Measuring Maximum Continuous SPL with Multi- Tone Stimuli Maximum... · • Amplifier clipping...

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Measuring Maximum Continuous SPL with Multi- Tone Stimuli Gregor Höhne

Transcript of Measuring Maximum Continuous SPL with Multi- Tone Stimuli Maximum... · • Amplifier clipping...

  • Measuring Maximum Continuous SPL with Multi-

    Tone Stimuli

    Gregor Höhne

  • Agenda

    • Introduction/Motivation

    o What is max SPL and why do we need to specify it

    o Limiting factors for max SPL

    • Existing Measurement Techniques

    o Overview on ANSI/CEA-2010-A and B

    • Proposed Improvements

    o Multi-tone Stimuli

    o Compression Prediction

    o Advanced Interpretation

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  • What limits the Sound Pressure Output ?

    for a sinusoidal input with different On/Off Cycle

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    SOUND PRESSURE LEVEL

    dB

    - [

    V]

    (rm

    s)

    Frequency [Hz]

    Maximal SPL (short term)

    1 s on, 1 min off

    Maximal SPL (long term)

    Stepped sine 1 min on, 1 min off

    Limited by voice coil heating

    Limited by peak

    displacement

    Limited by maximal acceleration handled by

    the coil, cone, glue

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  • Factors Limiting Maximal Output

    Peak displacement

    • Transducer nonlinearities distortion, compression

    • Mechanical protection system attenuation of bass signal

    Acceleration

    • Cone, coil Damage of the mechanical parts

    Peak voltage at amplifier output (active loudspeaker system)

    • Amplifier clipping impulsive distortion

    • Limiter, gain control, protection

    Coil temperature

    • Increase of Re Power compression thermal damage

    • Thermal protection system attenuation of total signal

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  • Large Signal Performance

    • Maximal SPLmax rated at reference point (1 m, on-axis) in specified frequency range (or corresponding maximum input umax)

    • Compression of fundamental component (thermal and nonlinear effect)

    • Harmonic distortion (THD + nth-order components, equivalent input distortion measured with steady-state tones or burst, sweep)

    • Intermodulation distortion (two-tone IMD, multi-tone MTD)

    • Impulsive distortion (PHD, CHD) indicating rub&buzz, loose particles

    • Modulated noise (MOD) indicating air leakage

    • Durability verified in long-term and accelerated life testing (100 h)

    Specifications for Active and Passive Loudspeaker Systems

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  • Agenda

    • Introduction/Motivation

    o What is max SPL and why do we need to specify it

    o Limiting factors for max SPL

    • Existing Measurement Techniques

    o Overview on ANSI/CEA-2010-A and B

    • Proposed Improvements

    o Multi-tone Stimuli

    o Compression Prediction

    o Advanced Interpretation

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  • ANSI/CEA-2010-A/B

    Targets: • How loud in volume and how low in frequency is the speaker capable of

    operation?

    • measure and report maximum usable sound pressure level • required output power of amplifier

    • for Manufacturer - capability of the speaker

    • for Consumer - Simple rating „…to select, purchase and enjoy a subwoofer,

    that will complement their main full-range loudspeaker system.“

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  • Burst Test (CEA-2010-A)

    -2

    -1

    0

    1

    2

    0 200 400 600

    Stimulus

    Limit Check

    [ms]

    [V]

    Maximum SPL (last passed Peak value)

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    0 200 400 600

    [ms]

    [Pa]

    Microphone Signal

    Peak Value

    Increase Voltage

    FAIL

    PASS

    10 100 1k 10k [Hz]

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    Thresholds

    [dB]

    fundamental 2nd

    3rd 4th

    5th

    higher order + noise

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  • Burst Test Results

    Tone Burst Center Frequency (Hz)

    Maximum SPL CEA-2010 Rating

    20 79

    84 25 85

    31.5 89

    40 96

    100 50 101

    63 104

    SPLMAX rated to 1m and 2.83V

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    100

    20 30 40 50 60

    Input V

    oltage

    Maximum SPL

    [dB

    SP

    L]

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  • SPL Continuous (ANSI/CEA 2010 B)

    FAIL

    PASS

    1 min Heating

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    [ d B

    ]

