• 參數(shù)資料
    型號(hào): AD820BRZ
    廠商: Analog Devices Inc
    文件頁數(shù): 9/24頁
    文件大?。?/td> 0K
    描述: IC OPAMP JFET R-R 1.8MHZ 8SOIC
    產(chǎn)品培訓(xùn)模塊: Pulse Oximetry Solutions
    Top Five Problems in Photodiode Opamp Circuits
    標(biāo)準(zhǔn)包裝: 98
    放大器類型: J-FET
    電路數(shù): 1
    輸出類型: 滿擺幅
    轉(zhuǎn)換速率: 3 V/µs
    增益帶寬積: 1.9MHz
    電流 - 輸入偏壓: 2pA
    電壓 - 輸入偏移: 300µV
    電流 - 電源: 700µA
    電流 - 輸出 / 通道: 20mA
    電壓 - 電源,單路/雙路(±): 5 V ~ 36 V,±2.5 V ~ 18 V
    工作溫度: -40°C ~ 85°C
    安裝類型: 表面貼裝
    封裝/外殼: 8-SOIC(0.154",3.90mm 寬)
    供應(yīng)商設(shè)備封裝: 8-SO
    包裝: 管件
    產(chǎn)品目錄頁面: 772 (CN2011-ZH PDF)
    AD820
    Rev. H | Page 17 of 24
    OUTPUT CHARACTERISTICS
    The AD820 unique bipolar rail-to-rail output stage swings
    within 5 mV of the negative supply and 10 mV of the positive
    supply with no external resistive load. The approximate output
    saturation resistance of the AD820 is 40 Ω sourcing and 20 Ω
    sinking. This can be used to estimate output saturation voltage
    when driving heavier current loads. For instance, when sourcing
    5 mA, the saturation voltage to the positive supply rail is 200 mV;
    when sinking 5 mA, the saturation voltage to the negative rail
    is 100 mV.
    The open-loop gain characteristic of the amplifier changes
    as a function of resistive load, as shown in Figure 10 through
    Figure 13. For load resistances over 20 kΩ, the AD820 input
    error voltage is virtually unchanged until the output voltage is
    driven to 180 mV of either supply.
    If the AD820 output is driven hard against the output saturation
    voltage, it recovers within 2 μs of the input returning to the
    linear operating region of the amplifier.
    Direct capacitive load interacts with the effective output imped-
    ance of the amplifier to form an additional pole in the amplifier
    feedback loop, which can cause excessive peaking on the pulse
    response or loss of stability. The worst case occurs when the
    amplifier is used as a unity-gain follower. Figure 40 shows
    AD820 pulse response as a unity-gain follower driving 350 pF.
    This amount of overshoot indicates approximately 20 degrees
    of phase margin—the system is stable, but is nearing the edge.
    Configurations with less loop gain, and as a result less loop
    bandwidth, are much less sensitive to capacitance load effects.
    Figure 41 is a plot of noise gain vs. the capacitive load that results
    in a 20 degree phase margin for the AD820. Noise gain is the
    inverse of the feedback attenuation factor provided by the
    feedback network in use.
    00
    87
    3-
    04
    1
    20mV
    2s
    100
    90
    10
    0%
    Figure 40. Small Signal Response of AD820 as Unity-Gain Follower Driving
    350 pF Capacitive Load
    00
    87
    3-
    0
    42
    5
    1
    300
    30k
    CAPACITIVE LOAD FOR 20 PHASE MARGIN (pF)
    N
    OIS
    E
    GA
    IN
    (
    1+
    )
    P
    I
    P
    F
    4
    3
    2
    1k
    3k
    10k
    +
    RF
    R1
    Figure 41. Noise Gain vs. Capacitive Load Tolerance
    Figure 42 shows a possible configuration for extending
    capacitance load drive capability for a unity-gain follower. With
    these component values, the circuit drives 5000 pF with a 10%
    overshoot.
    0
    08
    73
    -04
    3
    AD820
    +
    +
    +VS
    –VS
    0.01F
    20pF
    20k
    100
    VOUT
    VIN
    3
    2
    4
    7
    6
    +
    Figure 42. Extending Unity-Gain Follower Capacitive Load Capability
    Beyond 350 pF
    SINGLE-SUPPLY HALF-WAVE AND FULL-WAVE
    RECTIFIERS
    An AD820 configured as a unity-gain follower and operated
    with a single supply can be used as a simple half-wave rectifier.
    The AD820 inputs maintain picoamp level input currents even
    when driven well below the negative supply. The rectifier puts
    that behavior to good use, maintaining an input impedance of
    over 1011 Ω for input voltages from 1 V from the positive supply
    to 20 V below the negative supply.
    The full- and half-wave rectifier shown in Figure 43 operates as
    follows: when VIN is above ground, R1 is bootstrapped through
    the unity-gain follower, A1, and the loop of Amplifier A2. This
    forces the inputs of A2 to be equal; thus, no current flows through
    R1 or R2, and the circuit output tracks the input. When VIN is
    below ground, the output of A1 is forced to ground. The
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