ST TSH330 User Manual

TSH330
1.1 GHz Low-Noise Operational Amplifier
Bandwidth: 1.1GHz (Gain=+2)
Quiescent current: 16.6 mA
Slew rate: 1800V/µs
Input noise: 1.3nV/Hz
Distortion: SFDR = -78dBc (10MHz, 2Vp-p)
Output stage optimized for driving 100
loads
Description
The TSH330 is a current feedback operational amplifier using a very high-speed complementary technology to provide a large bandwidth of
1.1GHz in gain of 2 while drawing only 16.6mA of quiescent current. In addition, the TSH330 offers
0.1dB gain flatness up to 160MHz with a gain of 2. With a slew rate of 1800V/µs and an output stage optimized for driving a standard 100 load, this device is highly suitable for applications where speed and low-distortion are the main requirements.
The TSH330 is a single operator available in the SO8 plastic package, saving board space as well as providing excellent thermal and dynamic performances.
Pin Connections (top view)
D
SO-8
(Plastic Micropackage)
1
NC
-IN
+IN
-VCC
2
3
4
_
+
SO8
NC
8
7
+VCC
6NCOutput
5
Applications
Communication & video test equipment
Medical instrumentation
ADC drivers
Order Codes
Part Number Temperature Range Package Conditioning Marking
TSH330ID
TSH330IDT SO8 Tape&Reel TSH330I
June 2005 Revision 3 1/19
-40°C to +85°C
SO8 Tube TSH330I
TSH330 Absolute Maximum Ratings

1 Absolute Maximum Ratings

Table 1. Key parameters and their absolute maximum ratings
Symbol Parameter Value Unit
V
T
T
R R P
Supply Voltage
CC
V
Differential Input Voltage
id
V
Input Voltage Range
in
Operating Free Air Temperature Range
oper
Storage Temperature
stg
Maximum Junction Temperature
T
j
SO8 Thermal Resistance Junction to Ambient 60 °C/W
thja
SO8 Thermal Resistance Junction to Case 28 °C/W
thjc
SO8 Maximum Power Dissipation4 (@Ta=25°C) for Tj=150°C
max
HBM: Human Body Model HBM: Human Body Model (pins 2 and 3) 0.6 kV
ESD
MM: Machine Model MM: Machine Model (pins 2 and 3) 80 V CDM: Charged Device Model (pins 1, 4, 5, 6, 7 and 8) 1.5 kV CDM: Charged Device Model (pins 2 and 3) 1 kV Latch-up Immunity 200 mA
1) All voltages values are measured with respect to the ground pin.
2) Differential voltage are non-inverting input terminal with respect to the inverting input terminal.
3) The magnitude of input and output voltage must never exceed VCC +0.3V.
4) Short-circuits can cause excessive heating. Destructive dissipation can result from short circuit on amplifiers.
5) Human body model, 100pF discharged through a 1.5kresistor into pMin of device.
6) This is a minimum Value. Machine model ESD, a 200pF cap is charged to the specified voltage, then discharged directly into the IC with
no external series resistor (internal resistor < 5), into pin to pin of device.
1
2
3
5
(pins 1, 4, 5, 6, 7 and 8)
6
(pins 1, 4, 5, 6, 7 and 8)
6V +/-0.5 V +/-2.5 V
-40 to + 85 °C
-65 to +150 °C 150 °C
830 mW
2kV
200 V
Table 2. Operating conditions
Symbol Parameter Value Unit
V V
1) Tested in full production at 5V (±2.5V) supply voltage.
Supply Voltage
CC
Common Mode Input Voltage
icm
2/19
1
4.5 to 5.5 V
-Vcc+1.5V, +Vcc-1.5V V
Electrical Characteristics TSH330

