they have the same frequency

37:46

and

37:47

wavelength their amplitude are not equal

37:50

but do not affect

37:51

coherence pink and blue waves are

37:54

coherent this is because both waves

37:56

maintain a constant phase difference of

37:59

90° and they have the same frequency and

38:02

wavelength their amplitude are not equal

38:05

but do not affect

38:07

coherence red and green waves are not

38:10

coherent this is because they do not

38:12

maintain a constant phase difference and

38:15

do not have the same frequency or

38:22

wavelength to investigate the

38:24

interference of water waves in the

38:25

Ripple tank two Dippers connected to the

38:29

same oscillator vibrate with the same

38:31

frequency generating two coherent water

38:34

waves when the bar vibrates each Dipper

38:38

acts as a source of circular ripples

38:40

spreading

38:41

outwards where these sets of ripples

38:43

overlap an interference pattern is

38:45

projected onto the screen below this

38:48

interference pattern is visible on the

38:51

screen the pattern consists of

38:53

alternating regions of constructive and

38:56

destructive interference

38:58

along this line are locations of

39:00

destructive interference resulting in

39:03

nodes along this line are locations of

39:06

constructive interference resulting in

39:09

antinodes along this line are locations

39:12

of destructive interference resulting in

39:15

nodes along this line are locations of

39:18

constructive interference resulting in

39:21

antinodes along this line are locations

39:23

of destructive interference resulting in

39:26

nodes

39:27

along this line are locations of

39:29

constructive interference resulting in

39:33

antinodes along this line are locations

39:35

of destructive interference resulting in

39:38

nodes another way to observe

39:41

interference in a ripple tank is to use

39:43

plain waves passing through two gaps in

39:45

a barrier the water waves are defract at

39:49

the gaps and then interfere Beyond

39:51

creating a similar pattern

39:57

the interference pattern in the Ripple

39:59

tank two sources S1 and S2 produce

40:03

coherent waves with a phase difference

40:05

of zero the waves have the same

40:08

wavelength Lambda given the red line

40:11

represents the crest and green line

40:13

represents the trough along the yellow

40:16

lines are locations of constructive

40:18

interference resulting in

40:21

antinodes these points are formed the

40:23

superposition of wave crests with crests

40:26

or wave trough with troughs along this

40:29

black lines are locations of destructive

40:32

interference resulting in

40:34

nodes these points are formed the

40:36

superposition of wave crests with

40:39

troughs recall that at the nodes have

40:41

the phase differences to be Pi 3 Pi 5 Pi

40:45

7 pi and so on or

40:49

180°

40:51

540° 900° and so on and their patch

40:56

differences are half Lambda 3 half

40:58

Lambda 5 half Lambda and so on at the

41:02

antinodes have the phase differences to

41:04

be zero 2 pi 4 Pi 6 pi and so on or zero

41:11

360°

41:13

720° and so on and their patch

41:16

differences are zero Lambda 2 Lambda 3

41:20

Lambda and so on the difference in

41:23

distance from any point along black and

41:25

yellow lines to sources S1 and S2

41:28

respectively is the path difference for

41:30

that line the central yellow line marks

41:34

the zero order antinode

41:36

a0 at this antinode both the path

41:39

difference and the phase difference are

41:41

zero this means that the distance from

41:44

any point on this line to the two

41:46

sources S1 and S2 is equal for example

41:50

at point a on this line the distance S1

41:53

to a is 5 Lambda and the distance S2 to

41:56

a is also 5 Lambda at the left next

42:00

black line marks the first order node

42:03

N1 at this node the path difference is

42:06

half a wavelength and the phase

42:08

difference are

42:10

180° this means that the difference in

42:12

distance from any point on this line to

42:15

the two sources S1 and S2 is half a

42:19

wavelength for example at point B on

42:21

this line the distance S1 to B is 5

42:24

Lambda and the distance S2 to B is also

42:27

5.5 Lambda at the next yellow line marks

42:31

the first order anode

42:33

A1 at this anode the path difference is

42:37

one wavelength and the phase difference

42:39

are

42:41

360° this means that the difference in

42:43

distance from any point on this line to

42:45

the two sources S1 and S2 is one

42:49

wavelength for example at Point C on

42:52

this line the distance S1 to C is 4.5

42:56

Lambda and the distance S2 to C is also

