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    參數(shù)資料
    型號: LTC1966CMS8
    廠商: LINEAR TECHNOLOGY CORP
    元件分類: 模擬專用變換器
    英文描述: Precision Micropower, SIGMA RMS-to-DC Converter
    中文描述: RMS TO DC CONVERTER, PDSO8
    封裝: PLASTIC, MSOP-8
    文件頁數(shù): 17/32頁
    文件大小: 444K
    代理商: LTC1966CMS8
    17
    LTC1966
    sn1966 1966fas
    prior generation log/antilog RMS-to-DC converters, whose
    averaging time constants are dependent on the signal
    level, resulting in excruciatingly long waits for the output
    to go to zero.
    The shape of the rising and falling edges will be dependent
    on the total percent change in the step, but for less than the
    100% changes shown in Figure 11, the responses will be
    less distorted and more like a standard exponential decay.
    For example, when the input amplitude is changed from
    100mV to 110mV (+10%) and back (–10%), the step
    responses are essentially the same as a standard expo-
    nential rise and decay between those two levels. In such
    cases, the time constant of the decay will be in between
    that of the rising edge and falling edge cases of Figure 11.
    Therefore, the worst case is the falling edge response as
    it goes to zero, and it can be used as a design guide.
    APPLICATIOU
    W
    U
    U
    Figure12 shows the settling accuracy vs settling time for
    a variety of averaging capacitor values. If the capacitor
    value previously selected (based on error requirements)
    gives an acceptable settling time, your design is done.
    But with 100
    μ
    F, the settling time to even 10% is a full 38
    seconds, which is a long time to wait. What can be done
    about such a design If the reason for choosing 100
    μ
    F is
    to keep the DC error with a 75mHz input less than 0.1%,
    the answer is: not much. The settling time to 1% of 76
    seconds is just 5.7 cycles of this extremely low frequency.
    Averaging very low frequency signals takes a long time.
    However, if the reason for choosing 100
    μ
    F is to keep the
    peak error with a 10Hz input less than 0.05%, there is
    another way to achieve that result with a much improved
    settling time.
    Figure 11a. LTC1966 Rising Edge with C
    AVE
    = 1
    μ
    F
    Figure 11b. LTC1966 Falling Edge with C
    AVE
    = 1
    μ
    F
    TIME (SEC)
    0
    0
    L
    20
    40
    60
    80
    100
    120
    0.1
    0.2
    0.3
    0.4
    1966 F11a
    0.5
    C
    AVE
    = 1
    μ
    F
    TIME (SEC)
    0
    0
    L
    20
    40
    60
    80
    100
    120
    0.2
    0.4
    0.6
    0.8
    1966 F11b
    1
    C
    AVE
    = 1
    μ
    F
    SETTLING TIME (SEC)
    0.01
    0.1
    S
    1
    10
    1
    10
    0.1
    100
    1966 F12
    C = 100
    μ
    F
    C = 47
    μ
    F
    C = 22
    μ
    F
    C = 10
    μ
    F
    C = 4.7
    μ
    F
    C = 2.2
    μ
    F
    C = 0.47
    μ
    F
    C = 0.22
    μ
    F
    C = 0.1
    μ
    F
    C = 1
    μ
    F
    Figure 12. LTC1966 Settling Time with One Cap Averaging
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