2 Electrical Characteristics

Table 3. Electrical characteristics for VCC= ±2.5Volts, T
=+25°C (unless otherwise specified)
amb
Symbol Parameter Test Condition Min. Typ. Max. Unit
DC performance
V
io
V
I
ib+
I
ib-
CMR
SVR
PSR
ICC
Input Offset Voltage
Offset Voltage between both inputs
Vio drift vs. Temperature T
io
Non Inverting Input Bias Current
DC current necessary to bias the input +
Inverting Input Bias Current
DC current necessary to bias the input -
Common Mode Rejection Ratio
20 log
(∆Vic/∆Vio)
Supply Voltage Rejection Ratio
20 log
(∆Vcc/∆V
out
)
Power Supply Rejection Ratio
20 log
(∆Vcc/∆V
out
)
Supply Current
DC consumption with no input signal
T
amb
T
< T < T
< T
< T
amb
amb
amb
amb
< T < T
< T
< T
max.
max.
max.
max.
min.
min.
T
amb
T
min.
T
amb
T
min.
Vic = ±1V T
< T
amb
< T
max.
min.
Vcc= 3.5V to 5V
< T
T
min.
amb
< T
max.
Vcc=200mVp-p@1kHz
< T
T
min.
amb
< T
max.
-3.1 0.18 +3.1
0.8
1.6 µV/°C
26 55 21
722
13
50 54
54
63 74
67 56
52 No load 16.6 20.2 mA T
< T
min.
amb
< T
max.
16.6 mA
Dynamic performance and output characteristics
R
Bw
SR
V
V
Transimpedance
Output Voltage/Input Current Gain in open loop of a CFA.
OL
For a VFA, the analog of this feature is the Open Loop Gain (A
VD
)
-3dB Bandwidth
Frequency where the gain is 3dB below the DC gain A
Note: Gain Bandwidth Product criterion is
V
not applicable for Current-Feedback­Amplifiers
Gain Flatness @ 0.1dB
Band of frequency where the gain varia­tion does not exceed 0.1dB
Slew Rate
Maximum output speed of sweep in large signal
High Level Output Voltage RL = 100
OH
Low Level Output Voltage RL = 100
OL
= ±1V, RL = 100
V
out
< T
T
min.
out=20mVp-p, RL = 100
V
= +1
A
V
= +2
A
V
amb
< T
max.
AV = -4
= -4, T
A
V
Small Signal V
= +2, RL = 100
A
V
= 2Vp-p, AV = +2,
V
out
min.
< T
amb
=20mVp-p
out
< T
RL = 100
< T
< T
amb
amb
< T
< T
max.
max.
T
min.
T
min.
104 153 k
152 k
1500 1100
550
max.
630 600
160
1800 V/µs
1.5 1.64 V
1.54
-1.55 -1.5 V
-1.5
mV
µA
µA
dB
dB
dB
MHz
3/19
TSH330 Electrical Characteristics
Table 3. Electrical characteristics for VCC= ±2.5Volts, T
=+25°C (unless otherwise specified)
amb
Symbol Parameter Test Condition Min. Typ. Max. Unit
I
Isink
out
Short-circuit Output current coming in the op-amp.
Output to GND 360 453
< T
T
min.
amb
< T
max.
427
See fig-17 for more details
Isource
Output current coming out from the op­amp.
Output to GND -340 -400
< T
T
min.
amb
< T
max.
-350
See fig-18 for more details
Noise and distortion
eN
iN
SFDR
Equivalent Input Noise Voltage
see application note on page 13
Equivalent Input Noise Current (+)
see application note on page 13
Equivalent Input Noise Current (-)
see application note on page 13
Spurious Free Dynamic Range
The highest harmonic of the output spectrum when injecting a filtered sine wave
F = 100kHz
F = 100kHz
F = 100kHz
= +2, Vout = 2Vp-p,
A
V
= 100
R
L
