IVC102U/2K5 [TI]

精密交换式集成器互阻抗放大器 | D | 14 | -40 to 125;
IVC102U/2K5
型号: IVC102U/2K5
厂家: TEXAS INSTRUMENTS    TEXAS INSTRUMENTS
描述:

精密交换式集成器互阻抗放大器 | D | 14 | -40 to 125

放大器 光电二极管
文件: 总16页 (文件大小:250K)
中文:  中文翻译
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®
IVC102  
PRECISION SWITCHED INTEGRATOR  
TRANSIMPEDANCE AMPLIFIER  
DESCRIPTION  
APPLICATIONS  
The IVC102 is a precision integrating amplifier with  
FET op amp, integrating capacitors, and low leakage  
FET switches. It integrates low-level input current for  
a user-determined period, storing the resulting voltage  
on the integrating capacitor. The output voltage can be  
held for accurate measurement. The IVC102 provides  
a precision, lower noise alternative to conventional  
transimpedance op amp circuits that require a very  
high value feedback resistor.  
PRECISION LOW CURRENT MEASUREMENT  
PHOTODIODE MEASUREMENTS  
IONIZATION CHAMBER MEASUREMENTS  
CURRENT/CHARGE-OUTPUT SENSORS  
LEAKAGE CURRENT MEASUREMENT  
FEATURES  
ON-CHIP INTEGRATING CAPACITORS  
The IVC102 is ideal for amplifying low-level sensor  
currents from photodiodes and ionization chambers.  
The input signal current can be positive or negative.  
GAIN PROGRAMMED BY TIMING  
LOW INPUT BIAS CURRENT: 750fA max  
LOW NOISE  
TTL/CMOS-compatible timing inputs control the inte-  
gration period, hold and reset functions to set the  
effective transimpedance gain and to reset (discharge)  
the integrator capacitor.  
LOW SWITCH CHARGE INJECTION  
FAST PULSE INTEGRATION  
Package options include 14-Pin plastic DIP and SO-14  
surface-mount packages. Both are specified for the  
–40°C to 85°C industrial temperature range.  
LOW NONLINEARITY: 0.005% typ  
14-PIN DIP, SO-14 SURFACE MOUNT  
V+  
14  
–1  
C3  
30pF  
60pF  
6
5
4
VO  
=
CINT  
IIN(t) dt  
VB  
C2  
10pF  
Positive or Negative  
Signal Integration  
C1  
Ionization  
Chamber  
S2  
3
2
10  
9
0V  
IIN  
VO  
S1  
Hold  
Integrate  
Hold  
Reset  
1
S1  
S2  
Photodiode  
11  
12  
13  
Analog  
Ground  
V–  
Digital  
Ground  
S1  
S2  
Logic Low closes switches  
InternationalAirportIndustrialPark • MailingAddress:POBox11400 • Tucson,AZ85734 • StreetAddress:6730S.TucsonBlvd. • Tucson,AZ85706  
Tel:(520)746-1111 • Twx:910-952-1111 • Cable:BBRCORP • Telex:066-6491 • FAX:(520)889-1510 • ImmediateProductInfo:(800)548-6132  
PDS-1329A  
© 1996 Burr-Brown Corporation  
P
rin  
ted  
in U.S.A. June, 1996  
SBFS009  
SPECIFICATIONS  
At TA = +25°C, VS = ±15V, RL = 2kΩ, CINT = C1 + C2 + C3, 1ms integration period(1), unless otherwise specified.  
