TI TLE2301INE

TLE2301
EXCALIBUR 3-STATE-OUTPUT WIDE-BANDWIDTH
POWER OPERATIONAL AMPLIFIER
SLOS131 – DECEMBER 1993
D
D
D
D
D
D
D
D
NE PACKAGE
(TOP VIEW)
High Output Drive Capability . . . 1 A Min
3-State Outputs
High Gain-Bandwidth Product
8 MHz Typ
Low Total Harmonic Distortion
< 0.08% Typ
High Slew Rate . . . 12 V/µs Typ
Class AB Output Stage
Thermal Shutdown
Mains-Line Driver Circuit Application
Included
COMP2
VCC +
OUT1
VCC –
VCC –
OUT2
VCC +
TRS2
1
16
2
15
3
14
4
13
5
12
6
11
7
10
8
9
COMP1
VCC –
1N +
VCC –
VCC –
IN –
VCC –
TRS1
Terminals 4, 5, 12 and 13 are
connected to the lead frame.
description
MAXIMUM PEAK-TO-PEAK OUTPUT VOLTAGE
vs
FREQUENCY
VO(PP) – Maximum Peak-to-Peak Output Voltage – V
The TLE2301 is a power operational amplifier that
can deliver an output current of 1 A at high
frequencies with very low total harmonic
distortion. The device has an integral 3-state
mode to drive the output stage into a
high-impedance state and also to reduce the
supply current to less than 3.5 mA.
The combination of high output current and
3-state outputs makes the TLE2301 ideal for
implementing the signalling transformer driver in
mains-based telemetering modems. This
combination of features also makes the device
well suited for other high-current applications
(e.g., motor drivers and audio circuits).
Using the Texas Instruments established
Excalibur process, the TLE2301 is able to achieve
slew rates in excess of 12 V/µs and a gainbandwidth product of 8 MHz. The TLE2301 uses
a 16-pin NE power package to provide better
power handling capabilities than standard dual-inline packages.
8
VCC ± = ± 5 V
TA = 25°C
7
6
RL = 4.3 Ω
RL = 8.1 Ω
RL = 20 Ω
5
4
3
2
1
0
100
1k
10 k
100 k
f – Frequency – Hz
1M
10 M
Figure 1
The TLE2301 is characterized for operation over
the industrial temperature range of – 40°C to
85°C.
AVAILABLE OPTION
PACKAGE
TA
VIOmax AT 25°C
THERMALLY-ENHANCED
PLASTIC DIP
(NE)
– 40°C to 85°C
10 mV
TLE2301INE
Copyright  1993, Texas Instruments Incorporated
PRODUCTION DATA information is current as of publication date.
Products conform to specifications per the terms of Texas Instruments
standard warranty. Production processing does not necessarily include
testing of all parameters.
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1
TLE2301
EXCALIBUR 3-STATE-OUTPUT WIDE-BANDWIDTH
POWER OPERATIONAL AMPLIFIER
SLOS131 – DECEMBER 1993
equivalent schematic (entire device)
COMP1
COMP2
VCC +
OUT1
+
_
TRS1
OUT2
TRS2
VCC –
IN +
IN –
equivalent schematic (TRS1 and TRS2 inputs)
VCC +
TRS1
TRS2
VCC –
2
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TLE2301
EXCALIBUR 3-STATE-OUTPUT WIDE-BANDWIDTH
POWER OPERATIONAL AMPLIFIER
SLOS131 – DECEMBER 1993
Terminal Functions
TERMINAL
DESCRIPTION
NAME
NO.
COMP1
COMP2
16
1
COMP1 and COMP2 are compensation network terminals
IN +
14
Noninverting input
IN –
11
Inverting input
OUT1
OUT2
3
6
Two low-distortion class-AB output stages.
g
Each is capable of sourcing
g more than 500 mA. OUT1 and OUT2 should be
connected together for all applications.