F = 10MHz F = 20MHz F = 100MHz F = 150MHz
1.3 nV/Hz
22 pA/Hz
16 pA/Hz
-78
-73
-48
-37
Table 4. Closed-loop gain and feedback components
mA
dBc
V
CC
(V)
Gain
Rfb (Ω)
-3dB Bw (MHz) 0.1dB Bw (MHz)
+10 200 280 50
-10 200 270 45
+2 300 1000 160
±2.5
-2 270 530 180
+1 300 1500 38
-1 260 600 280
4/19
Electrical Characteristics TSH330
Figure 1. Frequency response, positive gain
24 22 20 18 16 14 12 10
8 6 4
Gain (dB)
2 0
-2
-4
Small Signal
-6
Vcc=5V
-8
Load=100
-10 1M 10M 100M 1G
Gain=+10
Gain=+4
Gain=+2
Gain=+1
Frequency (Hz)
Figure 2. Gain flatness, gain=+4
12,2
12,0
11,8
11,6
Gain Flatness (dB)
11,4
Vin
Vin
8k2
8k2
22pF
22pF
Gain=+4, Vcc=5V,
Gain=+4, Vcc=5V, Small Signal
Small Signal
1M 10M 100M
+
+
-
-
100R
100R
300R
300R
Vout
Vout
Frequency (Hz)
Figure 4. Frequency response, negative gain
24 22 20 18 16 14 12 10
8 6 4
Gain (dB)
2 0
-2
-4
Small Signal
-6
Vcc=5V
-8
Load=100
-10 1M 10M 100M 1G
Gain=-10
Gain=-4
Gain=-2
Gain=-1
Frequency (Hz)
Figure 5. Gain flatness, gain=+2
6,2
6,0
Vin
Vin
+
+
Vout
5,8
8k2
8k2 1pF
Gain Flatness (dB)
1pF
5,6
Gain=+2, Vcc=5V,
Gain=+2, Vcc=5V, Small Signal
Small Signal
5,4
1M 10M 100M 1G
-
-
300R
300R
300R
300R
Vout
Frequency (Hz)
Figure 3. Compensation, gain=+2
10
8 6 4 2 0
-2
-4
-6
Vin
Vin
-8
Gain (dB)
-10
8k2
8k2
-12
1pF
1pF
-14
-16
-18
Gain=+ 2, Vcc=5V,
Gain=+ 2, Vcc=5V, Small Signal
Small Signal
-20
-22 1M 10M 100M 1G
+
+
-
-
300R
300R
300R
300R
Frequency (Hz)
Vout
Vout
Figure 6. Compensation, gain=+4
16 14 12 10
8 6 4 2
Vin
Vin
0
-2
Gain (dB)
-4
8k2
8k2
-6
22pF
22pF
-8
-10
-12
Gain=+4, Vcc=5V,
Gain=+4, Vcc=5V,
-14
Small Signal
Small Signal
-16 1M 10M 100M 1G
+
+
-
-
100R
100R
300R
300R
Vout
Vout
Frequency (Hz)
5/19
TSH330 Electrical Characteristics
Figure 7. Compensation, gain=+10
24 22 20 18 16 14 12 10
Vin
Vin
8 6
Gain (dB)
4
15pF
15pF
2 0
-2
Gain=+10, Vcc=5V,
Gain=+10, Vcc=5V,
-4
Small Signal
Small Signal
-6
-8 1M 10M 100M 1G
22R
22R
+
+
-
-
200R
200R
Vout
Vout
Frequency (Hz)
Figure 8. Input current noise vs. frequency
150 140 130 120 110 100
90 80 70
(pA/VHz)
60
n
i
50 40 30 20 10
Neg. Current Noise
Pos. Current Nois e
1k 10k 100k 1M 10M
Frequency (Hz)
Figure 10. Quiescent current vs. Vcc
20
15
10
5
0
-5
-10
Icc (mA)
-15
-20
Gain=+2 Vcc=5V
-25
Input to ground, no load
-30 1,25 1,50 1,75 2,00 2,25 2,50
Icc(+)
Icc(-)
+/-Vcc (V)
Figure 11. Input voltage noise vs. frequency
4.0
3.5
3.0
2.5
(nV/VHz)
n
e
2.0
1.5
1.0 1k 10k 100k 1M 10M
Frequency (Hz)
Figure 9. Output amplitude vs. load
4,0
3,5
3,0
Vout max. (Vp-p)
2,5
2,0
10 100 1k 10k 100k
6/19
Load (ohms)
Freq=? Gain=+2 Vcc=5V
Figure 12. Noise figure
40
35
30
25
20
NF (dB)
15
10
5
0
1 10 100 1k 10k 100k
Rsource (ohms)
Vcc=5V
Electrical Characteristics TSH330
Figure 13. Output amplitude vs. frequency
5
4
3
2
Vout max. (Vp-p)
1
Gain=+2 Vcc=5V Load=100
0
1M 10M 100M 1G
Frequency (Hz)