42:59

5.5 Lambda at the next black line marks

43:03

the second order node

43:04

N2 at this node the path difference is

43:08

three half wavelength and the phase

43:10

difference are

43:12

540° this means that the difference in

43:15

distance from any point on this line to

43:17

the two sources S1 and S2 is three half

43:21

wavelength for example at Point D on

43:24

this line the distance S1 to D is 3

43:26

Lambda and the distance S 2 to D is also

43:29

4.5 Lambda at the next yellow line marks

43:33

the second order antinode

43:35

A2 at this antinode the path difference

43:39

is two wavelength and the phase

43:41

difference are

43:43

720° this means that the difference in

43:45

distance from any point on this line to

43:48

the two sources S1 and S2 is two

43:51

wavelength for example at Point e on

43:54

this line the distance S1 to e is 4

43:57

Lambda and the distance S 2 to e is also

44:00

6 Lambda at the next black line marks

44:03

the third order node

44:05

N3 at this node the path difference is

44:08

five half wavelength and the phase

44:10

difference are

44:12

900° this means that the difference in

44:15

distance from any point on this line to

44:17

the two sources S1 and S2 is five half

44:20

wve length for example at Point F on

44:24

this line the distance S1 to F is 3 l

44:27

Lambda and the distance S2 to F is also

44:30

5.5 Lambda at the next yellow line marks

44:34

the third order antinode

44:36

A3 at this anode the path difference is

44:39

three wavelength and the phase

44:41

difference are 1,

44:44

180° this means that the difference in

44:46

distance from any point on this line to

44:48

the two sources S1 and S2 is three

44:52

wavelength for example at Point G on

44:55

this line the distance S1 1 to G is 2.5

44:58

Lambda and the distance S2 to G is also

45:01

5.5 Lambda this pattern is symmetric

45:05

about the central yellow line like

45:11

this exam style question one two sources

45:16

of microwaves p and Q produce coherent

45:19

waves with a phase difference of

45:22

180° the waves have the same wavelength

45:25

Lambda and at the point s there is a

45:28

minimum in the interference pattern

45:30

produced by waves from the two sources

45:33

the distance Qs minus PS is called the

45:36

path difference which expression could

45:39

represent the path difference at the

45:42

initial the waves from sources p and Q

45:45

have phase difference of

45:47

180° so the path difference between two

45:50

waves is half a

45:52

wavelength the path difference for

45:54

minimum interferences at Point s can be

45:56

one half Lambda 3 halfes Lambda 5 Hales

46:00

Lambda and so on the half Lambda path

46:03

difference from the sources adds to any

46:05

path difference to determine the overall

46:07

path difference at Point s Choice a the

46:11

overall path difference = 1/4 Lambda +

46:15

12 Lambda = 3/4 Lambda this is

46:19

incorrect Choice B the overall path

46:22

difference equal 1 12 Lambda + 1 12

46:25

Lambda = 1 lamb Lambda this is

46:29

incorrect Choice C the overall path

46:32

difference equals 1 Lambda + 1 12 Lambda

46:35

equal 3es Lambda this is correct Choice

46:40

D the overall path difference equals 3es

46:43

Lambda + 1 12 Lambda = 2 Lambda this is

46:48

incorrect exam style question two an

46:52

outdoor concert has two large speakers

46:55

beside the stage for broadcasting

46:57

music in order to test the speakers they

47:00

are made to emit sound of the same

47:02

wavelength and the same

47:04

amplitude the curved lines in the

47:06

diagram represent wave fronts where is

47:09

the loudest sound heard the wave fronts

47:12

connect points of equal phase in the

47:14

sound wave such as

47:16

compressions the loudest sound occurs

47:19

where constructive interference takes

47:21

place constructive interference happens

47:24

when compressions from both speakers

47:26

overlap or when rare factions from both

47:29

speakers

47:30

overlap this occurs where the wave

47:32

fronts from the two speakers

47:34

intersect so D is

47:40

correct investigating the interference

47:43

of sound waves two identical

47:46

loudspeakers connected to a single

47:48

generator produce coherent sound waves

47:51

with a phase difference of zero as a

47:54

microphone is moved along line AB in

47:56

front of the loudspeakers a series of

47:59

alternating loud and quiet regions is

48:02

observed at the loud regions

48:04

constructive interference occurs

48:07

resulting in a sound intensity that is

48:09

twice that of a single

48:11

loudspeaker these regions are called

48:14

antinodes at the quiet regions

48:16

