MANagement of anthropogenic NOISE and MANagement of anthropogenic NOISE and its impacts on terrestrial and marine habitats its impacts on terrestrial and marine habitats in sensitive areasin sensitive areas

Author: Angelo Farina – HTTP://www.angelofarina.it E-mail: farina@unipr.it – Skype: angelo.farina

““Underwater applications of the Brahma and Underwater applications of the Brahma and Citymap technologies for the Interreg project:

Citymap technologies for the Interreg project:

““

MANagement of anthropogenic NOISE and MANagement of anthropogenic NOISE and its impacts on terrestrial and marine habitats its impacts on terrestrial and marine habitats

in sensitive areas in sensitive areas

University of Parma

Industrial Engineering Department HTTP://ied.unipr.it

Goals

• Explanation of the Ambisonics technology, as currently employed in room acoustics

• Brahma: the first underwater 4-channels digital sound recorder

• A tetrahedrical hydrophone array for Brahma

• Sound source localization from Ambisonics (B-format) recordings

• Noise immission mapping employing a modified version of the CITYMAP computer program

Ambisonics technology

• Ambisonics was invented in the seventies by Michael Gerzon (UK)

• It was initially a method for recording a 4-

channel stream, which later was played back inside a special loudspeaker rig

• It is based on the pressure-velocity

decomposition of the sound field at a point

• It makes it possible to capture the complete

three-dimensional sound field, and to reproduce it quite faithfully

Ambisonics recording and playback

Reproduction occurs over an array of 8-24 loudspeakers, through an Ambisonics decoder

Original Room Sound Source

SoundField Microphone

B-format 4- channels signal

(WXYZ) Ambisonics decoder

Speaker array in the reproduction room

Recording Processing

Playback Encoding

B-Format

Decoding

Speaker-feeds

Ambisonics Technology

The Soundfield microphone

• This microphone is equipped with 4

subcardioid capsules, placed on the faces of a thetraedron

• The signal are analogically processed in its own special control box, which derives 4 “B-format” signals

• These signals are:

• W : omnidirectional (sound pressure)

• X,Y,Z : the three figure-of-eight microphones aligned with the ISO cartesian reference system – these signals are the cartesian components of the “particle velocity” vector

Other tetrahedrical microphones

• Trinnov, DPA, CoreSound, Brahma are other

microphone systems which record natively the A-format signals, which later are digitally converted to B-format

The B-format components

• Physically, W is a signal proportional to the pressure, XYZ are signals proportional to the three Cartesian

components of the particle velocity

• when a sound wave

impinges over the microphone from the “negative” direction of the x-axis, the signal on the X output will have polarity

reversed with respect to the W signal

A-format to B-format

• The A-format signals are the “raw” signals coming from the 4 capsules, loated at 4 of the 8 vertexes of a cube, typically at locations FLU-FRD-BLD-BRU

A-format to B-format

• The A-format signals are converted to the B-format signals by matrixing:

W' = FLU+FRD+BLD+BRU X' = FLU+FRD-BLD-BRU Y' = FLU-FRD+BLD-BRU Z' = FLU-FRD-BLD+BRU

• and then applying proper filtering:

X Y Z W

Directional components:

velocity

Omnidirectional component:

pressure

Soundfield Microphone

Polar Diagram

B-FORMAT

Recording Encoding

Processing Decoding and Playback

Recording

Recording Encoding

Processing

0 W

1

X Y Z

=0,707

=cos(A)cos(E)

=sin(A)cos(E)

s(t)=

=sin(E)

*s(t)

*s(t)

*s(t)

*s(t)

2

1

2

2

 Y  Z 

X

Decoding and Playback

Encoding (synthetic B-format)











































Z k Y

k W

k X

k Z

Z k Y

k W

k X

k Y

Z k Y

k W

k X

k W

Z k Y

k W

k X

k X

44 43

42 41

34 33

32 31

24 23

22 21

14 13

12 11

' ' '

