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 100Ω 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 NumberTemperature RangePackageConditioningMarking
TSH330ID
TSH330IDTSO8Tape&ReelTSH330I
June 2005Revision 31/19
-40°C to +85°C
SO8TubeTSH330I
TSH330Absolute Maximum Ratings
1 Absolute Maximum Ratings
Table 1.Key parameters and their absolute maximum ratings
SymbolParameterValueUnit
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)0.6kV
ESD
MM: Machine Model
MM: Machine Model (pins 2 and 3)80V
CDM: Charged Device Model (pins 1, 4, 5, 6, 7 and 8)1.5kV
CDM: Charged Device Model (pins 2 and 3)1kV
Latch-up Immunity200mA
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 1.5kΩ resistor 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 < 5Ω), 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
+/-0.5V
+/-2.5V
-40 to + 85°C
-65 to +150°C
150°C
830mW
2kV
200V
Table 2.Operating conditions
SymbolParameterValueUnit
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 5.5V
-Vcc+1.5V, +Vcc-1.5VV
Electrical CharacteristicsTSH330
2 Electrical Characteristics
Table 3.Electrical characteristics for VCC= ±2.5Volts, T
=+25°C (unless otherwise specified)
amb
SymbolParameterTest ConditionMin.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. TemperatureT
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.
-3.10.18+3.1
0.8
1.6µV/°C
2655
21
722
13
5054
54
6374
67
56
52
No load16.620.2mA
T
< T
min.
amb
< T
max.
16.6mA
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 VoltageRL = 100Ω
OH
Low Level Output VoltageRL = 100Ω
OL
= ±1V, RL = 100Ω
∆V
out
< T
T
min.
out=20mVp-p, RL = 100Ω
V
= +1
A
V
= +2
A
V
amb
< T
max.
AV = -4
= -4, T
A
V
Small Signal V
= +2, RL = 100Ω
A
V
= 2Vp-p, AV = +2,
V
out
min.
< T
amb
=20mVp-p
out
< T
RL = 100Ω
< T
< T
amb
amb
< T
< T
max.
max.
T
min.
T
min.
104153kΩ
152kΩ
1500
1100
550
max.
630
600
160
1800V/µs
1.51.64V
1.54
-1.55-1.5V
-1.5
mV
µA
µA
dB
dB
dB
MHz
3/19
TSH330Electrical Characteristics
Table 3.Electrical characteristics for VCC= ±2.5Volts, T
=+25°C (unless otherwise specified)
amb
SymbolParameterTest ConditionMin.Typ.Max.Unit
I
Isink
out
Short-circuit Output current coming in
the op-amp.
Output to GND360453
< 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
= 100Ω
R
L
F = 10MHz
F = 20MHz
F = 100MHz
F = 150MHz
1.3nV/√Hz
22pA/√Hz
16pA/√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)
+1020028050
-1020027045
+23001000160
±2.5
-2270530180
+1300150038
-1260600280
4/19
Electrical CharacteristicsTSH330
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
1M10M100M1G
Gain=+10
Gain=+4
Gain=+2
Gain=+1
Ω
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
1M10M100M
+
+
-
-
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
1M10M100M1G
Gain=-10
Gain=-4
Gain=-2
Gain=-1
Ω
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
1M10M100M1G
-
-
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
1M10M100M1G
+
+
-
-
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
1M10M100M1G
+
+
-
-
100R
100R
300R
300R
Vout
Vout
Frequency (Hz)
5/19
TSH330Electrical 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
1M10M100M1G
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
1k10k100k1M10M
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
1,251,501,752,002,252,50
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
1k10k100k1M10M
Frequency (Hz)
Figure 9. Output amplitude vs. load
4,0
3,5
3,0
Vout max. (Vp-p)
2,5
2,0
101001k10k100k
6/19
Load (ohms)
Freq=?