TRS1
TRS2
9
8
TRS1 and TRS2 are 3-state input terminals. TRS2 should be connected to the ground of the circuit generating the 3-state
command ((normally
µP g
ground).
yµ
) The TLE2301 is brought
g into 3-state mode by
y raising
g TRS1 2 V above TRS2. Placing
g the
TLE2301 in a 3-state mode reduces the supply current to below 2.2 mA (typ). Normal operation resumes by bringing TRS1
to within 0.8 V of TRS2. The 3-state function can be disabled by connecting both TRS1 and TRS2 to VCC – .
VCC –
10, 15
High-impedance VCC – input terminals. Although these do not carry any of the device’s supply current, they increase the
stability of the device and should be connected to the negative supply terminal (VCC –).
VCC –
4, 5,
12, 13
Negative supply terminals and substrate. As with all NE packages, the substrate is directly connected to the lead frame.
The result is that the junction-to-ambient thermal impedance (ZθJA) is greatly reduced by soldering the negative supply
terminals to the copper area of the printed-circuit board (PCB).
VCC +
2, 7
Positive supply terminals. Both terminals should be connected to the positive voltage supply.
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3
TLE2301
EXCALIBUR 3-STATE-OUTPUT WIDE-BANDWIDTH
POWER OPERATIONAL AMPLIFIER
SLOS131 – DECEMBER 1993
absolute maximum ratings over operating free-air temperature range (unless otherwise noted)†
Supply voltage, VCC + (see Note 1) . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 22 V
Supply voltage, VCC – (see Note 1) . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . – 22 V
Differential input voltage, VID (see Note 2) . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . ± 44 V
Duration of short-circuit current at (or below) 25°C (see Note 3) . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . unlimited
Continuous total dissipation at (or below) 25°C free-air temperature (see Notes 4 and 5) . . . . . . . 2075 mW
Continuous total dissipation at 85°C case temperature (see Note 5) . . . . . . . . . . . . . . . . . . . . . . . . . 4640 mW
Operating free-air temperature range, TA . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . – 40°C to 85°C
Operating case or virtual junction temperature range . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . – 40°C to 150°C
Storage temperature range . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . – 65°C to 150°C
† Stresses beyond those listed under “absolute maximum ratings” may cause permanent damage to the device. These are stress ratings only, and
functional operation of the device at these or any other conditions beyond those indicated under “recommended operating conditions” is not
implied. Exposure to absolute-maximum-rated conditions for extended periods may affect device reliability.
NOTES: 1. All voltage values, except differential voltages, are with respect to the midpoint between VCC + and VCC – .
2. Differential voltages are at IN+ with respect to IN –.
3. The outputs when connected together may be shorted to either supply. Temperature and/or supply voltages must be limited to ensure
that the maximum dissipation rating is not exceeded.
4. For operation above 25°C free-air temperature, derate linearly at the rate of 16.56 mW/°C.
5. For operation above 25°C case temperature, derate linearly at the rate of 71.4 mW/°C. To avoid exceeding the design maximum
virtual junction temperature, these ratings should not be exceeded. Due to variations in individual device electrical characteristics
and thermal resistance, the built-in thermal overload protection may be activated at power levels slightly above or below the rated
dissipation.