' ^{z z}

R y

R x

y

R y

R x

x w w





















'

) cos(

) sin(

'

) sin(

) cos(

' '

) cos(

) sin(

'

) sin(

) cos(

' ' '

T z

T y

z

T z

T y

y x x

w w





















) cos(

) sin(

' '

) sin(

) cos(

' '

T z

T x

z y y

T z

T x

x

w w





















Rotation

Tilt

Tumble

Recording Encoding

Processing Decoding and Playback

Processing

Decoding & Playback

r

y z

x





 ^{G W G} ^{X cos( ) Y cos( ) Z cos( )}

2

F_i  1  ₁   ₂         

W X Y Z

G₁ G₂ G₂ G₂

cos 1

cos 1

cos 1

InvFilt₁

cos 2

cos 2

cos 2

InvFilt₂

Each speaker feed is simply a weighted sum of the 4 B-format signals.

The weighting coefficients are

computed by the cosines of the angles between the loudspeaker and the three Cartesian axes

Recording Encoding

Processing Decoding and Playback

Software for Ambisonics decoding

Audiomulch VST host

Gerzonic bPlayer

Gerzonic Emigrator

Software for Ambisonics processing

Visual Virtual Microphone by David McGriffy (freeware)

Rooms for Ambisonics playback

University of Bologna

University of Ferrara ASK (UNIPR) – Reggio Emilia

Rooms for Ambisonics playback

University of Parma (Casa della Musica)

BRAHMA: 4-channels recorder

• A Zoom H2 digital sound recorder is modified in India,

allowing 4 independent inputs with phantom power supply

BRAHMA: 4-channels recorder

• The standard microphone system is usually a terahedrical probe equipped with 4 cardioid electrect microphones

Hydrophones for Brahma

• Brahma provides phantom power (5V) for transducers equipped with integral electronics. Hence the ideal

hydrophone is the Acquarian Audio H2A:

Aquarian Audio Products A division of AFAB Enterprises

1004 Commercial Ave. #225 Anacortes, WA 98221 USA (360) 299-0372 www.AquarianAudio.com

Sensitivity: -180dB re: 1V/Pa (+/-4dB 20Hz-4.5KHz)

Frequency range: <10 Hz to >100KHz (approximate sensitivity @100KHz

= -220dB re: 1V/Pa)

Polar Response: Omnidirectional (horizontal)

Operating depth: <80 meters

Output impedance: 1 K (typical)

Power: 0.6 mA (typical)

Physical: (cable and output plug excluded)

Dimensions: 25mm x 46mm

Mass: 105 grams

Underwater probe for Brahma

• For underwater recordings, a special setup of 4 screw- mounted hydrophones is available:

Underwater case for Brahma

• Due to the small size (like a cigarette packet) it is easy to insert the Brahma inside a waterproof cylindrical

container, sealed with O-rings

• An external lead-acid battery can be included for

continuous operation up to one week (in level-activated recording mode)

cable

6V 12 Ah battery

BRAHMA: 4-channels recorder

• The probe can be mounted on a weighted base, allowing for underwater placement of the recorded, inside a waterproof case. However, the

cables are long enough (15m) also for keeping the recorder on the boat

BRAHMA: 4-channels underwater recorder

• The system is aligned vertically by means of a bubble

scope, and horizontally by means of a magnetic compass:

BRAHMA: 4-channels underwater recorder

• Once placed on the sea bed, the system is usually well accepted (and ignored) by the marine life:

Brahmavolver: the processing software

• Brahma records A-format signals. They can be converted to standard B-format by means of the Brahmavolver

program, running on Linux / Windows / Mac-OSX

BRAHMA: technical specs

• Sampling rates: 44.1 kHz, 48 kHz, 96 kHz (2 ch. only)

• Recording format: 1 or 2 stereo WAV files on SD card

• Bit Resolution: 16 or 24 bits

• 3 fixed gain settings, with 20 dB steps (traceable)

• Memory usage: 1.9 Gbytes/h (@ 44.1 kHz, 24 bits, 4 ch.)

