standing waves resonance. standing waves in strings an incident wave undergoes fixed end reflection...

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Standing Waves Resonance

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Page 1: Standing Waves Resonance. Standing waves in Strings An incident wave undergoes fixed end reflection Standing waves produce nodes where the amplitude is

Standing WavesResonance

Page 2: Standing Waves Resonance. Standing waves in Strings An incident wave undergoes fixed end reflection Standing waves produce nodes where the amplitude is

Standing waves in Strings

• An incident wave undergoes fixed end reflection

• Standing waves produce nodes where the amplitude is zero

• Interference produces a wave that appears stationary with nodes and antinodes

Page 3: Standing Waves Resonance. Standing waves in Strings An incident wave undergoes fixed end reflection Standing waves produce nodes where the amplitude is

Standing waves in Strings• A symmetrical patern is stationary if:

– Frequency doesn’t change– Distance between the two ends is

constant• If the frequency increases, the

wavelength decreases so nodes get closer together.

• At certain frequencies (determined by the length of the medium) standing waves can set up to create antinodes (max amplitude) and nodes.

• Earthquakes in buildings achieve maximum destruction if a standing wave exists in the building!!

Page 4: Standing Waves Resonance. Standing waves in Strings An incident wave undergoes fixed end reflection Standing waves produce nodes where the amplitude is

Standing waves in Strings

• The 1st harmonic satisfies L = ½ λ with L as the string length

• At the fixed ends, there are always nodes

• The number of antinodes matches the harmonic number

• ƒo

Page 5: Standing Waves Resonance. Standing waves in Strings An incident wave undergoes fixed end reflection Standing waves produce nodes where the amplitude is

Standing waves in Strings

• The 2nd harmonic satisfies L = λ • There are 3 nodes and 2 antinodes• This is also called the 1st overtone

(1 above the fundamental frequency)

• 2ƒo

Page 6: Standing Waves Resonance. Standing waves in Strings An incident wave undergoes fixed end reflection Standing waves produce nodes where the amplitude is

Standing waves in Strings

• The 3rd harmonic satisfies L = (3/2) λ • There are 4 nodes and 3 antinodes• This is also called the 2nd overtone (2

above the fundamental frequency)• 3ƒo

Page 7: Standing Waves Resonance. Standing waves in Strings An incident wave undergoes fixed end reflection Standing waves produce nodes where the amplitude is

Standing waves in Strings

• 1st harmonic• Fundamental

frequency (ƒo)

• 2nd harmonic • 1st overtone• 2ƒo

• 3rd harmonic

• 2nd overtone• 3ƒo

Page 8: Standing Waves Resonance. Standing waves in Strings An incident wave undergoes fixed end reflection Standing waves produce nodes where the amplitude is

Standing waves in Strings

•Nodes are always ½ λ apart•The general formula can be derived:

•n = 1, 2, 3…the harmonic number•This same relationship applies to open end air columns (like with woodwind instruments)

2

nL

Page 9: Standing Waves Resonance. Standing waves in Strings An incident wave undergoes fixed end reflection Standing waves produce nodes where the amplitude is

Closed End Air Columns• A tube filled with water can be slowly

drained out while holding a tuning fork vibrating over th open end.

• At certain air column lengths, standing waves will be set up (with an anti-node at the top) and a loud sound is heard at this resonance point.

• Fixed end reflection of the sound occurs from the water surface

• Resonances occur at multiples of the wavelength at specific lengths.

Page 10: Standing Waves Resonance. Standing waves in Strings An incident wave undergoes fixed end reflection Standing waves produce nodes where the amplitude is

Closed End Air Columns

• 1st harmonic• L = ¼λ• ƒo• 2nd harmonic• L = ¾λ • 2ƒo• 3rd harmonic• L = 1¼ λ • 3ƒo

Page 11: Standing Waves Resonance. Standing waves in Strings An incident wave undergoes fixed end reflection Standing waves produce nodes where the amplitude is

Open End Air Columns

• Reflection with open tubes occurs due to pressure differences (air below tube is free to move) allowing open end reflection.

• Standing waves occur with the same geometry as waves in strings.

• Note: we use transverse waves to MODEL how sound behaves but really the patternd are more complicated to draw with longitudinal waves!!

Page 12: Standing Waves Resonance. Standing waves in Strings An incident wave undergoes fixed end reflection Standing waves produce nodes where the amplitude is

Open End Air Columns• 1st harmonic• ƒo

• 2nd harmonic• 1st overtone• 2ƒo

• 3rd harmonic• 2nd overtone• 3ƒo

Page 13: Standing Waves Resonance. Standing waves in Strings An incident wave undergoes fixed end reflection Standing waves produce nodes where the amplitude is

Closed End Air Columns

• General Formula:

• n = harmonic number: 1, 2, 3. etc

4

)12(

nL

Page 14: Standing Waves Resonance. Standing waves in Strings An incident wave undergoes fixed end reflection Standing waves produce nodes where the amplitude is

QuestionsEx 1) The first resonant length of a

closed air column occurs when the length is 18 cm.

a) What is the wavelength of the sound?

b) What is the speed of sound if a 512 Hz source is used?

a) First resonance occurs: L = ¼ λ = 18 cm.

λ = 72 cmb) v = f λ

= 512 Hz (0.72 m)= 3.7 x 102 m/s

Page 15: Standing Waves Resonance. Standing waves in Strings An incident wave undergoes fixed end reflection Standing waves produce nodes where the amplitude is

QuestionsEx 1) A tuning fork is held over a

column filled with water. When the water is drained, the first resonance is heard at an air column length of 9.0 cm.

a) What is the wavelength of the tuning fork?

b) What is the air column length for the 2nd resonance?

c) Find the frequency of the tuning fork if it’s 20.0oC.

Page 16: Standing Waves Resonance. Standing waves in Strings An incident wave undergoes fixed end reflection Standing waves produce nodes where the amplitude is

Questions

a) First resonance occurs: L = ¼ λ = 9.0 cm.

λ = 36 cmb) L2 = ¾ λ = ¾ (36 cm)

= 27 cmc) v=f λ

332 m/s + 0.6 m/s/oC(T) = f(0.36 m)F = 9.6 x 102 Hz

Page 17: Standing Waves Resonance. Standing waves in Strings An incident wave undergoes fixed end reflection Standing waves produce nodes where the amplitude is

Questions• A 500. Hz tuning forl is used to

determine the resonances in an adjustable air column of air at both ends. The length of the air column changes by 33.4 cm between resonant sounds.

a) Find the wavelength of the sound wave.

b) Find the speed of sound.c) Determine the air temperature.

Answers: 66.8 cm, 334 m/s, 3.33oC

Page 18: Standing Waves Resonance. Standing waves in Strings An incident wave undergoes fixed end reflection Standing waves produce nodes where the amplitude is

Questions• Solution:a) Resonances occur ½ λ apart.

1/2 λ = 33.4 cmλ = 66.8 cm

b) v = f λv = 500 Hz (0.668 m)

= 334 m/sc) v = 332 m/s + 0.6 m/s/oC (T)

334 m/s = 332 m/s + 0.6 m/s/oC (T)T = 3.33oC