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전자부품 반도체 검색엔진( 무료 PDF 다운로드 ) - 데이터시트뱅크

LTC2230 데이터 시트보기 (PDF) - Linear Technology

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LTC2230
Linear
Linear Technology 
LTC2230 Datasheet PDF : 32 Pages
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LTC2230/LTC2231
APPLICATIO S I FOR ATIO
60) may be used to provide the common mode bias level.
VCM can be tied directly to the center tap of a transformer
to set the DC input level or as a reference level to an op amp
differential driver circuit. The VCM pin must be bypassed to
ground close to the ADC with a 2.2μF or greater capacitor.
Input Drive Impedance
As with all high performance, high speed ADCs, the
dynamic performance of the LTC2230/LTC2231 can be
influenced by the input drive circuitry, particularly the
second and third harmonics. Source impedance and input
reactance can influence SFDR. At the falling edge of ENC,
the sample-and-hold circuit will connect the 1.6pF sam-
pling capacitor to the input pin and start the sampling
period. The sampling period ends when ENC rises, holding
the sampled input on the sampling capacitor. Ideally the
input circuitry should be fast enough to fully charge
the sampling capacitor during the sampling period
1/(2FENCODE); however, this is not always possible and the
incomplete settling may degrade the SFDR. The sampling
glitch has been designed to be as linear as possible to
minimize the effects of incomplete settling.
For the best performance, it is recommended to have a
source impedance of 100Ω or less for each input. The
source impedance should be matched for the differential
inputs. Poor matching will result in higher even order
harmonics, especially the second.
Input Drive Circuits
Figure 3 shows the LTC2230/LTC2231 being driven by an
RF transformer with a center tapped secondary. The
secondary center tap is DC biased with VCM, setting the
ADC input signal at its optimum DC level. Terminating on
the transformer secondary is desirable, as this provides a
common mode path for charging glitches caused by the
sample and hold. Figure 3 shows a 1:1 turns ratio trans-
former. Other turns ratios can be used if the source
impedance seen by the ADC does not exceed 100Ω for
each ADC input. A disadvantage of using a transformer is
the loss of low frequency response. Most small RF trans-
formers have poor performance at frequencies below
1MHz.
Figure 4 demonstrates the use of a differential amplifier to
20
convert a single ended input signal into a differential input
signal. The advantage of this method is that it provides low
frequency input response; however, the limited gain band-
width of most op amps will limit the SFDR at high input
frequencies.
Figure 5 shows a single-ended input circuit. The imped-
ance seen by the analog inputs should be matched. This
circuit is not recommended if low distortion is required.
The 25Ω resistors and 12pF capacitor on the analog inputs
serve two purposes: isolating the drive circuitry from the
sample-and-hold charging glitches and limiting the
wideband noise at the converter input. For input frequen-
cies higher than 100MHz, the capacitor may need to be
decreased to prevent excessive signal loss.
0.1μF T1
ANALOG
1:1
INPUT
25Ω
25Ω 0.1μF
25Ω 25Ω
T1 = MA/COM ETC1-1T
RESISTORS, CAPACITORS
ARE 0402 PACKAGE SIZE
VCM
2.2μF
AIN+
AIN+
12pF
AIN–
AIN–
LTC2230/
LTC2231
22301 F03
Figure 3. Single-Ended to Differential
Conversion Using a Transformer
HIGH SPEED
DIFFERENTIAL
AMPLIFIER
25Ω
ANALOG
INPUT
++
3pF
CM
25Ω
AMPLIFIER = LTC6600-20, AD8138, ETC.
VCM
2.2μF
AIN+
AIN+
12pF
AIN–
AIN–
3pF
LTC2230/
LTC2231
22301 F04
Figure 4. Differential Drive with an Amplifier
1k 1k
0.1μF
ANALOG
INPUT
25Ω
25Ω
0.1μF
VCM
2.2μF
AIN+
AIN+
12pF AIN
AIN
LTC2230/
LTC2231
22301 F05
Figure 5. Single-Ended Drive
22301fb

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