• Recording time: more than 16 hours (with 32 Gb SD card)

• Power Supply: 6 V DC, 200 mA max

• Automatic recording when programmable threshold is exceeded

• The SD card can be read and erased through the USB port

Source localization from B-format signals

• At every instant, the source position is known in spherical coordinates by analyzing the B-format signal

 = azimuth -  = elevation

x

y z

buoy

Tetrahedrical hydrophonic probe

boat





Trajectory from multiple recording buoys

• Employing several buoys, the complete trajectory can be triangulated

The CITYAMP computer program

• Developed by University of Parma and

Italian Ministry for the Environment in 1995 during the EU-funded DISIA project

• CITYMAP makes it possible to map the

sound pressure level in large urban areas, due to noise sources such as roads,

railways and industrial plants

Sound sources

• CITYMAP manages 4 types of sound sources:

– Roads – Railways

– Wide-area industrial plants – “point sources”

• CITYMAP contains an comprehensive data- base of noise emission of Italian vehicles

(cars, trucks, motorbikes, trains, etc.)

Measurements of noise emission

• The emission data base is formed on recordings of vehicle pass-bys recorded in octave bands, with 0.5s time resolution, so that the time profile of each pass-by was obtained

60 65 70 75 80 85 90

0 1 2 3 4 5 6

Tempo (s)

Livello Sonoro (dBA)

Time profile of the pass-by of a car - d=7.5 m

Integrating this area, the Single Event Level (SEL) is

obtained:

SEL = Leq + 10log[T]

Data-Base of SEL – road vehicles

• Averaging over a large number of pass-bys,the typical value of SEL was obtained for 5 categories of vehicles, 8 speeds and 5 types of rolling surfaces:

Vehicle Type V1 - cars

V2 – small trucks, bus;

V3 – heavy trucks, double-decker bus;

V4 - TIR;

V5 - motorbykes.

Velocity ranges

C1 - 0<V<25 km/h acceler.;

C2 - 25<V<50 km/h acceler.;

C3 - 0<V<25 km/h deceler.;

C4 - 25<V<50 km/h deceler.;

C5 - 50<V<70 km/h;

C6 - 70<V<90 km/h;

C7 - 90<V<110km/h;

C8 - V > 110 km/h.

Type of rolling surface:

A1 – standard bitume – slope negligible;

A2 – standard bitume, slope > +5%;

A3 –standard bitume, slope < -5%;

A4 - pavé, slope negligible;

A5 – sound absorbing road pavement, slope negligible.

Data-Base of SEL – railway vehicles

• Averaging over a large number of pass-bys,the typical value of SEL was obtained for 3 categories of vehicles, 4 speeds and 2 types of rolling surfaces:

Vehicle type

V1 – freight train;

V2 – passenger (regional);

V3 – passenger (intercity);

Speed ranges

C1 - 0<V<60 km/h C2 - 60<V<90 km/h

C3 - 90<V<120 km/h C4 - V > 120 km/h.

Type of rails

A1 – Continuous Welded Rail on concrete sleepers and ballast;

A2 – Short rails with open joints on wood sleepers and ballast.

Computation formulas

• First of all, we get the Leq at 7.5m from axis of the road:

L N

eq m

SEL L L

i i

i asfalto i pendenza i

, . lg

, ,

7 5 10

1 5

10 10

16 3600

  































 



 

• Or from the axis of the track (railways):

L N L

eq m

SEL L L

i i

i

i binario i pendenza i

, . lg

, ,

7 5 10

1 3

10 10

16 3600 100

  

 





























 



 

Propagation at distant receivers

• The total sound power emitted by each segment of linear source is regrouped at its center:

• Then the sound level at a distance d is computed as if it was a point source:

 ^L 

L

L



 10  lg   7 . 5 

L L e

eq W d

   d

 



 



 

10 lg 4 ²





• At each receiver, the contribuition of all segments of roads and railways are energetically summed