IVC102P, U  
PARAMETER  
CONDITIONS  
MIN  
TYP  
MAX  
UNITS  
TRANSFER FUNCTION  
Gain Error  
vs Temperature  
Nonlinearity  
Input Current Range  
Offset Voltage(2)  
vs Temperature  
vs Power Supply  
Droop Rate, Hold Mode  
VO = –(IIN)(TINT)/CINT  
CINT = C1 + C2 + C3  
±5  
±25  
±0.005  
±100  
–5  
±30  
150  
–1  
+25/–17  
%
ppm/°C  
%
µA  
mV  
µV/°C  
µV/V  
nV/µs  
V
O = ±10V  
IIN = 0, C = 50pF  
±20  
IN  
VS = +4.75/–10 to +18/–18V  
750  
OP AMP  
Input Bias Current  
vs Temperature  
Offset Voltage (Op Amp VOS  
vs Temperature  
vs Power Supply  
Noise Voltage  
S1, S2 Open  
–100  
See Typical Curve  
±750  
±5  
fA  
)
±0.5  
±5  
10  
mV  
µV/°C  
µV/V  
VS = +4.75/–10 to +18/–18V  
f = 1kHz  
100  
10  
nV/Hz  
INTEGRATION CAPACITORS  
C1 + C2 + C3  
80  
100  
±25  
10  
30  
60  
120  
pF  
ppm/°C  
pF  
pF  
pF  
vs Temperature  
C1  
C2  
C3  
OUTPUT  
Voltage Range, Positive  
Negative  
RL = 2kΩ  
RL = 2kΩ  
(V+)–3  
(V–)+3  
(V+)–1.3  
(V–)+2.6  
V
V
Short-Circuit Current  
Capacitive Load Drive  
Noise Voltage  
±20  
500  
mA  
pF  
See Typical Curve  
DYNAMIC CHARACTERISTIC  
Op Amp Gain-Bandwidth  
Op Amp Slew Rate  
Reset  
2
3
MHz  
V/µs  
Slew Rate  
Settling Time, 0.01%  
3
6
V/µs  
µs  
10V Step  
DIGITAL INPUTS  
(TTL/CMOS Compatible)  
(Logic High)  
(Logic Low)  
V
IH (referred to digital ground)  
2
–0.5  
5.5  
0.8  
V
V
VIL (referred to digital ground)  
IIH  
IIL  
VIH = 5V  
VIL = 0V  
2
0
100  
µA  
µA  
ns  
Switching Time  
POWER SUPPLY  
Voltage Range: Positive  
Negative  
Current: Positive  
Negative  
+4.75  
–10  
+15  
–15  
4.1  
–1.6  
–0.2  
–2.3  
+18  
–18  
5.5  
V
V
mA  
mA  
mA  
mA  
–2.2  
Analog Ground  
Digital Ground  
TEMPERATURE RANGE  
Operating Range  
Storage  
–40  
–55  
85  
125  
°C  
°C  
Thermal Resistance, θJA  
DIP  
100  
150  
°C/W  
°C/W  
SO-14  
NOTES: (1) Standard test timing: 1ms integration, 200µs hold, 100µs reset. (2) Hold mode output voltage after 1ms integration of zero input current. Includes op  
amp offset voltage, integration of input error current and switch charge injection effects.  
The information provided herein is believed to be reliable; however, BURR-BROWN assumes no responsibility for inaccuracies or omissions. BURR-BROWN assumes  
no responsibility for the use of this information, and all use of such information shall be entirely at the user’s own risk. Prices and specifications are subject to change  
without notice. No patent rights or licenses to any of the circuits described herein are implied or granted to any third party. BURR-BROWN does not authorize or warrant  
any BURR-BROWN product for use in life support devices and/or systems.  
®
2
IVC102  
ABSOLUTE MAXIMUM RATINGS  
ELECTROSTATIC  
DISCHARGE SENSITIVITY  
This integrated circuit can be damaged by ESD. Burr-Brown  
recommends that all integrated circuits be handled with  
appropriate precautions. Failure to observe proper handling  
and installation procedures can cause damage.  
Supply Voltage, V+ to V– .................................................................... 36V  
Logic Input Voltage...................................................................... V– to V+  
Output Short Circuit to Ground ............................................... Continuous  
Operating Temperature ................................................. –40°C to +125°C  
Storage Temperature ..................................................... –55°C to +125°C  
Lead Temperature (soldering, 10s) ................................................. 300°C  
ESD damage can range from subtle performance degrada-  
tion to complete device failure. Precision integrated circuits  
may be more susceptible to damage because very small  
parametric changes could cause the device not to meet its  
published specifications.  
PIN CONNECTIONS  
Top View  
14-Pin DIP/  
SO-14 Surface Mount  
Analog Ground  
1
2
3
4
5
6
7
14 V+  
IIN  
–In  
C1  
13 Digital Ground  
12 S2  
11 S1  
C2  
10 VO  
C3  
9
8
V–  
NC  
NC  
NC = No Internal Connection  
Connect to Analog Ground for Lowest Noise  
PACKAGE INFORMATION  
PACKAGE DRAWING  
PRODUCT  
PACKAGE  
NUMBER(1)  
IVC102P  
IVC102U  
14-Pin DIP  
SO-14 Surface Mount  
010  
235  
NOTE: (1) For detailed drawing and dimension table, please see end of data  
sheet, or Appendix D of Burr-Brown IC Data Book.  
®
3
IVC102  
TYPICAL PERFORMANCE CURVES  
At TA = +25°C, VS = ±15V, RL = 2kΩ, CINT = C1 + C2 + C3, 1ms integration period, unless otherwise specified.  