    3dB compression

    Reference

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    10 2 10 3 10 4

    Frequency [Hz]

    Increase Voltage

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    DEBUG U(f)

    U(f)

    Shaped Pink Noise

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    DEBUG p(f)

    p(f)

    microphone spectrum

    SPLMUCO (Maximum Usable Continuous SPL)

    𝑆𝑃𝐿𝑀𝑈𝐶𝑂

    = 10 ∙ lg 𝑝(𝑓𝑖)2

    𝑛

    𝑖=1

    Transfer Function H(f)

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  • Pink Noise Stimulus

    • Musik-like Signal

    • Allows only interpretation of transfer function o THD and IMD only visible when having severe impact on fundamental

    o Usually only thermal compression is visible

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    Input Signal Generation According to ANSI/CEA 2010-B

    HP 20Hz LP 4.4kHz LP 8kHz Pink Noise

  • Overview - ANSI/CEA 2010 A & B CEA 2010 A – Burst Test CEA 2010 B - SPL Continuous

    Stimulus • burstshort excitation • 6.5 periodes • single frequency

    • shaped pink noise • full band excitation • additional preheating (1 min)

    Limits • harmonic burst distortion (e.g. 2nd -10dB, 3rd -20 dB etc. )

    • Compression in passband of magnitude within 3 -3.5 dB

    Results • Maximum SPL of each frequency bands

    Peak of microphone signal

    • SPLMUCO – Maximum Usable Continuous SPL

    Summed full band sound pressure

    Conclusion Harmonic distortion checked x Intermodulation distortion not

    considered x thermal effects not considered x impulse distortion not

    detected (loose particle)

    variation of amplitude response considering thermal effects x distortion not considered

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  • SPL Continuous with Multi-Tone Stimulus

    Properties - Full band excitation (music like)

    - Sparse spectrum

    - Deterministic stimulus

    - Finite crest factor

    Benefits - Persistent excitation of the transducer (reproducible)

    - Separation of distortion without a model

    - Defined pdf(x)

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  • How to generate the Stimulus ?

    Signal source

    loudspeaker

    ~ FTMicrophone

    Spectrum

    AnalyzerAmplifier

    Filter

    f f

    Spectrum of

    distortion

    components

    f

    N

    i

    iii tffUtu1

    2cos)(

    NiwithfTT

    f Ristarti ,...,12int1 /

    Frequencies of the sparse line spectrum logarithmically spaced

    m

    i

    i

    ma

    mmod

    2

    *21

    Random phase

    Benefits:

    - ensure comparability of the results measured by different instruments

    - easy to generate (by software implementation)

    - Modification of the stimulus should be possible (bandwidth , resolution R)

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  • Multi-Tone Measurement

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    Spectrum p(f) of microphone signal

    [dB

    ]Frequency [Hz]

    Signal lines Noise + Distortions Noise floor

    Signal level MTND

    Distortion f Sparse multi-tone complex

    Stimulus Output signal

    • distortion at fundamental frequencies • harmonic components • difference-tone components • summed tone components

    • Music-like signal • Good for quick testing

    of overall performance

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    Spectrum p(f) of microphone signal

    [dB

    ]

    Frequency [Hz]

    Signal lines Noise + Distortions Noise floor Signal level

    MTND Driver (1) - SPL Continuous - p(f)

    Multitone Distortion (MTND)

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    Noise Floor

    Distortion

    Fundamental

    microphone spectrum Relative multitone distortion from voltage

    Inp

    ut V

    olta

    ge

    1V

    6V

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  • The Causes of Multi-Tone Distortion

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    Fundamental Multi-tone Distortion

    Distortion

    Fundamental

    resonance frequency Cone Vibration

    L(i) (rising with frequency)

    Bl(x) (independent of frequency)

    Kms(x)

    L(x) (rising with frequency)

    Doppler (rising with frequency)

    Kms(x)

    Bl(x)

    L(x)

    L(i)

    Cone Vibration

    Doppler Effect

    Rms(v) Rms(v)

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  • Proposed Measurement Setup

    • Measurement of voltage at terminals gives easy clipping detection

    • Measurement of driver impedance allows additional interpretations

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    Signal Source Loudspeaker MicrophoneAmplifier