Figure 14. Distortion vs. amplitude
-20
-25
-30
-35
-40
-45
-50
-55
-60
-65
HD2
-70
-75
HD2 & HD3 (dBc)
-80
-85
HD3
-90
-95
-100 01234
Output Amplitude (Vp-p)
Gain=+2 Vcc=5V F=10MHz Load=100
Figure 16. Distortion vs. amplitude
-20
-25
-30
-35
-40
-45
-50
HD2
-55
-60
-65
-70
-75
HD2 & HD3 (dBc)
-80
-85
-90
HD3
-95
-100 01234
Output Amplitude (Vp-p)
Gain=+2 Vcc=5V F=30MHz
Load=100
Figure 17. Isink
600
550
500
-1V
-1V
450
400
350
300
250
Isink (mA)
200
150
100
50
0
-2,0 -1,5 -1,0 -0,5 0,0
+
+
_
_
RG
RG
+2.5V
+2.5V
VOL
VOL
without load
without load
-2.5V
-2.5V
Amplifier in open
Amplifier in open loop without load
loop without load
Isink
Isink
V
V
V (V)
Figure 15. Distortion vs. amplitude
-20
-25
-30
-35
-40
-45
-50
HD2
-55
-60
-65
-70
-75
HD2 & HD3 (dBc)
-80
-85
HD3
-90
-95
-100 01234
Output Amplitude (Vp-p)
Gain=+2 Vcc=5V F=20MHz Load=100
Figure 18. Isource
0
-50
-100
-150
-200
-250
-300
-350
Isource (mA)
-400
-450
-500
-550
-600 0,0 0,5 1,0 1,5 2,0
+1V
+1V
V (V)
+
+
_
_
RG
RG
+2.5V
+2.5V
VOH
VOH
without load
without load
Isour ce
Isour ce
-2.5V
-2.5V
Amplifier in open
Amplifier in open loop without load
loop without load
V
V
7/19
TSH330 Electrical Characteristics
Figure 19. Slew rate
2,0
1,5
1,0
0,5
Output Response (V)
Gain=+2
0,0
-2ns -1ns 0s 1ns 2ns 3ns
Vcc=5V Load=100
Time (ns)
Figure 20. Reverse isolation vs. frequency
0
-20
-40
Figure 22. CMR vs. temperature
64
62
60
58
56
54
CMR (dB)
52
50
Gain=+1
48
Vcc=5V
46
Load=100
-40 -20 0 20 40 60 80 100 120
Temperature (°C)
Figure 23. SVR vs. temperature
85
80
75
70
-60
Gain (dB)
-80
Small Signal Vcc=5V Load=100
-100 1M 10M 100M 1G
Frequency (Hz)
Figure 21. Bandwidth vs. temperature
1,3
1,2
1,1
1,0
0,9
Bw (GHz)
0,8
0,7
Gain=+2
0,6
Vcc=5V
Load=100
0,5
-40-20 0 20406080100120
Temperature (°C)
65
SVR (dB)
60
Gain=+1
55
Vcc=5V
Load=100
50
-40 -20 0 20 40 60 80 100 120
Temperature (°C)
Figure 24. ROL vs. temperature
200
180
160
(M)
OL
140
R
120
Open Loop Vcc=5V
100
-40 - 20 0 20 40 60 80 100 120
Temperature (°C)
8/19
Electrical Characteristics TSH330
V
(micro
V)
Figure 25. I-bias vs. temperature
24
22
20
18
16
(µA)
14
BIAS
I
12
10
8
6
Ib(+)
Ib(-)
Gain=+1 Vcc=5V Load=100
-40-20 0 20406080100120
Temperature (°C)
Figure 26. Vio vs. temperature
1000
800
600
IO
400
200
Open Loop Vcc=5V
Load=100
0
-40 -20 0 20 40 60 80 100 120
Temperature (°C)
Figure 28. Icc vs. temperature
20
15
10
5
0
-5
(mA)
-10
CC
I
-15
-20
Gain=+1
-25
Vcc=5V no Load
-30
In+/In- to GND
-35
-40 -20 0 20 40 60 80 100 120
Icc(+)
Icc(-)
Figure 29. Iout vs. temperature
600
400
200
-200
Iout (mA)
-400
-600
-800
Isource
0
Isink
Output: short-circuit Gain=+1 Vcc=5V
-40 -20 0 20 40 60 80 100 120
Temperature (°C)
Temperature (°C)
Figure 27. VOH & VOL vs. temperature
2
1
0
(V)
-1
OH & OL
V
-2
-3
-4
VOH
VOL
Gain=+1 Vcc=5V
Load=100
-40-200 20406080
Temperature (°C)
9/19
TSH330 Evaluation Boards