INPUT BIAS CURRENT vs TEMPERATURE  
TOTAL OUTPUT NOISE vs CIN  
rms Variation  
100p  
10p  
1p  
1000  
100  
10  
of 100 Measurement  
Cycles, TINT = 1ms.  
CINT = 10pF  
CINT = 30pF  
S1, S2 Open  
CINT = 100pF  
CINT = 300pF  
CINT = 1000pF  
100f  
10f  
Reset Mode, S1 Open, S2 Closed.  
1
–50  
–25  
0
25  
50  
75  
100  
125  
10  
100  
IN (pF)  
1000  
Temperature (°C)  
C
RESET TIME vs CINT  
S1 CHARGE INJECTION vs INPUT CAPACITANCE  
30  
25  
20  
15  
10  
5
2.0  
1.8  
1.6  
1.4  
1.2  
1.0  
0.8  
0.6  
0.4  
0.2  
0
100pF  
Time Required to  
Reset from ±10V  
to 0V.  
S1  
CIN  
0.01%  
Q  
VO  
=
100pF  
1%  
0
0
100 200 300 400 500 600 700 800 900 1000  
INT (pF)  
10  
100  
1000  
C
Input Capacitance, CIN (pF)  
S2 CHARGE INJECTION vs INPUT CAPACITANCE  
(V+) = +18V  
1.0  
0.9  
0.8  
0.7  
0.6  
0.5  
0.4  
0.3  
0.2  
0.1  
0
(V+) = +15V  
(V+) = +4.75V  
S2  
100pF  
CIN  
Q  
VO  
=
100pF  
10  
100  
1000  
Input Capacitance, CIN (pF)  
®
4
IVC102  
BASIC RESET-AND-INTEGRATE MEASUREMENT  
APPLICATION INFORMATION  
Figure 1 shows the circuit and timing for a simple reset-and-  
integrate measurement. The input current is connected di-  
rectly to the inverting input of the IVC102, pin 3. Input  
current is shown flowing out of pin 3, which produces a  
positive-going ramp at VO. Current flowing into pin 3 would  
produce a negative-going ramp.  
Figure 1 shows the basic circuit connections to operate the  
IVC102. Bypass capacitors are shown connected to the  
power supply pins. Noisy power supplies should be avoided  
or decoupled and carefully bypassed.  
The Analog Ground terminal, pin 1, is shown internally  
connected to the non-inverting input of the op amp. This  
terminal connects to other internal circuitry and should be  
connected to ground. Approximately 200µA flows out of  
this terminal.  
A measurement cycle starts by resetting the integrator output  
voltage to 0V by closing S2 for 10µs. Integration of the input  
current begins when S2 opens and the input current begins to  
charge CINT. VO is measured with a sampling a/d converter  
at the end of an integration period, just prior to the next reset  
period. The ideal result is proportional to the average input  
current (or total accumulated charge).  
Digital Ground, pin 13, should be at the same voltage  
potential as analog ground (within 100mV). Analog and  
Digital grounds should be connected at some point in the  
system, usually at the power supply connections to the  
circuit board. A separate Digital Ground is provided so that  
noisy logic signals can be referenced to separate circuit  
board traces.  
Switch S2 is again closed to reset the integrator output to 0V  
before the next integration period.  
This simple measurement arrangement is suited to many  
applications. There are, however, limitations to this basic  
approach. Input current continues to flow through S2 during  
the reset period. This leaves a small voltage on CINT equal  
to the input current times RS2, the on-resistance of S2,  
approximately 1.5k.  
Integrator capacitors C1, C2 and C3 are shown connected in  
parallel for a total CINT = 100pF. The IVC102 can be used  
for a wide variety of integrating current measurements. The  
input signal connections and control timing and CINT value  
will depend on the sensor or signal type and other applica-  
tion details.  
V+  
+15V  
0.1µF  
14  
C3  
30pF  
60pF  
6
Figure 1a  
C2  
10pF  
5
4
C1  
IIN  
S2  
3
2
Photodiode  
Sampling  
A/D  
Converter  
10  
9
VO  
Digital  
Data  
S1  
1
0.1µF  
11  
12  
S2  
13  
–15V  
V–  
Analog  
Ground  
Logic  
High  
(+5V)  
Digital  
Ground  
See timing  
signal below  
Charge Injection  
of S2  
0V  
Figure 1b  
Op Amp VOS  
+
T2  
IIN • RS2  
T1  
VO  
0V  
Integrate  
S2  
(S2 Open)  
10µs  
Reset  
10µs  
Reset  
FIGURE 1. Reset-and Integrate Connections and Timing.  