destructive interference occurs

48:18

resulting in a sound intensity that is

48:20

lower than that of a single

48:22

loudspeaker these regions are called

48:25

nodes the the central loud region marks

48:28

the zero order

48:30

antinode at this antinode both the path

48:33

difference and the phase difference are

48:35

zero at the next quiet region marks the

48:38

first order node at this node the path

48:41

difference is half a wavelength and the

48:44

phase difference are Pi

48:45

radians at the next loud region marks

48:48

the first order

48:50

antinode at this antinode the path

48:53

difference is one wavelength and the

48:55

phase difference are 2 pi radi Ian at

48:58

the next quiet region marks the second

49:00

order node at this node the path

49:03

difference is three half wavelength and

49:05

the phase difference are 3 Pi

49:08

radians this pattern is symmetric about

49:10

the central quiet like this the graph

49:14

shows the variation of sound intensity

49:16

detected by the microphone with distance

49:18

from point A as displayed on the

49:21

C the intensity at nodes may not be

49:25

exactly zero due to the presence of

49:27

background

49:32

noise exam style question three two

49:36

loudspeakers are placed near to each

49:38

other and facing in the same direction a

49:41

microphone connected to an oscilloscope

49:44

is moved along a line some distance away

49:46

from the loudspeakers as shown which

49:49

statement about the waves emitted by the

49:51

loudspeakers is not a necessary

49:53

condition for the microphone to detect a

49:56

fixed point along the line where there

49:58

is no sound Choice a the waves must be

50:01

emitted in Phase this is not a necessary

50:05

because the interference can be occurred

50:07

if the waves emitted in out of phase

50:10

Choice B the waves must be emitted with

50:12

a similar

50:14

amplitude this is a necessary because we

50:16

need to detect where no sound which

50:18

means that completely destructive

50:21

interference Choice C the waves must

50:24

have the same

50:25

frequency this is necessary because it

50:28

is condition of coherent waves Choice D

50:31

the waves must have the same

50:33

wavelength this is necessary because it

50:36

is condition of coherent

50:42

waves investigating the interference of

50:45

light waves a white light source is used

50:49

rather than a laser a monochromatic

50:51

filter allows only one wavelength of

50:54

light to pass through a single slit

50:57

diffracts the light this defract light

51:00

arrives in phase at the double slit

51:02

which ensures that the two parts of the

51:04

double slit behave as coherent sources

51:06

of light the double slit is placed a

51:09

centimeter or two beyond the single slit

51:12

acts as two coherent sources the

51:15

interference pattern is observed on a

51:17

screen about a meter away the bright

51:20

fringes have equal intensity and are

51:23

equally fringes separation as shown the

51:26

experiment has to be carried out in a

51:28

darkened room as the intensity of the

51:31

light is low and the fringes are hard to

51:33

see when a red filter is used a

51:36

interference pattern is shown when a

51:39

green filter is used a interference

51:42

pattern is shown showing that the Fringe

51:44

separation is smaller than with red

51:46

light when a blue filter is used a

51:50

interference pattern is shown showing

51:52

that the Fringe separation is smaller

51:54

than with green light when no filter the

51:58

interference pattern of white light is

52:00

shown this pattern shows a spectrum

52:03

cooler with blue light fringes closer to

52:05

the center and red light fringes further

52:08

away this is because red light has a

52:10

longer wavelength than blue light and

52:13

longer wavelengths defract more spread

52:15

out more three key factors influence the

52:19

experimental setup slit width slit

52:22

widths are typically a fraction of a

52:25

millimeter since visible light

52:27

wavelengths are much smaller minimal

52:29

defraction occurs allowing for

52:31

sufficient light intensity to observe

52:34

fringes narrower slits would

52:36

significantly reduce light intensity

52:39

slit separation double slits are usually

52:42

separated by about a

52:44

millimeter larger separations would

52:46

result in closely spaced fringes making

52:49

them difficult to

52:50

distinguish screen distance the screen

52:53

is placed approximately 1 M from the

52:56

slits

52:57

this distance provides clearly separated

52:59

fringes without excessive dimming of the

53:06

light exam style question four light of

53:10

