- 您現(xiàn)在的位置：買(mǎi)賣(mài)IC網(wǎng) > PDF目錄3424 > AD641AN (Analog Devices Inc)IC AMP LOG LP 2.3MA 20DIP PDF資料下載
參數(shù)資料
| 型號(hào)： | AD641AN |
| 廠商： | Analog Devices Inc |
| 文件頁(yè)數(shù)： | 15/16頁(yè) |
| 文件大?。?/td> | 0K |
| 描述： | IC AMP LOG LP 2.3MA 20DIP |
| 標(biāo)準(zhǔn)包裝： | 1 |
| 放大器類型： | 對(duì)數(shù) |
| 電路數(shù)： | 1 |
| -3db帶寬： | 250MHz |
| 電流 - 輸入偏壓： | 7µA |
| 電壓 - 輸入偏移： | 50µV |
| 電流 - 電源： | 35mA |
| 電流 - 輸出 / 通道： | 2.3mA |
| 電壓 - 電源，單路/雙路(±)： | ±4.5 V ~ 7.5 V |
| 工作溫度： | -40°C ~ 85°C |
| 安裝類型： | 通孔 |
| 封裝/外殼： | 20-DIP（0.300"，7.62mm） |
| 供應(yīng)商設(shè)備封裝： | 20-PDIP |
| 包裝： | 管件 |
第1頁(yè)第2頁(yè)第3頁(yè)第4頁(yè)第5頁(yè)第6頁(yè)第7頁(yè)第8頁(yè)第9頁(yè)第10頁(yè)第11頁(yè)第12頁(yè)第13頁(yè)第14頁(yè)當(dāng)前第15頁(yè)第16頁(yè)
REV. C
AD641
–8–
FUNDAMENTALS OF LOGARITHMIC CONVERSION
The conversion of a signal to its equivalent logarithmic value
involves a nonlinear operation, the consequences of which can be
very confusing if not fully understood. It is important to realize
from the outset that many of the familiar concepts of linear
circuits are of little relevance in this context. For example, the
incremental gain of an ideal logarithmic converter approaches
infinity as the input approaches zero. Further, an offset at the
output of a linear amplifier is simply equivalent to an offset at
the input, while in a logarithmic converter it is equivalent to a
change of amplitude at the input—a very different relationship.
We assume a dc signal in the following discussion to simplify the
concepts; ac behavior and the effect of input waveform on cali-
bration are discussed later. A logarithmic converter having a
voltage input VIN and output VOUT must satisfy a transfer func-
tion of the form
VOUT = VY LOG (VIN/VX)
Equation (1)
where VY and VX are fixed voltages which determine the scaling
of the converter. The input is divided by a voltage because the
argument of a logarithm has to be a simple ratio. The logarithm
must be multiplied by a voltage to develop a voltage output.
These operations are not, of course, carried out by explicit com-
putational elements, but are inherent in the behavior of the
converter. For stable operation, VX and VY must be based on
sound design criteria and rendered stable over wide temperature
and supply voltage extremes. This aspect of RF logarithmic
amplifier design has traditionally received little attention.
When VIN = VX, the logarithm is zero. VX is, therefore, called
the Intercept Voltage, because a graph of VOUT versus LOG
(VIN)—ideally a straight line—crosses the horizontal axis at this
point (see Figure 20). For the AD641, VX is calibrated to ex-
actly 1 mV. The slope of the line is directly proportional to VY.
Base 10 logarithms are used in this context to simplify the rela-
tionship to decibel values. For VIN = 10 VX, the logarithm has a
value of 1, so the output voltage is VY. At VIN = 100 VX, the
output is 2 VY, and so on. VY can therefore be viewed either as
the Slope Voltage or as the Volts per Decade Factor.
The AD641 conforms to Equation (1) except that its two out-
puts are in the form of currents, rather than voltages:
IOUT = IY LOG (VIN/VX)
Equation (2)
ACTUAL
0
INPUT ON
LOG SCALE
YY
2VY
IDEAL
VYLOG (VIN/VX)
VIN = VX
VIN = 100VX
VIN = 10VX
ACTUAL
SLOPE = VY
IDEAL
+
–
Figure 20. Basic DC Transfer Function of the AD641
IY, the Slope Current, is 1 mA. The current output can readily
be converted to a voltage with a slope of 1 V/decade, for ex-
ample, using one of the 1 k
resistors provided for this purpose,
in conjunction with an op amp, as shown in Figure 21.
9
12
8
13
7
14
6
15
10
11
LOG
OUT
LOG
COM
SIG
+OUT
+VS
–VS ITC BL2
SIG
–OUT
AD641
C1
330pF
1mA PER DECADE
AD846
R1
48.7
R2
OUTPUT VOLTAGE
1V PER DECADE
FOR R2 = 1k
100mV PER dB
FOR R2 = 2k
Figure 21. Using an External Op Amp to Convert the
AD641 Output Current to a Buffered Voltage Output
Intercept Stabilization
Internally, the intercept voltage is a fraction of the thermal volt-
age kT/q, that is, VX = VXOT/TO, where VXO is the value of VX
at a reference temperature TO. So the uncorrected transfer
function has the form:
IOUT = IY LOG (VIN TO/VXOT)
Equation (3)
Now, if the amplitude of the signal input VIN could somehow be
rendered PTAT, the intercept would be stable with tempera-
ture, since the temperature dependence in both the numerator
and denominator of the logarithmic argument would cancel.
This is what is actually achieved by interposing the on-chip
attenuator, which has the necessary temperature dependence to
cause the input to the first stage to vary in proportion to abso-
lute temperature. The end limits of the dynamic range are now
totally independent of temperature. Consequently, this is the pre-
ferred method of intercept stabilization for applications where
the input signal is sufficiently large.