®
5
IVC102  
In addition, the offset voltage of the internal op amp and  
charge injection of S2 contribute to the voltage on CINT at the  
start of integration.  
measurement from the final sample at T2. Op amp offset  
voltage, charge injection effects and I•RS2 offset voltage on  
S2 are removed with this two-point measurement. The effec-  
tive integration period is the time between the two measure-  
ments, T2-T1.  
Performance of this basic approach can be improved by  
sampling VO after the reset period at T1 and subtracting this  
COMPARISON TO CONVENTIONAL TRANSIMPEDANCE AMPLIFIERS  
With the conventional transimpedance amplifier circuit  
of Figure 2a, input current flows through the feedback  
resistor, RF, to create a proportional output voltage.  
VO is proportional to the integration time, TINT, and  
inversely proportional to the feedback capacitor, CINT  
.
The effective transimpedance gain is TINT /CINT. Ex-  
tremely high gain that would be impractical to achieve  
with a conventional transimpedance amplifier can be  
achieved with small integration capacitor values and/or  
long integration times. For example the IVC102 with  
CINT = 100pF and TINT = 100ms provides an effective  
transimpedance of 1G. A 10nA input current would  
produce a 10V output after 100ms integration.  
VO = –IIN RF  
The transimpedance gain is determined by RF. Very large  
values of RF are required to measure very small signal  
current. Feedback resistor values exceeding 100Mare  
common.  
The IVC102 (Figure 2b) provides a similar function,  
converting an input current to an output voltage. The  
The integrating behavior of the IVC102 reduces noise by  
averaging the input noise of the sensor, amplifier, and  
external sources.  
input current flows through the feedback capacitor, CINT  
,
charging it at a rate that is proportional to the input  
current. With a constant input current, the IVC102’s  
output voltage is  
VO = –IIN TINT/CINT  
after an integration time of TINT  
.
Conventional Transimpedance Amplifier  
Figure 2a  
Integrating Transimpedance Amplifier  
Figure 2b  
IIN  
IIN  
CINT  
RF  
VO  
VO  
–1  
VO  
=
CINT  
IIN(t) dt  
VO = –IIN RF  
for constant IIN, at the end of TINT  
Provides time-continuous output  
TINT  
VO = –IIN  
CINT  
voltage proportional to IIN  
.
Output voltage after integration period is  
proportional to average IIN throughout  
the period.  
FIGURE 2. Comparison to a Conventional Transimpedance Amplifier.  
CURRENT-OUTPUT SENSORS  
Figure 3 shows a model for many current-output sensors  
such as photodiodes and ionization chambers. Sensor output  
is a signal-dependent current with a very high source resis-  
tance. The output is generally loaded into a low impedance  
so that the terminal voltage is kept very low. Typical sensor  
capacitance values range from 10pF to over 100pF. This  
capacitance plays a key role in operation of the switched-  
input measurement technique (see next section).  
®
6
IVC102  
V+  
+15V  
0.1µF  
14  
C3  
60pF  
6
5
4
3a  
C2  
10pF  
30pF  
C1  
S2  
Photodiode  
Sensor  
3
2
10  
9
VO  
I
R
C
Digital  
Data  
A/D  
Converter  
S1  
1
0.1µF  
11  
S1  
12  
S2  
13  
–15V  
V–  
I: Signal - Dependent Current  
R: Sensor Resistance  
C: Sensor Capacitance  
See timing  
signals below  
Effective  
Signal Integration  
Period, TS  
A
3b  
0V  
0V  
VO waveform with  
approx. half-scale input current.  
Charge transferred  
from sensor C  
VO  
B
to CINT  
.
(S1 Open)  
(S1 Closed)  
(S2 Open)  
S1  
S2  
10µs  
10µs  
10µs  
10µs  
10µs  
Hold Reset Pre-Int.  
Hold  
Hold Reset  
+10mV  
VO waveform with  
zero input current.  
Op Amp  
VOS  
Transfer Function  
Offset Voltage  
3c  
0V  
VO  
0V  
A
Ramp due to  
input bias current  
(exaggerated).  
Q  
S1 Closing  
Q  
S1 Opening  
–10mV  
Q  
S2 Opening  
B
FIGURE 3. Switched-Input Measurement Technique.  
SWITCHED-INPUT MEASUREMENT TECHNIQUE  
Input connections and timing are shown in Figure 3.  
