standing waves 1 part 1: strings (transverse standing waves) 05/03/08

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Standing Waves 1 Part 1: Strings (Transverse Standing Waves) 05/03/08

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Page 1: Standing Waves 1 Part 1: Strings (Transverse Standing Waves) 05/03/08

Standing Waves 1

Part 1: Strings (Transverse Standing Waves)

05/03/08

Page 2: Standing Waves 1 Part 1: Strings (Transverse Standing Waves) 05/03/08

Standing Waves

A standing (or stationary) wave occurs when two waves of the same frequency pass through each other in opposite directions.

Page 3: Standing Waves 1 Part 1: Strings (Transverse Standing Waves) 05/03/08

Formation of a Standing Wave

Page 4: Standing Waves 1 Part 1: Strings (Transverse Standing Waves) 05/03/08

Waves Travelling in Opposite Directions: The diagram shows

two waves (in green and blue) travelling in opposite directions on a string, setting up a standing wave (in black).

Note that the standing wave is the sum of the two travelling waves.

Page 5: Standing Waves 1 Part 1: Strings (Transverse Standing Waves) 05/03/08

Energy in a Standing Wave

No energy is transferred by a standing wave.

Energy is trapped in the wave, changing between kinetic and potential energy as particles vibrate back and forth.

Standing waves is a resonance effect, because the superposition of the two waves of identical frequency results in an increased amplitude of oscillation.

Page 6: Standing Waves 1 Part 1: Strings (Transverse Standing Waves) 05/03/08

Properties II Nodes are points on the standing wave

that remain stationary at all times. Antinodes are points on the standing

wave that have the greatest displacement.

Page 7: Standing Waves 1 Part 1: Strings (Transverse Standing Waves) 05/03/08

Harmonics in a String The 1st harmonic in a

string has a wavelength of twice the length of the string.

The 2nd harmonic has a wavelength equal to the length of the string.

The 3rd harmonic has a wavelength equal to 2/3 the length of the string.

Page 8: Standing Waves 1 Part 1: Strings (Transverse Standing Waves) 05/03/08

Problem 1:Telephone wires often resonate and hum in high

winds. When the wind blows in a particular direction, some wires are heard to resonate at 50 Hz. The telephone poles are 25 m apart.

Sketch such a telephone wire vibrating at its fundamental frequency.

Calculate the wavelength of the fundamental. [50 m]

Calculate the wave speed. [2500 ms-1]

Sketch the wave pattern of the second harmonic.

Page 9: Standing Waves 1 Part 1: Strings (Transverse Standing Waves) 05/03/08

Problem 2:A guitar string is 75.0 cm long. It is made to vibrate at its

fundamental frequency.

What is the wavelength of the vibration? [1.50 m] The frequency of the note is 465 Hz. Calculate the speed

of the wave in the guitar string.[698 m s-1]

What is the frequency of the third harmonic? [1395 Hz] Calculate the wavelength of the third harmonic.

[0.50 m] The string is shortened to 35.0 cm as the player’s fingers

move down the fret board. Calculate the new fundamental frequency.

[996 Hz]

Page 10: Standing Waves 1 Part 1: Strings (Transverse Standing Waves) 05/03/08

Demonstrations Slinky – transverse waves

Guitar – identify the first, second, third, fourth harmonics by forcing nodes.

Page 11: Standing Waves 1 Part 1: Strings (Transverse Standing Waves) 05/03/08

Standing Waves

Part 2: Pipes(Longitudinal Standing Waves)

Page 12: Standing Waves 1 Part 1: Strings (Transverse Standing Waves) 05/03/08

Longitudinal Standing Waves When we blow across a bottle, we set up a

standing wave that is at the natural frequency of the bottle.

If we add water to the bottle, we have reduced the amount of space available for the wave to be set up in. The wavelength of the fundamental is also reduced.

Page 13: Standing Waves 1 Part 1: Strings (Transverse Standing Waves) 05/03/08

Longitudinal Waves A column of air inside a pipe can vibrate –

these vibrations are longitudinal: they behaves like compressions in a spring.

Page 14: Standing Waves 1 Part 1: Strings (Transverse Standing Waves) 05/03/08

Open and Closed Pipes As demonstrated in the diagram below, the

closed end of a pipe acts much like the fixed point of a string – here a node forms.

The open end of a pipe, however, forms an antinode.

Page 15: Standing Waves 1 Part 1: Strings (Transverse Standing Waves) 05/03/08

Problem 3An organ pipe is closed at one end and open at the other.

Sketch the wave pattern of the fundamental resonance inside the pipe.

The pipe is tuned to 50.0 Hz for its fundamental note. Calculate the wavelength of this note, given that the speed of sound is 320 m s-1.

[6.4 m] Calculate the length of the organ pipe.

[1.6 m] Sketch the wave pattern when the third harmonic is set

up in the pipe. Calculate the frequency of the third harmonic.

[150 Hz]

Page 16: Standing Waves 1 Part 1: Strings (Transverse Standing Waves) 05/03/08

Problem 2Some physics students use a speaker (loudspeaker) to

resonate a pipe that is open at both ends. The pipe is 1.20 m long.

Calculate the wavelength of the fundamental resonance.

[2.40 m] One end of the pipe is now closed off. Does the speaker

need to be changed to a higher or lower pitch in order to re-tune the pipe to the new fundamental? Explain.

Assuming that the speed of sound is 320 m s-1, calculate the new resonant frequency.

[67 Hz]

Page 17: Standing Waves 1 Part 1: Strings (Transverse Standing Waves) 05/03/08

Practice Complete problems 1, 3, 4, 5 Complete worksheet 3 on standing waves.