3 Evaluation Boards

An evaluation board kit optimized for high-speed operational amplifiers is available (order code: KITHSEVAL/STDL). The kit includes the following evaluation boards, as well as a CD-ROM containing datasheets, articles, application notes and a user manual:
z SOT23_SINGLE_HF BOARD: Board for the evaluation of a single high-speed op-amp in SOT23-5
package.
z SO8_SINGLE_HF: Board for the evaluation of a single high-speed op-amp in SO8 package. z SO8_DUAL_HF: Board for the evaluation of a dual high-speed op-amp in SO8 package. z SO8_S_MULTI: Board for the evaluation of a single high-speed op-amp in SO8 package in inverting
and non-inverting configuration, dual and single supply.
z SO14_TRIPLE: Board for the evaluation of a triple high-speed op-amp in SO14 package with video
application considerations.
Board material:
z 2 layers
z FR4 (εr=4.6)
z epoxy 1.6mm z copper thickness: 35µm
Figure 30. Evaluation kit for high-speed op-amps
10/19
Power Supply Considerations TSH330

4 Power Supply Considerations

Correct power supply bypassing is very important for optimizing performance in high-frequency ranges. Bypass capacitors should be placed as close as possible to the IC pins to improve high-frequency bypassing. A capacitor greater than 1µF is necessary to minimize the distortion. For better quality bypassing, a capacitor of 10nF can be added using the same implementation conditions. Bypass capacitors must be incorporated for both the negative and the positive supply.
For example, on the SO8_SINGLE_HF board, these capacitors are C6, C7, C8, C9.
Figure 31. Circuit for power supply bypassing
+VCC
+VCC
+
+
-
-
10microF
10microF
+
+
10nF
10nF
10nF
10nF
10microF
10microF +
+
-VCC
-VCC
Single power supply
In the event that a single supply system is used, new biasing is necessary to assume a positive output dynamic range between 0V and +V will provide an output dynamic from +0.9V to +4.1V on 100 load.
The amplifier must be biased with a mid-supply (nominally +V component of the signal at this value. Several options are possible to provide this bias supply, such as a virtual ground using an operational amplifier or a two-resistance divider (which is the cheapest solution). A high resistance value is required to limit the current consumption. On the other hand, the current must be high enough to bias the non-inverting input of the amplifier. If we consider this bias current (55µA max.) as the 1% of the current through the resistance divider to keep a stable mid-supply, two resistances of 470can be used.
The input provides a high pass filter with a break frequency below 10Hz which is necessary to remove the original 0 volt DC component of the input signal, and to fix it at +V
Figure 32 Evaluation Boards
illustrates a 5V single power supply configuration for the SO8_SINGLE evaluation board (see
on page 10).
supply rails. Considering the values of VOH and VOL, the amplifier
CC
/2), in order to maintain the DC
CC
/2.
CC
11/19
TSH330 Power Supply Considerations
A capacitor CG is added in the gain network to ensure a unity gain in low-frequency to keep the right DC component at the output. C a consideration of the cut off frequency of this low-pass filter.
Figure 32. Circuit for +5V single supply
10µF
10µF
IN
IN
+5V
+5V
R1
R1 470
470
R2
R2 470
470
contributes to a high-pass filter with Rfb//RG and its value is calculated with
G
+5V
+5V
+
Rin
Rin 1k
1k
+ 1µF
+ 1µF
10nF
10nF
+
+
R
R
CG
CG
+
_
_
fb
fb
R
R
G
G
100µF
100µF
OUT
OUT
100
100
12/19
Noise Measurements TSH330