While the basic reset-and-integrate measurement arrange-  
ment in Figure 1 is satisfactory for many applications, the  
switched-input timing technique shown in Figure 3 has  
important advantages. This method can provide continuous  
integration of the input signal. Furthermore, it can hold the  
output voltage constant after integration for stable conver-  
sion (desirable for a/d converter without a sample/hold).  
The timing diagram, Figure 3b, shows that S1 is closed only  
when S2 is open. During the short period that S1 is open  
(30µs in this timing example), any signal current produced  
by the sensor will charge the sensor’s source capacitance.  
This charge is then transferred to CINT when S1 is closed. As  
a result, no charge produced by the sensor is lost and the  
input signal is continuously integrated. Even fast input  
pulses are accurately integrated.  
®
7
IVC102  
The input current, IIN, is shown as a conventional current  
flowing into pin 2 in this diagram but the input current could  
be bipolar (positive or negative). Current flowing out of pin  
2 would produce a positive-ramping VO.  
OFFSET ERRORS  
Figure 3c shows the effect on VO due to op amp input offset  
voltage, input bias current and switch charge injection. It  
assumes zero input current from the sensor. The various  
offsets and charge injection (Q) jumps shown are typical of  
that seen with a 50pF source capacitance. The specified  
“transfer function offset voltage” is the voltage measured  
during the hold period at B. Transfer function offset voltage  
is dominated by the charge injection of S2 opening and op  
amp VOS. The opening and closing charge injections of S1  
are very nearly equal and opposite and are not significant  
contributors.  
The timing sequence proceeds as follows:  
Reset Period  
The integrator is reset by closing switch S2 with S1 open. A  
10µs reset time is recommended to allow the op amp to slew  
to 0V and settle to its final value.  
Pre-Integration Hold  
S2 is opened, holding VO constant for 10µs prior to integra-  
tion. This pre-integration hold period assures that S2 is fully  
open before S1 is closed so that no input signal is lost. A  
minimum of 1µs is recommended to avoid switching over-  
lap. The 10µs hold period shown in Figure 3b also allows an  
a/d converter measurement to be made at point A. The  
purpose of this measurement at A is discussed in the “Offset  
Errors” section.  
Note that using a two-point difference measurement at A  
and B can dramatically reduce offset due to op amp VOS and  
S2 charge injection. The remaining offset with this B-A  
measurement is due to op amp input bias current charging  
CINT. This error is usually very small and is exaggerated in  
the figure.  
Integration on CINT  
DIGITAL SWITCH INPUTS  
Integration of the input current on CINT begins when S1 is  
closed. An immediate step output voltage change occurs as  
the charge that was stored on the input sensor capacitance is  
transferred to CINT. Although this period of charging CINT  
occurs only while S1 is closed, the charge transferred as S1  
is closed causes the effective integration time to be equal to  
the complete conversion period—see Figure 3b.  
The digital control inputs to S1 and S2 are compatible with  
standard CMOS or TTL logic. Logic input pins 11 and 12  
are high impedance and the threshold is approximately 1.4V  
relative to Digital Ground, pin 13. A logic “low” closes the  
switch.  
Use care in routing these logic signals to their respective  
input pins. Capacitive coupling of logic transitions to sensi-  
tive input nodes (pins 2 through 6) and to the positive power  
supply (pin 14) will dramatically increase charge injection  
and produce errors. Route these circuit board traces over a  
ground plane (digital ground) and route digital ground traces  
between logic traces and other critical traces for lowest  
charge injection. See Figure 4.  
The integration period could range from 100µs to many  
minutes, depending on the input current and CINT value.  
While S1 is closed, IIN charges CINT, producing a negative-  
going ramp at the integrator output voltage, VO. The output  
voltage at the end of integration is proportional to the  
average input current throughout the complete conversion  
cycle, including the integration period, reset and both hold  
periods.  
5V logic levels are generally satisfactory. Lower voltage  
logic levels may help reduce charge injection errors, de-  
pending on circuit layout. Logic high voltages greater than  
5.5V, or higher than the V+ supply are not recommended.  
Hold Period  
Opening S1 halts integration on CINT. Approximately 5µs  
after S1 is opened, the output voltage is stable and can be  
measured (at point B). The hold period is 10µs in this  
example. CINT remains charged until a S2 is again closed, to  
reset for the next conversion cycle.  
Analog  
V+  
Input trace guarded  
all the way to sensor.  
Ground  
Switch logic inputs  
guarded by digital  
ground.  
In this timing example, S1 is open for a total of 30µs. During  
this time, signal current from the sensor charges the sensor  
source capacitance. Care should be used to assure that the  
voltage developed on the sensor does not exceed approxi-  
mately 200mV during this time. The IIN terminal, pin 2, is  
internally clamped with diodes. If these diodes forward bias,  
signal current will flow to ground and will not be accurately  
integrated.  
