Wittek Stereo Surround (1)

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    about Stereo and Surround

    Considerations on Stereo andSurround recording, reproductionand perception

    Helmut Wittek

    SCHOEPS GmbH, Karlsruhe, Germany

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    Contents

    Contents:

    - An overview of psychoacoustics and appliedmicrophone techniques

    - Both theory and practical demonstration, bycalculating and listening

    Topics

    Source localisation / stereophonic localisation

    Theories of microphone design Microphone setups and their properties

    The microphone and its properties

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    Source localisation

    Where is the source?

    At which distance?

    In which room, what is the room like? What does the

    source radiate?

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    2 radiating sources

    Only one perceived phantom source

    Existing theory:Summing localisation = synthesis of theloudspeaker signals that leads to the original

    source signal (Blumlein)

    Stereophonic localisation

    L R

    Phantom

    source

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    Real source, 15on the right

    Phantom Source,

    perceived ca. 15on the right,L=7dB, t=0 ms

    Phantom Source,

    perceived ca. 15on the right,L=3.5dB, t=0.2ms

    Phantom Source,perceived ca. 15on the right,

    L=0dB, t=0.4 ms

    Summing localisation

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    Summing localisation

    Real sourcePerceived Direction + 15

    Phantom sourcePerceived Direction + 15Interchannel Level Difference

    L = 7 dB 0,13 ms

    0,13 ms

    Interaural Cross Correlation( = Interaural Time Delay ITDvs. frequency)

    -1 ms +1 ms0

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    Summing localisation

    Virtual sourcePerceived Direction + 15

    Phantom sourcePerceived Direction + 15Interchannel Time Delay

    t = 0,4 ms 0,4 ms

    0,13 ms

    Interaural Cross Correlation( = Interaural Time Delay ITDvs. frequency)

    -1 ms +1 ms0

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    Other hypothesis

    Problems of the summing localisation theory: Works only below ca.1500 Hz

    Works only for level panning

    Works only in the sweet spot

    It cannot explain the perceived sound colour

    Other hypothesis for stereophonic

    localisation/perception:Stereo signals can be perceivedseparately

    Binaural decolouration (Salomons, Brggen)

    Association model (Theile, 1980)

    After the separate localisation, the fusion of thecoherent signals takes place no physicalsuperposition, no comb filtering

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    Consequences for the sound engineer

    1. Do we aim at a physical synthesis instereo? (as doAmbisonics, Blumlein)

    2. Can only coincident microphones create

    spatial sound?

    3. Are time differences allowed?(see e.g. Lipshitz: Are the purists wrong?,JAES)

    4. Can we use microphones at ear spacing?(like ORTF, SCHOEPS sphere microphone)

    5. Is it wise to allow crosstalk in surroundmicrophones? (see Lee/Rumsey, AES)

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    Source localisation

    Where is the source?

    At which distance?

    In which room, what is the room like?

    t0 ms 30 ms

    Direction Distance,

    Depth,Spaciousness

    Spatial impression

    Theile

    Envelopment

    Reverberance

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    Source localisation

    Discrete Signals:

    Correlated at both ears

    From discrete directions

    Diffuse Signals:

    Decorrelated at both ears

    From all directions

    t0 ms 30 ms

    Direction Distance,

    Depth,Spaciousness

    Spatial impression

    Theile

    Envelopment

    Reverberance

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    s

    Directions and points in time

    010

    2030 ms

    time

    Direct Sound

    Early Reflections

    Reverb

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    5.1 Reflection pattern

    L R

    010

    2030

    mstime

    Direct Sound

    Early Reflections

    Reverb

    1. Envelopment is hardly possible in 2-ch stereo

    2. No real depth is possible in 2-ch stereo3. Reflection density too high! has to be reduced

    4. Reverb should be reproduced as diffuse as

    possible decorrelated!

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    Diffuse field correlation

    Reproduction of thereverb tail:

    - Should be diffuse,should be perceived

    from everywhere- The more correlation,

    the narrower theimage of the reverb tail

    The diffuse soundshould be reproduceddecorrelated. The

    decisive measure iscalled:

    Diffuse field correlation

    (DFC)

    L R

    L R

    L R

    DFC = 0

    DFC = 0.5

    DFC = 1

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    Perceptual consequence of correlated diffusefield reproduction Demo

    DFC of coincident microphone setups:

    Diffuse field correlation

    0

    Blumlein,

    90,Figure-8

    XY,

    180,Cardioids

    XY,

    120,Super-

    cardioids

    XY,

    90,Cardioids

    Setup

    0.50.230.75DFC

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    Correlation

    Correlation vs. microphone angle

    Supe

    rcardioids

    Co

    rrelationcoe

    fficient(DFC

    )

    XY

    Omnis

    Offset angle ()

    Blumlein

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    a/b and ORTF correlation

    DFC of spaced microphones Calculation

    Shuffling techniques could correct for that

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    Directional Imaging

    Level and timedifferences govern theperceived phantomsource direction

    L = f (L) ;

    t = f (t) ;

    = L

    + t

    ;

    The necessaryinterchanneldifferences are rather

    similar to thoseknown from naturalhearing

    7,5 % / dB

    100%

    50%

    75%

    25%Phantom

    sourceshift

    0 3 9 126

    Interchannel level difference L [dB]

    15

    A

    DC

    B

    100%

    50%

    75%

    25%Phantoms

    ourceshift

    0 0,2 0,8 1,00,60,4Interchannel time differencet [ms]