5 Noise Measurements

The noise model is shown in
z eN: input voltage noise of the amplifier z iNn: negative input current noise of the amplifier z iNp: positive input current noise of the amplifier
Figure 33
, where:
Figure 33. Noise model
iN+
R1
R1
iN+
iN-
iN-
N1
N1
N2
N2
eN
eN
R3
R3
N3
N3
+
+
_
_
R2
R2
output
output
HP3577
HP3577 Input noise:
Input noise: 8nV/Hz
8nV/Hz
The thermal noise of a resistance R is:
4kTRF
where F is the specified bandwidth.
On a 1Hz bandwidth the thermal noise is reduced to
4kTR
where k is the Boltzmann's constant, equal to 1,374.10-23J/°K. T is the temperature (°K).
The output noise eNo is calculated using the Superposition Theorem. However eNo is not the simple sum of all noise sources, but rather the square root of the sum of the square of each noise source, as shown in
Equation 1
eNo2eN2g2iNn2R22iNp
:
eNo V12V22V32V42V52V6
+++++=
2
2
+×+×
R3
×
2
g
×
2
2
R2
------- -
4kTR1 4kTR2 1
R1
R2
------- -+
R1
2
×++×+=
4kTR3
Equation 1
Equation 2
13/19
TSH330 Noise Measurements
The input noise of the instrumentation must be extracted from the measured noise value. The real output noise value of the driver is:
2
eNo Measured()
instrumentation
()
=
2
Equation 3
The input noise is called the Equivalent Input Noise as it is not directly measured but is evaluated from the measurement of the output divided by the closed loop gain (eNo/g).
After simplification of the fourth and the fifth term of
eNo2eN2g2iNn2R22iNp
2
+×+×
Measurement of the Input Voltage Noise
If we assume a short-circuit on the non-inverting input (R3=0), from
eNo eN2g2iNn2R22g4kTR2
R3
×
Equation 2
2
2
g
×
eN
we obtain:
g4kTR21
Equation 4
×+×+×=
2
R2
------- -+
4kTR3
×+×+=
R1
we can derive:
Equation 4
Equation 5
In order to easily extract the value of eN, the resistance R2 will be chosen to be as low as possible. In the other hand, the gain must be large enough:
R3=0, gain: g=100
Measurement of the Negative Input Current Noise
To measure the negative input current noise iNn, we set R3=0 and use
iNn
Equation 5
. This time the gain
must be lower in order to decrease the thermal noise contribution:
R3=0, gain: g=10
Measurement of the Positive Input Current Noise
To extract iNp from
Equation 3
, a resistance R3 is connected to the non-inverting input. The value of R3
iNp
must be chosen in order to keep its thermal noise contribution as low as possible against the iNp contribution:
R3=100W, gain: g=10
14/19
Intermodulation Distortion Product TSH330

6 Intermodulation Distortion Product

The non-ideal output of the amplifier can be described by the following series:
Vout C0C1VinC2V
++ +=
2
in
C
n
V
in
n
due to non-linearity in the input-output amplitude transfer, where the input is V component, C
) is the fundamental and C
1(Vin
is the amplitude of the harmonics of the output signal V
n
=Asinωt, C0 is the DC
in
out
A one-frequency (one-tone) input signal contributes to harmonic distortion. A two-tone input signal contributes to harmonic distortion and to the intermodulation product.
The study of the intermodulation and distortion for a two-tone input signal is the first step in characterizing the driving capability of multi-tone input signals.
In this case:
tsin
ω
V
A
in
A
1
tsin+=
ω
2
then:
V
outC0C1
++ +=
A
()C
tsin
ω
A
1
tsin+
ω
2
A ω
()
2
tsin
A
1
2
tsin+
ω
2
C
A ω
()
n
tsin
A
1
n
tsin+
ω
2
From this expression, we can extract the distortion terms, and the intermodulation terms form a single sine wave: second-order intermodulation terms IM2 by the frequencies (ω
2
amplitude of C2A
+2ω2) and (ω1+2ω2) with an amplitude of (3/4)C3A3.
ω
1
and third-order intermodulation terms IM3 by the frequencies (2ω1-ω2), (2ω1+ω2), (
) and (ω1+ω2) with an
1-ω2
The measurement of the intermodulation product of the driver is achieved by using the driver as a mixer by a summing amplifier configuration (see
Figure 34
). In this way, the non-linearity problem of an external
mixing device is avoided.
Figure 34. Inverting summing amplifier (using evaluation board SO8_S_MULTI)
.
Vin1
Vin1
Vin2
Vin2
fb
fb
R
R1
R1
R2
R2
R
R
R
_
_
Vout
Vout
+
+
100
100
15/19
TSH330 The Bias of an Inverting Amplifier