1
14  
Digital  
Ground  
S2  
S1  
Input nodes  
guarded by  
analog ground.  
A maximum of 333nA signal current could be accurately  
integrated on a 50pF sensor capacitance for 30µs before  
200mV would be developed on the sensor.  
7
8
VO  
IMAX = (50pF) (200mV)/30µs = 333nA  
Pins 7 and 8 have no internal  
connection but are connected to  
ground for lowest noise pickup.  
V–  
FIGURE 4. Circuit Board Layout Techniques.  
®
8
IVC102  
INPUT BIAS CURRENT ERRORS  
CHOOSING CINT  
Careful circuit board layout and assembly techniques are  
required to achieve the very low input bias current capability  
of the IVC102. The critical input connections are at ground  
potential, so analog ground should be used as a circuit board  
guard trace surrounding all critical nodes. These include  
pins 2, 3, 4, 5 and 6. See Figure 4.  
Internal capacitors C1, C2 and C3 are high quality metal/  
oxide types with low leakage and excellent dielectric char-  
acteristics. Temperature stability is excellent—see typical  
curve. They can be connected for CINT = 10pF, 30pF, 40pF,  
60pF, 70pF, 90pF or 100pF. Connect unused internal ca-  
pacitor pins to analog ground. Accuracy is ±20%, which  
directly influences the gain of the transfer function.  
Input bias current increases with temperature—see typical  
performance curve Input Bias Current vs Temperature.  
A larger value external CINT can be connected between pins  
3 and 10 for slower/longer integration. Select a capacitor  
type with low leakage and good temperature stability.  
Teflon , polystyrene or polypropylene capacitors generally  
provide excellent leakage, temperature drift and voltage  
coefficient characteristics. Lower cost types such as NPO  
ceramic, mica or glass may be adequate for many applica-  
tions. Larger values for CINT require a longer reset time—see  
typical curves.  
HOLD MODE DROOP  
Hold-mode droop is a slow change in output voltage prima-  
rily due to op amp input bias current. Droop is specified  
using the internal CINT = 100pF and is based on a –100fA  
typical input bias current. Current flows out of the inverting  
input of the internal op amp.  
–100fA  
Droop Rate =  
CINT  
FREQUENCY RESPONSE  
Integration of the input signal for a fixed period produces a  
deep null (zero response) at the frequency 1/TINT and its  
harmonics. An ac input current at this frequency (or its  
harmonics) has zero average value and therefore produces  
no output. This property can be used to position response  
nulls at critical frequencies. For example, a 16.67ms integra-  
tion period produces response nulls at 60Hz, 120Hz, 180Hz,  
etc., which will reject ac line frequency noise and its har-  
monics. Response nulls can be positioned to reduce interfer-  
ence from system clocks or other periodic noise.  
With CINT = 100pF, the droop rate is typically only  
1nV/µs—slow enough that it rarely contributes significant  
error at moderate temperatures.  
Since the input bias current increases with temperature, the  
droop rate will also increase with temperature. The droop  
rate will approximately double for each 10°C increase in  
junction temperature—see typical curves.  
Droop rate is inversely proportional to CINT. If an external  
integrator capacitor is used, a low leakage capacitor should  
be selected to preserve the low droop performance of the  
IVC102.  
Response to all frequencies above f = 1/TINT falls at –20dB/  
decade. The effective corner frequency of this single-pole  
response is approximately 1/2.8TINT  
.
For the simple reset-and-integrate measurement technique,  
TINT is equal to the to the time that S2 is open. The switched-  
input technique, however, effectively integrates the input  
signal throughout the full measurement cycle, including the  
reset period and both hold periods. Using the timing shown  
in Figure 3, the effective integration time is 1/Ts, where Ts  
is the repetition rate of the sampling.  
INPUT CURRENT RANGE  
Extremely low input currents can be measured by integrat-  
ing for long periods and/or using a small value for CINT  
Input bias current of the internal op amp is the primary  
source of error.  
.
Larger input currents can be measured by increasing the  
value of CINT and/or using a shorter integration time. Input  
currents greater than 200µA should not be applied to the pin  
2 input, however. The approximately 1.5kseries resistance  
of S1 will create an input voltage at pin 2 that will begin to  
forward-bias internal protection clamp diodes. Any current  
that flows through these protection diodes will not be accu-  
rately integrated. See “Input Impedance” section for more  
information on input current-induced voltage.  