Gain=+2
Vcc=5V
Figure 12. Noise figure
40
35
30
25
20
NF (dB)
15
10
5
0
1101001k10k100k
Rsource (ohms)
Vcc=5V
Electrical CharacteristicsTSH330
Figure 13. Output amplitude vs. frequency
5
4
3
2
Vout max. (Vp-p)
1
Gain=+2
Vcc=5V
Load=100
0
1M10M100M1G
Ω
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
Ω
Load=100
Figure 17. Isink
600
550
500
-1V
-1V
450
400
350
300
250
Isink (mA)
200
150
100
Ω
50
0
-2,0-1,5-1,0-0,50,0
+
+
_
_
RG
RG
+2.5V
+2.5V
VOL
VOL
withoutload
without load
-2.5V
-2.5V
Amplifier in open
Amplifier in open
loopwithoutload
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
Ω
-550
-600
0,00,51,01,52,0
+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
TSH330Electrical Characteristics
Figure 19. Slew rate
2,0
1,5
1,0
0,5
Output Response (V)
Gain=+2
0,0
-2ns-1ns0s1ns2ns3ns
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
Ω
Vcc=5V
46
Ω
Load=100
-40-20020406080100120
Temperature (°C)
Figure 23. SVR vs. temperature
85
80
75
70
-60
Gain (dB)
-80
Small Signal
Vcc=5V
Load=100
-100
1M10M100M1G
Ω
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
Ω
Load=100
0,5
-40-20 0 20406080100120
Temperature (°C)
65
SVR (dB)
60
Gain=+1
55
Vcc=5V
Ω
Load=100
50
-40-20020406080100120
Temperature (°C)
Figure 24. ROL vs. temperature
200
180
160
(MΩ)
OL
140
R
120
Open Loop
Vcc=5V
100
-40- 20020406080100120
Temperature (°C)
8/19
Electrical CharacteristicsTSH330
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
Ω
-40-20 0 20406080100120
Temperature (°C)
Figure 26. Vio vs. temperature
1000
800
600
IO
400
200
Open Loop
Vcc=5V
Ω
Load=100
0
-40-20020406080100120
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
-40-20020406080100120
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
-40-20020406080100120
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
Ω
Load=100
-40-200 20406080
Temperature (°C)
9/19
TSH330Evaluation 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 ConsiderationsTSH330
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 100Ω 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 470Ω can 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
TSH330Power 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
470Ω
470Ω
R2
R2
470Ω
470Ω
contributes to a high-pass filter with Rfb//RG and its value is calculated with
G
+5V
+5V
+
Rin
Rin
1kΩ
1kΩ
+ 1µF
+ 1µF
10nF
10nF
+
+
R
R
CG
CG
+
_
_
fb
fb
R
R
G
G
100µF
100µF
OUT
OUT
100Ω
100Ω
12/19
Noise MeasurementsTSH330
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:
4kTR∆F
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
:
eNoV12V22V32V42V52V6
+++++=
2
2
+×+×
R3
×
2
g
×
2
2
R2
------- -
4kTR1 4kTR2 1
R1
R2
------- -+
R1
2
×++×+=
4kTR3
Equation 1
Equation 2
13/19
TSH330Noise 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
eNoMeasured()
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
eNoeN2g2iNn2R22g4kTR2
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 ProductTSH330
6 Intermodulation Distortion Product
The non-ideal output of the amplifier can be described by the following series:
VoutC0C1VinC2V
++ +=
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
Aω
()
2
tsin
A
1
2
tsin+
ω
2
…C
Aω
()
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
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 FilteringTSH330
8 Active Filtering
Figure 36. Low-pass active filtering, Sallen-Key
C1
C1
R
R
1R2
1R2
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
100Ω
100Ω
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
TSH330Package Mechanical Data
9 Package Mechanical Data
SO-8 MECHANICAL DATA
DIM.
A1.351.750.0530.069
A10.100.250.040.010
A21.101.650.0430.065
B0.330.510.0130.020
C0.190.250.0070.010
D4.805.000.1890.197
E3.804.000.1500.157
e1.270.050
H5.806.200.2280.244
h0.250.500.0100.020
L0.401.270.0160.050
k˚ (max.)
ddd0.10.04
MIN.TYPMAX.MIN.TYP.MAX.
mm.inch
8
18/19
0016023/C
Revision HistoryTSH330
10 Revision History
DateRevisionDescription of Changes
Oct. 20041First release corresponding to Preliminary Data version of datasheet.
Dec. 20042Release of mature product datasheet.
Table 1
on page 2
June 20053
- Rthjc: Thermal Resistance Junction to Ambient replaced by Thermal
Resistance Junction to Case
Information furnished is believed to be accurate and reliable. However, STMicroelectronics assumes no responsibility for the consequences
of use of such information nor for any infringement of patents or other rights of third parties which may result from its use. No license is granted
by implication or otherwise under any patent or patent rights of STMicroelectronics. Specifications mentioned in this publication are subject
to change without notice. This publication supersedes and replaces all information previously supplied. STMicroelectronics products are not
authorized for use as critical components in life support devices or systems without express written approval of STMicroelectronics.
The ST logo is a registered trademark of STMicroelectronics
All other names are the property of their respective owners