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Resonance October 23, 2014 Leading Off… Don’t forget: Korean stops homework is due on Tuesday! Also new: mystery spectrograms! Today: Resonance Before.

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Presentation on theme: "Resonance October 23, 2014 Leading Off… Don’t forget: Korean stops homework is due on Tuesday! Also new: mystery spectrograms! Today: Resonance Before."— Presentation transcript:

1

2 Resonance October 23, 2014

3 Leading Off… Don’t forget: Korean stops homework is due on Tuesday! Also new: mystery spectrograms! Today: Resonance Before we get into that: dogs talking! And cats, too!

4 The Source The complex wave emitted from the glottis during voicing= The source of all voiced speech sounds. In speech (particularly in vowels), humans can shape this spectrum to make distinctive sounds. Some harmonics may be emphasized... Others may be diminished (damped) Different spectral shapes may be formed by particular articulatory configurations....but the process of spectral shaping requires the raw stuff of the source to work with.

5 Spectral Shaping Examples Certain spectral shapes seem to have particular vowel qualities.

6 Spectrograms A spectrogram represents: Time on the x-axis Frequency on the y-axis Intensity on the z-axis

7 Real Vowels

8 Ch-ch-ch-ch-changes Check out some spectrograms of sinewaves which change frequency over time:

9 The Whole Thing What happens when we put all three together? This is an example of sinewave speech.

10 The Real Thing Spectral change over time is the defining characteristic of speech sounds.  It is crucial to understand spectrographic representations for the acoustic analysis of speech.

11 Life’s Persistent Questions How do we get from here: To here? Answer: Fourier Analysis

12 Skipping Ahead! Shorter analysis windows give us: Better temporal resolution Worse frequency resolution = wide-band spectrograms Longer analysis windows give us: Better frequency resolution Worse temporal resolution = narrow-band spectrograms Higher sampling rates give us... A higher limit on frequencies to consider.

13 “Band”? Way back when, we discussed low-pass filters: This filter passes frequencies below 250 Hz. High-pass filters are also possible.

14 Band-Pass Filters A band-pass filter combines both high- and low-pass filters. It passes a “band” of frequencies around a center frequency.

15 Band-Pass Filtering Basic idea: components of the input spectrum have to conform to the shape of the band-pass filter.

16 Bandwidth Bandwidth is the range of frequencies over which a filter will respond at.707 of its maximum output. bandwidth Half of the acoustic energy passed through the filter fits within the bandwidth. Bandwidth is measured in Hertz.

17 Different Bandwidths narrow band wide band

18 Your Grandma’s Spectrograph Originally, spectrographic analyzing filters were constructed to have either wide or narrow bandwidths.

19 Narrow-Band Advantages Narrow-band spectrograms give us a good view of the harmonics in a complex wave… because of their better frequency resolution. modal voicing EGG waveform

20 Narrow-Band Advantages Narrow-band spectrograms give us a good view of the harmonics in a complex wave… because of their better frequency resolution. tense voicing EGG waveform

21 Comparison Remember that modal and tense voice can be distinguished from each other by their respective amount of spectral tilt. modal voicetense voice

22 A Real Vowel Spectrum Why does the “spectral tilt” go up and down in this example?

23 The Other Half Answer: we filter the harmonics by taking advantage of the phenomenon of resonance. Resonance effectively creates a series of band-pass filters in our mouths. += Wide-band spectrograms help us see properties of the vocal tract filter.

24 Formants Rather than filters, though, we may consider the vocal tract to consist of a series of “resonators”… with center frequencies, and particular bandwidths. The characteristic resonant frequencies of a particular articulatory configuration are called formants.

25 Wide Band Spectrogram Formants appear as dark horizontal bars in a wide band spectrogram. Each formant has both a center frequency and a bandwidth. formants F1 F2 F3

26 Narrow-Band Spectrogram A “narrow-band spectrogram” clearly shows the harmonics of speech sounds. …but the formants are less distinct. harmonics

27 A Static Spectrum Note: F0  160 Hz F1 F2 F3 F4

28 Questions 1.How does resonance occur? And how does it occur in our vocal tracts? 2.Why do sounds resonate at particular frequencies? 3.How can we change the resonant frequencies of the vocal tract? (spectral changes)

29 Some Answers Resonance: when one physical object is set in motion by the vibrations of another object. Generally: a resonating object reinforces (sound) waves at particular frequencies …by vibrating at those frequencies itself …in response to the pressures exerted on it by the (sound) waves. In the case of speech: The mouth (and sometimes, the nose) resonates in response to the complex waves created by voicing.

30 Traveling Waves Resonance occurs because of the reflection of sound waves. Normally, a wave will travel through a medium indefinitely Such waves are known as traveling waves. Check out the tsunami!

31 Reflected Waves If a wave encounters resistance, however, it will be reflected. What happens to the wave then depends on what kind of resistance it encounters… If the wave meets a hard surface, it will get a true “bounce” Compressions (areas of high pressure) come back as compressions Rarefactions (areas of low pressure) come back as rarefactions

32 Sound in a Closed Tube timetime

33 Wave in a closed tube With only one pressure pulse from the loudspeaker, the wave will eventually dampen and die out What happens when: another pressure pulse is sent through the tube right when the initial pressure pulse gets back to the loudspeaker?

34 Standing Waves The initial pressure peak will be reinforced The whole pattern will repeat itself Alternation between high and low pressure will continue...as long as we keep sending in pulses at the right time This creates what is known as a standing wave.

35 Tacoma Narrows Movie

36 Lenticular Clouds An interesting example of standing waves that we can often see around Calgary is called a lenticular cloud. These are formed by air (wind) bouncing in waves over the mountains. When the air reaches a certain height, it will condense into clouds. After it drops back down, the condensation will disappear.  The clouds stay in one place while the wind passes through them! (check out http://www.atoptics.co.uk)

37 Standing Wave Terminology node: position of zero pressure change in a standing wave node

38 Standing Wave Terminology anti-node: position of maximum pressure change in a standing wave anti-nodes

39 Resonant Frequencies Remember: a standing wave can only be set up in the tube if pressure pulses are emitted from the loudspeaker at the appropriate frequency Q: What frequency might that be? It depends on: how fast the sound wave travels through the tube how long the tube is How fast does sound travel? ≈ 350 meters / second = 35,000 cm/sec ≈ 1260 kilometers per hour (780 mph)

40 Calculating Resonance A new pressure pulse should be emitted right when: the first pressure peak has traveled all the way down the length of the tube and come back to the loudspeaker.

41 Calculating Resonance Let’s say our tube is 175 meters long. Going twice the length of the tube is 350 meters. It will take a sound wave 1 second to do this Resonant Frequency: 1 Hz 175 meters

42 Wavelength New concept: a standing wave has a wavelength The wavelength is the distance (in space) it takes a standing wave to go: 1.from a pressure peak 2.down to a pressure minimum 3.back up to a pressure peak For a waveform representation of a standing wave, the x- axis represents distance, not time.


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