INPUT IMPEDANCE  
The input impedance of a perfect transimpedance circuit is  
zero ohms. The input voltage ideally would be zero for any  
input current. The actual input voltage when directly driving  
the integrator input (pin 3) is proportional to the output slew  
rate of the integrator. A 1V/µs slew rate produces approxi-  
mately 100mV at pin 3. The input of the integrator can be  
modeled as a resistance:  
Input current greater than 200µA can, however, be con-  
nected directly to pin 3, using the simple reset-integrate  
technique shown in Figure 1. Current applied at this input  
can be externally switched to avoid excessive I•R voltage  
across S2 during reset. Inputs up to 5mA at pin 3 can be  
accurately integrated if CINT is made large enough to limit  
slew rate to less than 1V/µs. A 5mA input current would  
require CINT = 5nF to produce a 1V/µs slew rate. The input  
current appears as load current to the internal op amp,  
reducing its ability to drive an external load.  
RIN = 10–7/CINT  
(2)  
with RIN in and CINT in Farads.  
(3)  
Using the internal CINT = C1 + C2 + C3 = 100pF  
RIN = 10–7/100pF = 1kΩ  
Teflon E. I. Du Pont de Nemours & Co.  
®
9
IVC102  
Slew rate limit of the internal op amp is approximately  
3V/µs. For most applications, the slew rate of VOUT should  
be limited to 1V/µs or less. The rate of change is propor-  
0
–10  
–20  
–30  
–40  
–50  
tional to IIN and inversely proportional to CINT  
:
–20dB/decade  
slope  
Corner at  
f = 0.32/TINT  
IIN  
Slew Rate =  
CINT  
–3dB at  
f = 0.44/TINT  
This can be important in some applications since the slew-  
induced input voltage is applied to the sensor or signal  
source. The slew-induced input voltage can be reduced by  
increasing CINT, which reduces the output slew rate.  
● ● ●  
1/10TINT  
1/TINT  
Frequency  
10/TINT  
NONLINEARITY  
Careful nonlinearity measurements of the IVC102 yield  
typical results of approximately ±0.005% using the internal  
input capacitors (CINT = 100pF). Nonlinearity will be de-  
graded by using an external integrator capacitor with poor  
voltage coefficient. Performance with the internal capacitors  
is typically equal or better than the sensors it is used to  
measure. Actual application circuits with sensors such as a  
photodiode may have other sources of nonlinearity.  
FIGURE 5. Frequency Response of Integrating Converter.  
The input resistance seen at pin 2 includes an additional  
1.5k, the on-resistance of S1. The total input resistance is  
the sum of the switch resistance and RIN, or 2.5kin this  
example.  
®
10  
IVC102  
PACKAGE OPTION ADDENDUM  
www.ti.com  
10-Dec-2020  
PACKAGING INFORMATION  
Orderable Device  
Status Package Type Package Pins Package  
Eco Plan  
Lead finish/  
Ball material  
MSL Peak Temp  
Op Temp (°C)  
Device Marking  
Samples  
Drawing  
Qty  
(1)  
(2)  
(3)  
(4/5)  
(6)  
IVC102U  
ACTIVE  
ACTIVE  
SOIC  
SOIC  
D
D
14  
14  
50  
RoHS & Green  
NIPDAU  
Level-3-260C-168 HR  
Level-3-260C-168 HR  
-40 to 125  
-40 to 125  
IVC102U  
IVC102U  
IVC102U/2K5  
2500 RoHS & Green  
NIPDAU  
(1) The marketing status values are defined as follows:  
ACTIVE: Product device recommended for new designs.  
LIFEBUY: TI has announced that the device will be discontinued, and a lifetime-buy period is in effect.  
NRND: Not recommended for new designs. Device is in production to support existing customers, but TI does not recommend using this part in a new design.  
PREVIEW: Device has been announced but is not in production. Samples may or may not be available.  
OBSOLETE: TI has discontinued the production of the device.  
(2) RoHS: TI defines "RoHS" to mean semiconductor products that are compliant with the current EU RoHS requirements for all 10 RoHS substances, including the requirement that RoHS substance  
do not exceed 0.1% by weight in homogeneous materials. Where designed to be soldered at high temperatures, "RoHS" products are suitable for use in specified lead-free processes. TI may  
reference these types of products as "Pb-Free".  
RoHS Exempt: TI defines "RoHS Exempt" to mean products that contain lead but are compliant with EU RoHS pursuant to a specific EU RoHS exemption.  