    13 % / 0,1ms

    B

    D

    E

    A

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    Comparison of stereo setups

    Recording angle Recording angle 75%

    Image Assistant on www.hauptmikrofon.de

    Comparison of different stereo setups sharing thesame recording angle Demo Showroom

    www.schoeps.de/showroom/

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    2-ch Microphone Design

    Directional Image:can be calculated, differences betweenstereo techniques regarding the image

    Diffuse Field Correlation DFC:should be minimal: not possible with smalla/b or normal cardioid XY

    Further points of interest: Reality is not always ideal! Type and properties of single capsules

    (pressure/pressure gradient transducer)

    Direct/Reverb ratio controls reflection level Loudness balance

    Size of the setup

    Sensitivity to wind noise

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    XY

    UMS 20 UMS 20

    M100C

    CMXY

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    MS

    CMIT MS

    CMC 64 + CCM 8

    RCY

    SGMSC

    (CCM4 + CCM8)

    MS-BLM

    WSR MS

    UMS 20

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    ORTF and AB Stereo

    STCg

    MSTC 64 U, STC

    M100C

    UMS 20

    KFM 6

    MAB1000

    ORTF

    Outdoor Set

    Decca3 * CCM 2H

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    5.1 Reflection pattern

    RS

    L R

    LS

    C

    010

    2030

    mstime

    Direct Sound

    Early Reflections

    Reverb

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    L R

    C

    LS RS

    Early reflections

    Reverb

    Imaging area

    5.1 Spatial reproduction

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    Surround Microphone Design

    Directional Image: Image Assistant

    Crosstalk: no 3 correlated signals!

    L h

    C

    R

    L, R: Super-CardioidC: Cardioidb: 40 .... 100 cm

    h: 8 cm

    OCT

    b

    MK 41 MK 41V

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    Stability in 5.1

    Localisation curve on off-centre position

    INA 3OCT 70 Quasi-ORTF

    Einfallswinkel (Grad)

    Sitzposition LINKS: Lokalisationskurven experimentell

    (Mittelwert + 95% Vertrauensbereich)

    R

    Auslenkung

    (Grad)

    -60 0 60

    -30

    30

    0

    30-30

    -15

    15

    30

    15

    0

    -30

    -15

    Perceivedsourcedirection

    Sound source direction

    Quasi-ORTFINA 3OCT 70

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    OCT Surround

    Lh

    C

    R

    OCT Surround

    b

    b + 20 cm

    40 cm

    LS RS

    Early reflections

    Reverb

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    OCT Surround Setup

    OCT Surround(using MAB1000 and CCM microphones)

    40 cm

    Front + 20cm

    40 - 100 cm

    8 cm

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    OCT + Hamasaki

    Lh

    C

    R

    OCT + Hamasaki square

    b

    > 2 m

    LS RS

    Early reflections

    Reverb

    L R

    > 2 m

    + -

    + -

    +-

    +-

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    IRT cross

    IRT cross for Surround atmos: 20-25cm

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    Surround non-coincident

    IRT cross

    OCT Surround

    Decca3 * CCM 2H

    KFM 360

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    Double MS: The M/S principle

    R-LS

    RLM

    =

    +=

    )S-M(*

    2

    1R

    )SM(*2

    1L

    =

    +=

    M

    S

    LR

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    The Double M/S idea

    Front M/S pair

    Rear M/S pair

    CombinedDouble M/S triplet

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    The Double M/S decoding

    Double M/S enables 2 different decodingmethods:a) each pair is decoded separately

    b) decoding utilizes the third microphone as well

    L R

    L R

    a)

    b)

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    Crosstalk

    Crosstalk in Double M/S

    Avoid crosstalk by optimal decoding

    4ch 5ch

    T l f D di

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    Tools for Decoding

    Decoding variants: 2 M/S Matrices

    Hardware (MDMS U)

    Software (VST PlugIn)

    Try by yourself, its free!

    www.schoeps.de/dmsplugin.htm

    Fil di

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    Film recording

    Double M/S with shotgun

    S d i id t

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    Surround - coincident

    CMIT-Double M/S

    Double M/S

    Higher Order Techniq es

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    Higher Order Techniques

    Which higher order technique can be used inpractice?

    for reproduction:

    Wavefield synthesis (WFS) and Higher OrderAmbisonics (HOA) can recreate sound fields

    Stereo can (only) generate the sameperception in the sweet spot

    for recording:

    Higher order microphone techniques areeither noisy and/or can not yet deliver a fullysatisfying and stable timbral quality, but

    proposals will come for special applications

    WFS or Stereo?

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    WFS or Stereo?

    Wittek, Rumsey, Theile, Journal of the AES, Vol.55/9, 2007:

    Colouration of WFS and Stereo:

    Is stereo just a poor 2-ch wavefield synthesis?

    WFS or Stereo?

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    WFS or Stereo?

    Pe

    rceivedColouration

    Real - WFS - Stereo

    Wittek, Rumsey, Theile, Journal of the AES, Vol.55/9, 2007:

    Colouration of WFS and Stereo

    What does the microphone need?

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    What does the microphone need?

    The microphone is the basis for all. Well-known parameters govern the quality:

    Good frequency response

    Smooth polar pattern

    Low noise floor

    Good reliability

    And the sound

    Thank you.

    [email protected]