    A

    V

    ~

    Current Measurement

    Voltage Measurment

  • Checking Amplifier by Measured Voltage

    • Multi-tone spectrum allow easy observation of amplifier performance

    • Clipping can be detected by rising distortion lines

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    Spectrum U(f) of voltage at speaker terminals[d

    B] 0

    dB

    = 1

    V

    Frequency [Hz]

    Signal lines Noise + Distortion Noise floor

    Fundamental components

    Distortion generated by amplifier

    Noise floor

  • Voice Coil Temperature

    Measured via Electrical Resistance Re (t)

    • Based on voltage and current

    measurement

    • Re (t) corresponds with mean

    value of the temperature

    • Local temperature varies in

    overhang coils

    Better cooling of inner coil

    windings (Heat radiation to

    the pole tips, convection

    cooling, high air velocity)

    Indications of a thermal damage:

    • loose windings voice coil rubbing

    • shortcut of windings with pole gap reduced resistance

    • open coil maximal resistance limited by instrument

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  • Measuring Voice Coil Temperature

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    Pilot Tone

    • Pilot Tone at low frequencies can be used to measure the DC-resistance Re • Re is directly linked to voice coil temperature:𝜌 𝑇 = 𝜌(𝑇 0) 1 + 𝛼∆𝑇 • Can be used for temperature protection • Allows prediction of thermal compression

    Fourier

    Transform

    loudspeaker

    system

    current

    sensor

    U(t) I(t)

    -

    Stimulus

    voltage

    sensor

    power

    amplifier

    Pilot

    Tone

    Temperature

    Calculation

    Resistance of cold

    speaker

    Conductivity of Coil

    Material

    Increase of VC

    Temperature

  • Predicting Thermal Compression

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    MMD CMD RMD-1Bl

    Re (T0)

    v=dx/dt

    i

    Blv

    F=Bli

    USd

    p

    j2XAR(f)

    qa=Sdv

    pSd

    ZL(f)

    2RAR(f)

    ΔRe (ΔT)

    • Increasing temperature leads to increasing DC-resistance • Additional resistance reduces force driving the transducer • High influence where total speaker impedance is low • Predicted thermal compression at temperature T:

    𝐶(∆𝑇) = 20log10𝑍 𝑇0 + ∆𝑅𝑒(∆𝑇)

    𝑍((𝑇0)

  • Separating Thermal Compression

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    nonlinear effects

    1V - Reference

    6V – thermal comp. (predicted)

    6V - measured

    100 1k 10k

    Frequency [Hz]

    30

    dominated by thermal compression

    Transfer fucntion H(f)

    5

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    1,5 2,0 2,5 3,0 3,5 4,0 4,5 5,0 5,5 6,0

    Increase of voice coil temperature

    [V]

    [K]

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    Thermal Compression

    0°C 10°C 20°C 30°C 40°C

    ∆𝑇 = 10K

    ∆𝑇 = 20K

    ∆𝑇 = 30K

    ∆𝑇 = 40K

    Incr

    easi

    ng

    voic

    e co

    il te

    mp

    erat

    ure

    Frequency [Hz]

    [dB]

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  • Separating Distortion Sources with Nonlinear

    System Identification

    A

    V

    Digitalprocessing

    unit

    Power amplifier Speaker

    Nonlinear System

    Identification

    Voltage & Current

    Multi-tone complex

    Stimulus

    • Feeding measured state Signals allows identification of nonlinear loudspeaker parameters

    • Non-linear model allows revealing contribution of different distortion signals to total distortion

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  • Root Cause Analysis of Nonlinear Distortion

    Exercise: Microspeaker

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    Distortion Components

    [ d B

    ]

    Le(i)

    fundamental components

    20

    10 2 10 3 10 4

    Frequency [Hz]

    Bl(x)

    Kms(x)

    Le(x)

    out of band distortion

    total distortion

    Rms(x,v)

    fs=600 Hz

    showing the contribution of each nonlinearity

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  • Summary

    • Using multi-tone stimuli for determining the maximum continuous SPL allows:

    Easy interpretation of distortion generated by amplifier and transducer

    Possibility to utilize measured state signal for nonlinear system identification

    • Measuring the voice coil resistance allows:

    Implementation of temperature protection

    Separation of nonlinear effects from thermal compression

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