Effects of screens

• CITYMAP computes a simplified screening effect due to obstacles, such as building or noise barriers:

L     

 

10 lg 1 + 40 f 

 c

Frequency f is assumed equal to 340 Hz

B C

A

 = B + C -A

CITYMAP software architecture

Source Manager Misure di Potenza (ISO 3744)

Misure di Direttività (balloons)

Material Manager Certificati di prova

dei materiali AutoCad (TM)

Ray CAD

Geometry File (.RAY)

Surfer (TM)

Pyramid Tracer (DISIAPYR.EXE) data base

R,

data base L ,Q w



Geographical Information Service (GIS) - Cartografia Digitale

CITYMAP.EXE

CITYMAP.EXE File di descrizione

geometrica e di emissione sonora (.CMP)

Structured SPL file (.GRD)

SPL Contour Maps (.DXF or .WMF)

Unstructured SPL file (.DAT) Dati di traffico

stradale e ferroviario File di Interscambio

(.DXF)

data base

Programma di Interfaccia - CITYMAP.EXE emissione

veicoli

CITYMAP reads the

geometry from a DXF file, the traffic flow data are inserted, the emission value of each vehicle is read from the data- base, or from a specific SPK file for point sources.

Citymap computes the sound pressure level at a number of receivers, which can be

located also on a regular grid.

The resulting GRD file is later post-processed by Surfer, for creating the map

Geometry definition in AutoCAD

• Relevant entities are 3DPOLY on layers named as STRADE, BINARI, CASE, BARRIERE

Import of DXF file in Citymap

• It is possible to select what entities are to be imported, and if they have to be appended

Traffic flow data for roads and railways

• Clicking on an entity, a new window appears, making it easy to assign traffic data.

Single-point computation

• It is very fast to compute the sound pressure level in selected points (entity CIRCLE on layer PUNTI)

Computation on a grid of receivers

• It is also possible to define a regular grid of receivers, for charting SPL maps

Post-processing with Surfer

• Surfer converts the GRD file created by Citymap in a countor map chart

From Surfer back to AutoCAD

• Finally the contour map is imported back over the original plan, for showing the noise map

Underwater extension of Citymap

• If Citymap is to be employed for underwater applications, two main modifications are required:

– A new data-base of marine noise sources needs to be compiled – The propagation algorithm must be replaced with a more realistic

one, which takes into account the inhomogeneous medium and the multiple reflections between sea surface and sea floor.

• The first task is accomplished by performing thousands of recording of pass-by recordings with various types of

boats, at various speeds, and with different sea state

• The second task requires a substantial effort for the

software developer, who will have to rewrite completely the subroutine which performs the computations

Example of usage of Underwater Citymap

• Mapping of underwater sound pressure level due to a boat along a trajectory

Times and costs

• The prototype of the recording buoy has just been finalized and tested! – the cost has been anticipated by UNIPR and AIDA (our spinoff company)

• The series production of buoys will start at

beginning of 2010. The estimated cost is 3000 € each, and it is scheduled to build 6 of them

• The recordings for compiling the source emission database will begin in summer 2010, and will last 6 months, employing 3 buoys and 2 people (12 man-months, 25.000 €)

Times and costs

• The recordings for performing surveys in the selected marine sites will also start in summer 2010. The total number of buoys will be 6 (3 used also for boat recordings, 3 only for site

surveys), and a lot of work will be required fopr deploying and recvering the buoys. The estimate cost for the surveys is 25.000 €

• The modification of the Citymap program will tale one year for one programmer (cost 25.000 €)

• The analysis of the survey recordings and the elaboration of noise maps is also to be defined, depending on the amount of data to be

processed and on the extension of the areas to be mapped. It is actually estimated at 6.000 €

Internet resources

All the papers previously published by Angelo Farina can be downloaded from his personal web site:

www.angelofarina.it

The CITYMAP program can be downloaded from:

www.angelofarina.it/Public/Disia

Its use is free for academic research in public institutions (password issued on request)