7 The Bias of an Inverting Amplifier

A resistance is necessary to achieve a good input biasing, such as resistance R shown in
Figure 35
.
The magnitude of this resistance is calculated by assuming the negative and positive input bias current. The aim is to compensate for the offset bias current, which could affect the input offset voltage and the output DC component. Assuming Ib-, Ib+, R
in, Rfb and a zero volt output, the resistance R will be:
R
×
inRfb
R
---------------------- -=
RinR
+
fb
Figure 35. Compensation of the input bias current
fb
fb
R
R
Ib-
Ib-
Rin
Rin
Ib+
Ib+
_
_
+
+
R
R
Vcc+
Vcc+
Vcc-
Vcc-
Output
Output
Load
Load
16/19
Active Filtering TSH330

8 Active Filtering

Figure 36. Low-pass active filtering, Sallen-Key
C1
C1
R
R
1 R2
1 R2
IN
IN
RG
RG
From the resistors Rfb and RG we can directly calculate the gain of the filter in a classical non-inverting amplification configuration:
AVg1
+
+
C2
C2
_
_
fb
fb
R
R
R
fb
----------+== R
g
OUT
OUT
100
100
We assume the following expression as the response of the system:
Vout
ω
j
-------------------
T
ω
j
Vin
------------------------------------ ---------==
ω
j
12
g
2
j
jω
ω()
-------
ζ
--------------++
ω
2
c
ω
c
The cut-off frequency is not gain-dependent and so becomes:
ω
c
1
--------------------------------------= R1R2C1C2
The damping factor is calculated by the following expression:
1
ζ
ω
--­cC1R1C1R2C2R1C1R1
2
++()=
g
The higher the gain, the more sensitive the damping factor is. When the gain is higher than 1, it is preferable to use some very stable resistor and capacitor values. In the case of R1=R2=R:
R
fb
----------
1
R
g
2
ζ
2C2C
------------------------------------= 2C1C
Due to a limited selection of values of capacitors in comparison with resistors, we can fix C1=C2=C, so that:
R
fb
----------
1
R
g
2
ζ
2R2R
------------------------------------= 2R1R
17/19
TSH330 Package Mechanical Data

9 Package Mechanical Data

SO-8 MECHANICAL DATA
DIM.
A 1.35 1.75 0.053 0.069
A1 0.10 0.25 0.04 0.010
A2 1.10 1.65 0.043 0.065
B 0.33 0.51 0.013 0.020
C 0.19 0.25 0.007 0.010
D 4.80 5.00 0.189 0.197
E 3.80 4.00 0.150 0.157
e 1.27 0.050
H 5.80 6.20 0.228 0.244
h 0.25 0.50 0.010 0.020
L 0.40 1.27 0.016 0.050
k ˚ (max.)
ddd 0.1 0.04
MIN. TYP MAX. MIN. TYP. MAX.
mm. inch
8
18/19
0016023/C
Revision History TSH330

10 Revision History

Date Revision Description of Changes
Oct. 2004 1 First release corresponding to Preliminary Data version of datasheet.
Dec. 2004 2 Release of mature product datasheet.
Table 1
on page 2
June 2005 3
- Rthjc: Thermal Resistance Junction to Ambient replaced by Thermal Resistance Junction to Case
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19/19
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