When the attenuator is not used, the PTAT variation in VX will
result in the intercept being temperature dependent. Near 300K
(+27
°C) it will vary by 20 LOG (301/300) dB/°C, about 0.03 dB/
°C. Unless corrected, the whole output function would drift up
or down by this amount with changes in temperature. In the
AD641 a temperature compensating current IYLOG(T/TO) is
added to the output. This effectively maintains a constant inter-
cept VXO. This correction is active in the default state (Pin 8
open circuited). When using the attenuator, Pin 8 should be
grounded, which disables the compensation current. The drift
term needs to be compensated only once; when the outputs of
two AD641s are summed, Pin 8 should be grounded on at least
one of the two devices (both if the attenuator is used).
Conversion Range
Practical logarithmic converters have an upper and lower limit
on the input, beyond which errors increase rapidly. The upper
limit occurs when the first stage in the chain is driven into limit-
ing. Above this, no further increase in the output can occur and
the transfer function flattens off. The lower limit arises because
a finite number of stages provide finite gain, and therefore at
low signal levels the system becomes a simple linear amplifier.
相關(guān)PDF資料 |
PDF描述 |
|---|---|
| 94549-136HLF | BERGSTIK II SR STRAIGHT RET |
| 61276-1 | CONN RCPT 24-20AWG CRIMP GOLD |
| 68021-210 | BERGSTIK II DR RIGHT ANGLE |
| 324225 | CONN SHUR-PLUG 16-14AWG BLUE |
| 69193-514 | BERGSTIK II DR RIGHT ANGLE RET |
相關(guān)代理商/技術(shù)參數(shù) |
參數(shù)描述 |
|---|---|
| AD641ANZ | 功能描述:IC AMP LOG LP 2.3MA 20DIP RoHS:是 類別:集成電路 (IC) >> Linear - Amplifiers - Instrumentation 系列:- 標(biāo)準(zhǔn)包裝:50 系列:- 放大器類型:J-FET 電路數(shù):2 輸出類型:- 轉(zhuǎn)換速率:3.5 V/µs 增益帶寬積:1MHz -3db帶寬:- 電流 - 輸入偏壓:30pA 電壓 - 輸入偏移:2000µV 電流 - 電源:200µA 電流 - 輸出 / 通道:- 電壓 - 電源，單路/雙路(±):7 V ~ 36 V，±3.5 V ~ 18 V 工作溫度:0°C ~ 70°C 安裝類型:通孔 封裝/外殼:8-DIP（0.300"，7.62mm） 供應(yīng)商設(shè)備封裝:8-PDIP 包裝:管件 |
| AD641AP | 功能描述:IC AMP LOG LP 2.3MA 20PLCC RoHS:否 類別:集成電路 (IC) >> Linear - Amplifiers - Instrumentation 系列:- 其它有關(guān)文件:TS1854A View All Specifications 標(biāo)準(zhǔn)包裝:50 系列:- 放大器類型:通用 電路數(shù):4 輸出類型:滿擺幅 轉(zhuǎn)換速率:0.25 V/µs 增益帶寬積:630kHz -3db帶寬:- 電流 - 輸入偏壓:16nA 電壓 - 輸入偏移:1000µV 電流 - 電源:162µA 電流 - 輸出 / 通道:48mA 電壓 - 電源，單路/雙路(±):1.8 V ~ 6 V 工作溫度:-40°C ~ 125°C 安裝類型:表面貼裝 封裝/外殼:14-SOIC（0.154"，3.90mm 寬） 供應(yīng)商設(shè)備封裝:14-SO 包裝:管件 |
| AD641AP-REEL7 | 功能描述:IC AMP LOG LP 2.3MA 20PLCC RoHS:否 類別:集成電路 (IC) >> Linear - Amplifiers - Instrumentation 系列:- 標(biāo)準(zhǔn)包裝:50 系列:- 放大器類型:J-FET 電路數(shù):2 輸出類型:- 轉(zhuǎn)換速率:3.5 V/µs 增益帶寬積:1MHz -3db帶寬:- 電流 - 輸入偏壓:30pA 電壓 - 輸入偏移:2000µV 電流 - 電源:200µA 電流 - 輸出 / 通道:- 電壓 - 電源，單路/雙路(±):7 V ~ 36 V，±3.5 V ~ 18 V 工作溫度:0°C ~ 70°C 安裝類型:通孔 封裝/外殼:8-DIP（0.300"，7.62mm） 供應(yīng)商設(shè)備封裝:8-PDIP 包裝:管件 |
| AD641APZ | 功能描述:IC AMP LOG LP 2.3MA 20PLCC RoHS:是 類別:集成電路 (IC) >> Linear - Amplifiers - Instrumentation 系列:- 標(biāo)準(zhǔn)包裝:50 系列:- 放大器類型:J-FET 電路數(shù):2 輸出類型:- 轉(zhuǎn)換速率:3.5 V/µs 增益帶寬積:1MHz -3db帶寬:- 電流 - 輸入偏壓:30pA 電壓 - 輸入偏移:2000µV 電流 - 電源:200µA 電流 - 輸出 / 通道:- 電壓 - 電源，單路/雙路(±):7 V ~ 36 V，±3.5 V ~ 18 V 工作溫度:0°C ~ 70°C 安裝類型:通孔 封裝/外殼:8-DIP（0.300"，7.62mm） 供應(yīng)商設(shè)備封裝:8-PDIP 包裝:管件 |
| AD641-EB | 制造商:Analog Devices 功能描述:AD641 EVALUATION BOARD - Bulk |
發(fā)布緊急采購(gòu)，3分鐘左右您將得到回復(fù)。