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Two Vacuums Shopvac Bosch Dept. of Mech. Engineering 1

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Presentation on theme: "Two Vacuums Shopvac Bosch Dept. of Mech. Engineering 1"— Presentation transcript:

1 Two Vacuums Shopvac Bosch Dept. of Mech. Engineering 1
University of Kentucky 1

2 Bosch Vacuum Exhaust flows through foam Dept. of Mech. Engineering 2
University of Kentucky 2

3 Shopvac Vacuum Dept. of Mech. Engineering University of Kentucky 3

4 Sound Quality Bosch (original) Bosch (w/o foam) Shopvac
Bosch (w/o 1st peak) Dept. of Mech. Engineering University of Kentucky 4

5 Sound Quality: Jury Test
Note: Rate each vacuum on a scale from 1 to 10 where 1 is “very quiet” and 10 is “very loud.” Dept. of Mech. Engineering University of Kentucky 5

6 Foam Inside Bosch Vacuum
Dept. of Mech. Engineering University of Kentucky 6

7 Sound Intensity (Shopvac)
Dept. of Mech. Engineering University of Kentucky 7

8 Sound Intensity (Bosch)
Dept. of Mech. Engineering University of Kentucky 8

9 Sound Intensity (Bosch)
Dept. of Mech. Engineering University of Kentucky 9

10 Lesson 2 Noise Measurements
Slides © 2006 by A. F. Seybert

11 Instrumentation Function Generator Loud- Sound level meter sine wave
square wave Loud- speaker Sound level meter PC Spectrum analyzer Display 11 Dept. of Mech. Engineering University of Kentucky

12 SLM Calibration 94 dB tone @ 1 kHz Calibrator
Adjust until display reads 94 dB Calibration should be checked each time SLM is turned on and before it is turned off. 12 Dept. of Mech. Engineering University of Kentucky

13 Pure Tone Sounds Pure tones are sounds at a single frequency
13 Dept. of Mech. Engineering University of Kentucky

14 Fourier Series of a Square Wave
time Frequency Spectrum 14 Dept. of Mech. Engineering University of Kentucky

15 Reference Quantities and Decibel Scales
Definition of the decibel: Example: what is the sound pressure level of a pure tone sound having a peak sound pressure of 1 Pa? 15 Dept. of Mech. Engineering University of Kentucky

16 Typical Sound Pressure Levels
Source/Environment LP (dB) prms (Pa) Launch noise, near payload bay ,000 Heavy artillery near gunner’s head Large jet engine, 30 m Inside textile factory (uncontrolled) Shouted male voice, 1 m Two-person conversation Residential neighborhood, night Empty symphony hall Average threshold of hearing (1 kHz) 16 Dept. of Mech. Engineering University of Kentucky

17 Sound Level Meter Block Diagram
Micro- phone Meter Filter Circuit Amp Weighting Networks Rectifier RMS To oscilloscope or analyzer if desired pi Sound pressure e0 e1 e2 e3 e4 A, B, C, flat Fast/Slow 17 Dept. of Mech. Engineering University of Kentucky

18 The Electrodynamic (Moving Coil) Microphone
Sound Waves Vibrate Diaphragm Voltage output from coil is Proportional to velocity Of Diaphragm (the inverse of a loudspeaker) 18 Dept. of Mech. Engineering University of Kentucky

19 The Piezo-electric Microphone
19 Dept. of Mech. Engineering University of Kentucky

20 The Condenser (Capacitor) Microphone
20 Dept. of Mech. Engineering University of Kentucky

21 Condenser Microphone - Schematic
Sound Waves Diaphragm (foil, ” thick) Air gap, 0.001” Protective Grid Quartz insulator Back plate with damping holes e0 Polarization voltage Eb Variable capacitance case e0 Polarization voltage Eb Equivalent Circuit 21 Dept. of Mech. Engineering University of Kentucky

22 Characteristics of the Condenser Microphone
High sensitivity – 25 to 50 mV/Pa Requires polarizing voltage of V dc (needed to initially charge the microphone); determines sensitivity Wide frequency response (limited by diaphragm resonance frequency at high frequency and venting at low frequency) Good linearity over a wide range of sound levels High output impedance – requires signal conditioning close to diaphragm Susceptible to humidity when temperature is close to the dew point Delicate B&K 4190 ½” microphone: Sensitivity: 50 mV/Pa Polarization: 200 V dc Frequency range: 5 Hz – 10 kHz (+/- 1 dB); resonance freq. = 14 kHz SPL range: 15 dB – 148 dB (3% distortion) Operating temperature range: -30 to 150 degrees C 22 Dept. of Mech. Engineering University of Kentucky

23 Frequency Analysis of Noise
Uses of frequency analysis: Noise source diagnostics (resonances, etc.) Qualification testing of prototypes Conformance to company, industry, or international standards Other Types of frequency analysis: Narrowband (FFT based) – best frequency resolution (reveals narrow peaks due to resonances, harmonics); lots of data Octave band – best for broadband noise – limited data One-third, one-twelfth octave bands – narrower versions of octave band filters 23 Dept. of Mech. Engineering University of Kentucky

24 Octave Band Filters etc. 0.707 x center frequency Frequency (Hz)
63 125 250 1000 500 Each octave band filter has a fixed center frequency and is twice as wide as the one before it. Each octave band filter may be divided into three one-third octave band filters for more frequency resolution. etc. 0.707 x center frequency 24 Dept. of Mech. Engineering University of Kentucky

25 Octave Band Filters (Partial List)
Center Frequency (Hz) Lower Band Limit (Hz) Upper Band Limit (Hz) 63 44 88 125 177 250 355 500 710 1000 1420 2000 2840 4000 5680 8000 11360 16000 22720 25 Dept. of Mech. Engineering University of Kentucky

26 One-Third Octave Band Filters (Partial List)
Center Frequency (Hz) Lower Band Limit (Hz) Upper Band Limit (Hz) 50 44.7 56.2 63 70.8 80 89.1 100 112 125 141 160 178 200 224 250 282 315 355 26 Dept. of Mech. Engineering University of Kentucky

27 Example Same Spectrum, Various Frequency Bands
27 Dept. of Mech. Engineering University of Kentucky

28 Equal Loudness Contours
Experiment: ask subjects to compare a second tone to one at 1 kHz by increasing or decreasing the level of the second tone until it the two tones have equal loudness. Sounds at lower frequency must have a higher SPL to be judged equivalent in loudness to the tone at 1 kHz. The hearing mechanism does not have a flat frequency response. 28 Dept. of Mech. Engineering University of Kentucky


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