wavelength Lambda is incident normally

53:13

on two narrow slits S1 and S2 a small

53:16

distance apart bright and dark fringes

53:19

are observed on a screen a long distance

53:21

away from the slits the N dark Fringe

53:24

from the central bright Fringe is

53:26

observed at Point p on the screen which

53:29

equation is correct for all positive

53:31

values of n all positive values of n

53:35

equal 1 2 3 4 and so on the dark fringes

53:40

occur where destructive interference

53:42

take place which happens when the path

53:44

differences are 1 half Lambda 3 Hal

53:47

Lambda 5 Hales Lambda and so on Choice a

53:51

the path differences are 1 half Lambda

53:54

Lambda 3es Lambda and and so on this is

53:59

incorrect Choice B the path differences

54:01

are Lambda 2 Lambda 3 Lambda and so on

54:06

this is

54:07

incorrect Choice C the path differences

54:10

are 1 half Lambda 3 half Lambda 5 Hales

54:14

Lambda and so on this is correct Choice

54:18

D the path differences are three halfes

54:21

Lambda 5 Hales Lambda 7 Hales Lambda and

54:24

so on this is

54:31

incorrect Young's double slit experiment

54:34

a laser produces intense coherent light

54:38

as the light passes through the double

54:40

slits it is diffracted spreading out

54:43

into the space beyond this creates two

54:46

overlapping sets of waves and an

54:48

interference pattern is observed on a

54:51

screen placed about a meter away we will

54:54

focus on the interference pattern with

54:56

within this specific region within this

54:59

region the bright fringes exhibit equal

55:01

intensity and consistent Fringe

55:03

separation as shown the double slit

55:06

experiment can be used to determine the

55:08

wavelength Lambda of light the following

55:12

three quantities have to be measured

55:14

slit separation a in meters Fringe

55:18

separation X in meters this is the

55:21

distance between the centers of adjacent

55:23

bright or dark fringes s flip to screen

55:27

distance D in meters the formula for

55:30

calculating the wavelength is Lambda

55:33

equals ax / D this formula can explain

55:38

why the Fringe separation for red light

55:40

is greater than that for green and blue

55:42

light as shown in the diagram given a

55:46

constant slit separation a and slit to

55:48

screen distance D the wavelength Lambda

55:51

is directly proportional to The Fringe

55:53

separation X since red light has the

55:57

longest wavelength The Fringe separation

55:59

X for red light is greatest blue light

56:03

with the shortest wavelength exhibits

56:06

the smallest Fringe

56:11

separation exam style question five a

56:15

double slit interference experiment is

56:17

set up as shown fringes are formed on

56:20

the screen the distance between

56:23

successive bright fringes is found to be

56:25

4 m

56:26

M given the wavelength of red light

56:29

equals Lambda the slit separation equals

56:32

a the slit to screen distance equals D

56:35

and Fringe separation x = 4 mm as shown

56:39

in the diagram two changes are then made

56:42

to the experimental

56:43

Arrangement the double slit is replaced

56:46

by another double slit which has half

56:48

the spacing the screen is moved so that

56:51

its distance from the double slit is

56:53

twice as great what is now the distance

56:56

between successive bright

56:58

fringes from the equation Lambda equal

57:01

ax / D rearranging the equation as xal

57:07

Lambda D / a from the diagram the old

57:11

Fringe separation x = 4

57:14

mm substituting new D = 2D and new a = a

57:19

/ 2 so mux = 4 Lambda D / a substitute

57:26

Lambda d/ a = 4

57:29

mm so newx = 16

57:36

mm exam style question six the diagram

57:41

shows an arrangement for demonstrating

57:43

two Source interference using coherent

57:46

light of a single wavelength Lambda an

57:49

interference pattern is observed on a

57:51

screen 3.0 M away from the slits X and Y

57:55

which have a separation of 1.0

57:58

mm the central bright Fringe is at Q and

58:02

the second bright Fringe from the center

58:04

is at P what is the distance between q

58:07

and P the distance PQ equals

58:11

2x from the equation Lambda equal ax / D

58:17

rearranging the equation as xal Lambda D

58:20

/ a substituting D equal 3 m and a = 1.0

58:27

* 10^ -3 M we get The Fringe separation

58:32

x = 3 * 10^ 3 Lambda so 2x = 6 * 10^ 3

58:46

[Music]

58:49

Lambda hey everyone welcome to PL

58:53

Academy hope you found this video useful

58:57

if you did it would be awesome if you

58:59

could subscribe like the video share it

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with your friends and maybe drop a

