IVC102U/2K5 [TI]
精密交换式集成器互阻抗放大器 | D | 14 | -40 to 125;型号: | IVC102U/2K5 |
厂家: | 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 | 下载: | 下载PDF数据表文档文件 |
®
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 1.5kΩ.
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 1GΩ. 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 100MΩ are
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 1.5kΩ series 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 Ω 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
1.5kΩ, the on-resistance of S1. The total input resistance is
the sum of the switch resistance and RIN, or 2.5kΩ in 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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