Green: TI defines "Green" to mean the content of Chlorine (Cl) and Bromine (Br) based flame retardants meet JS709B low halogen requirements of <=1000ppm threshold. Antimony trioxide based  
flame retardants must also meet the <=1000ppm threshold requirement.  
(3) MSL, Peak Temp. - The Moisture Sensitivity Level rating according to the JEDEC industry standard classifications, and peak solder temperature.  
(4) There may be additional marking, which relates to the logo, the lot trace code information, or the environmental category on the device.  
(5) Multiple Device Markings will be inside parentheses. Only one Device Marking contained in parentheses and separated by a "~" will appear on a device. If a line is indented then it is a continuation  
of the previous line and the two combined represent the entire Device Marking for that device.  
(6)  
Lead finish/Ball material - Orderable Devices may have multiple material finish options. Finish options are separated by a vertical ruled line. Lead finish/Ball material values may wrap to two  
lines if the finish value exceeds the maximum column width.  
Important Information and Disclaimer:The information provided on this page represents TI's knowledge and belief as of the date that it is provided. TI bases its knowledge and belief on information  
provided by third parties, and makes no representation or warranty as to the accuracy of such information. Efforts are underway to better integrate information from third parties. TI has taken and  
continues to take reasonable steps to provide representative and accurate information but may not have conducted destructive testing or chemical analysis on incoming materials and chemicals.  
TI and TI suppliers consider certain information to be proprietary, and thus CAS numbers and other limited information may not be available for release.  
In no event shall TI's liability arising out of such information exceed the total purchase price of the TI part(s) at issue in this document sold by TI to Customer on an annual basis.  
Addendum-Page 1  
PACKAGE OPTION ADDENDUM  
www.ti.com  
10-Dec-2020  
Addendum-Page 2  
PACKAGE MATERIALS INFORMATION  
www.ti.com  
3-Jun-2022  
TAPE AND REEL INFORMATION  
REEL DIMENSIONS  
TAPE DIMENSIONS  
K0  
P1  
W
B0  
Reel  
Diameter  
Cavity  
A0  
A0 Dimension designed to accommodate the component width  
B0 Dimension designed to accommodate the component length  
K0 Dimension designed to accommodate the component thickness  
Overall width of the carrier tape  
W
P1 Pitch between successive cavity centers  
Reel Width (W1)  
QUADRANT ASSIGNMENTS FOR PIN 1 ORIENTATION IN TAPE  
Sprocket Holes  
Q1 Q2  
Q3 Q4  
Q1 Q2  
Q3 Q4  
User Direction of Feed  
Pocket Quadrants  
*All dimensions are nominal  
Device  
Package Package Pins  
Type Drawing  
SPQ  
Reel  
Reel  
A0  
B0  
K0  
P1  
W
Pin1  
Diameter Width (mm) (mm) (mm) (mm) (mm) Quadrant  
(mm) W1 (mm)  
IVC102U/2K5  
SOIC  
D
14  
2500  
330.0  
16.4  
6.5  
9.0  
2.1  
8.0  
16.0  
Q1  
Pack Materials-Page 1  
PACKAGE MATERIALS INFORMATION  
www.ti.com  
3-Jun-2022  
TAPE AND REEL BOX DIMENSIONS  
Width (mm)  
H
W
L
*All dimensions are nominal  
Device  
Package Type Package Drawing Pins  
SOIC 14  
SPQ  
Length (mm) Width (mm) Height (mm)  
356.0 356.0 35.0  
IVC102U/2K5  
D
2500  
Pack Materials-Page 2  
PACKAGE MATERIALS INFORMATION  
www.ti.com  
3-Jun-2022  
TUBE  
T - Tube  
height  
L - Tube length  
W - Tube  
width  
B - Alignment groove width  
*All dimensions are nominal  
Device  
Package Name Package Type  
SOIC  
Pins  
SPQ  
L (mm)  
W (mm)  
T (µm)  
B (mm)  
IVC102U  
D
14  
50  
506.6  
8
3940  
4.32  
Pack Materials-Page 3  
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IMPLIED WARRANTIES OF MERCHANTABILITY, FITNESS FOR A PARTICULAR PURPOSE OR NON-INFRINGEMENT OF THIRD  
PARTY INTELLECTUAL PROPERTY RIGHTS.  
These resources are intended for skilled developers designing with TI products. You are solely responsible for (1) selecting the appropriate  
TI products for your application, (2) designing, validating and testing your application, and (3) ensuring your application meets applicable  
standards, and any other safety, security, regulatory or other requirements.  
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is granted to any other TI intellectual property right or to any third party intellectual property right. TI disclaims responsibility for, and you  
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