59:04

comment your support really helps me

59:06

make more videos in this video I covered

59:10

everything on the syllabus like you can

59:12

see in the

59:17

figure defraction grating a defraction

59:21

grating consists of a large number of

59:23

equally spaced lines ruled onto a glass

59:26

or plastic slide each line acts as a

59:29

source of defraction for the incident

59:31

light the gratings can have up to 10,000

59:35

lines per

59:36

cimer when light passes through the

59:38

grating an interference pattern of

59:41

fringes is

59:42

observed in the diagram monochromatic

59:45

light from a laser is incident normally

59:47

on a transmission defraction grating

59:50

beyond the grating interference fringes

59:53

are formed and can be observed on a

59:55

screen Sim similar to the double slit

59:57

experiment the fringes are also referred

60:00

to as Maxima the central Fringe is

60:03

called the zeroth order maximum

60:06

a0 the next Fringe is the first order

60:09

maximum

60:10

A1 the next Fringe is the second order

60:13

maximum A2 and so on the pattern is

60:16

symmetrical so there are two first order

60:19

Maxima A1 2 second order Maxima A2 and

60:23

so on as shown to analyze the pattern we

60:26

measure the angles Theta and beta at

60:29

which the Maxima are formed rather than

60:31

measuring their

60:32

separation with double slits the fringes

60:35

are equally spaced and the angles are

60:37

very small with a defraction grating the

60:41

angles are much greater and the fringes

60:43

are not equally

60:48

spaced the differences in the

60:50

interference patterns between defraction

60:53

gratings and double slits are as follows

60:56

brighter and sharper fringes defraction

60:59

gratings typically produce brighter and

61:01

sharper fringes than double slits

61:03

because more light passes through the

61:05

numerous slits in the grating larger

61:08

Fringe separation defraction gratings

61:11

generally exhibit larger Fringe

61:13

separations than double slits because

61:15

the slit spacing in gratings is much

61:18

smaller than the slit separation in

61:20

typical double slit

61:21

experiments the wavelength Lambda can be

61:24

determined with a defraction grating by

61:27

measuring the angles at which the Maxima

61:29

occur we can determine the wavelength of

61:31

the incident light and calculating using

61:34

the equation D sin theta equals n Lambda

61:39

where D is the grating spacing in meters

61:42

Theta is the angle between the zero

61:44

order maximum and N order maximum n is

61:47

the order of Maximum as 1 2 3 and so on

61:50

and Lambda is the wavelength of light in

61:53

meters if the grating has K line per

61:56

meter then the grating spacing D can be

61:58

calculated using d = 1 /

62:07

K exam style question one a beam of red

62:11

laser light of wavelength 633 nanom is

62:16

incident normally on a defraction

62:18

grating with 600 lines per

62:21

millimet the beam of red light is now

62:23

replaced by a beam of blue laser light

62:26

of wavelength

62:27

445

62:29

nanom a replacement defraction grating

62:32

is used so that the first order maximum

62:34

of the blue light appears at the same

62:36

position on the screen as the first

62:38

order maximum of the red light from the

62:41

original

62:41

laser this means that the angle Theta is

62:45

the same for both and the first order

62:47

corresponds n equal 1 how many lines per

62:51

millimeter are there in the replacement

62:53

defraction grating using the equation D

62:56

sin Theta equal n Lambda for the blue

63:00

light and the replacement grating we

63:02

have D2 sin Theta = 1 time blue Lambda

63:06

for the red light and the original

63:08

grating we have D1 sin Theta = 1 * red

63:13

Lambda dividing the first equation by

63:15

the second equation we get D2 sin Theta

63:20

over D1 sin Theta equal blue Lambda over

63:23

red Lambda so sin Theta is the same for

63:27

both it cancels out leaving D2 / D1

63:31

equal blue Lambda over red Lambda

63:35

substituting blue Lambda 445 nanom and

63:39

red Lambda equal

63:41

633

63:43

nanom the nanometers cancel out so we

63:47

get D2 =

63:50

445 over 633 *

63:53

D1 substituting D2 = 1 / K2 and D1 = 1 /

64:00

K1 where K2 and K1 are the number of

64:04

line per millimeters for the replacement

64:06

and original gratings

64:08

respectively substituting K1 equals 600

64:12

per

64:13

MIM we solve K2 = 850 per millim for two

64:18

significant

64:23

figures exam style question question two

64:27

monochromatic light of wavelength 690

64:30

nanom passes through a defraction

64:33

grating with 300 lines per millimet

64:36

producing a series of Maxima bright

64:38

spots on a screen what is the greatest

64:41

number of Maxima that can be observed

64:44

the defraction grating with 300 lines

64:47

per millimet so grating spacing D equals

64:50

1 over 300 mm or 1 over 300 * 10 power

64:56

-3

64:57

M using the equation D sin Theta equal n

65:01

Lambda substituting d = 1 300 power -3 M

65:07

Theta = 90° and Lambda = 690 * 10^ -9

65:15

M we solve for n order Maxima equal

65:18

4.83 but n must be a whole numbers so

65:21

the maximum order is four so the

65:25

greatest number number of Maxima that

65:26

can be observed is 4 + 1 + 4 is equal to

65:30

9 Maxima which includes the zeroth order

65:33

maximum and four Maxima on left and

65:36

right hand sides as shown we substitute

65:39

the angle theta equals 90° because this

65:43

represents the maximum possible angle

65:45

from the zero order maximum to the

65:47

highest order

65:52

maximum I hope you found this video

65:55

helpful

65:56

if you did I would be grateful if you

65:59

would subscribe share like and leave a

66:01

positive comment your support will

66:04

encourage me to create more

66:06

content thank you

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