FREE-AIR TEMPERATURE
DISSIPATION DERATING CURVE
CASE TEMPERATURE
DISSIPATION DERATING CURVE
10
Derating Factor = 16.56 mW/°C
ZθJC = 60.4°C/ W
PD – Total Continuous Power Dissipation – W
PD – Total Continuous Power Dissipation – W
2.5
2
1.5
1
0.5
0
6
4
2
Derating Factor = 71.4 mW/°C
ZθJC = 14°C/ W
0
25
4
8
40
55
70
TA – Free-Air Temperature – °C
85
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25
50
75
TC – Case Temperature – °C
100
TLE2301
EXCALIBUR 3-STATE-OUTPUT WIDE-BANDWIDTH
POWER OPERATIONAL AMPLIFIER
SLOS131 – DECEMBER 1993
recommended operating conditions
Supply voltage, VCC ±
VCC± = ± 5 V
VCC± = ± 15 V
Common mode input voltage,
voltage VIC
Common-mode
High-level 3-state enable voltage, VIH
MIN
MAX
UNIT
± 4.5
± 20
V
–4
1.6
V
–14
11.8
V
2
Low-level 3-state enable voltage, VIL
Continuous output current
Operating free-air temperature, TA
– 40
V
0.8
V
1
A
85
°C
electrical characteristics at specified free-air temperature, VCC ± = ±5 V, CC = 15 pF (unless
otherwise noted) (see Figure 5)
PARAMETER
TEST CONDITIONS
VIO
Input offset voltage
VO = 0,,
RS = 50 Ω
VIC = 0,,
IIB
Input bias current
VO = 0,,
RS = 50 Ω
VIC = 0,,
VICR
Common-mode input voltage
g range
g
RS = 50 Ω
VOM +
Maximum positive peak output voltage swing
RL = 20 Ω
Ω,
See Note 6
VOM –
Maximum negative peak output voltage swing
RL = 20 Ω
Ω,
See Note 6
AVD
Large signal differential voltage amplification
Large-signal
VO = ± 2 V,,
RL = 20 Ω
VIC = 0,,
ri
Differential input resistance
ro
Output resistance (see Note 7)
CMRR
TA†
25°C
MIN
TYP
MAX
0.4
7
Full range
10
25°C
283
Full range
500
Full range
g
–4
to
1.6
25°C
3.3
Full range
3.2
25°C
– 3.2
Full range
– 3.1
25°C
65
Full range
60
25°C
TRS1 = 0.8 V
450
mV
nA
V
3.5
V
– 3.4
V
87
dB
1
25°C
UNIT
MΩ
1
Ω
100
kΩ
TRS1 = 2 V,
3-state mode
Common mode rejection ratio
Common-mode
VIC = VICRmin,,
RS = 50 Ω
VO = 0,,
25°C
65
88
dB
kSVR
Supply voltage rejection ratio (∆VCC ± /∆VIO)
Supply-voltage
VCC ± = ± 4.5 V to ± 20 V,,
VIC = 0,
No load
25°C
70
100
dB
IIH
Enable input current
current, high
VI = 2 V
V,
IIL
current low
Enable input current,
8V
VI = 0
0.8
IOS
Short-circuit output current (see Note 8)
VO = 0,
ICC
3 state mode
3-state
25°C
0.01
Full range
0.5
25°C
0.01
Full range
tp ≤ 50 µs
VO = 0
0,
No load
VO = 0,
3-state mode
No load,
Supply current
25°C
25°C
0.5
0.5
1
1.8
µA
µA
A
10
21
1.73
2.7
Full range
25°C
0.5
25
mA
Full range
3.5
† Full range is – 40°C to 85°C.
NOTES: 6. OUT1 and OUT2 are connected together for all tests.
7. TRS1 voltage is measured with respect to TRS2 potential.
8. Pulse testing techniques are used to maintain the junction temperature as close to the ambient temperature as possible. Thermal
effects must be taken into account separately (tp = pulse duration time) .
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TLE2301
EXCALIBUR 3-STATE-OUTPUT WIDE-BANDWIDTH
POWER OPERATIONAL AMPLIFIER
SLOS131 – DECEMBER 1993
electrical characteristics at specified free-air temperature, VCC ± = ±15 V, CC = 15 pF (unless
otherwise noted) (see Figure 5)
PARAMETER
TEST CONDITIONS
VIO
Input offset voltage
VO = 0,,
RS = 50 Ω
VIC = 0,,
IIB
Input bias current
VO = 0,,
RS = 50 Ω
VIC = 0,,
VICR
Common-mode input voltage
g range
g
RS = 50 Ω
VOM +
Maximum positive peak output voltage swing
RL = 20 Ω
Ω,
See Note 6
VOM –
Maximum negative peak output voltage swing
RL = 20 Ω
Ω,
See Note 6
AVD
Large signal differential voltage amplification
Large-signal
VO = ± 6 V,,
RL = 20 Ω
VIC = 0,,
ri
Differential input resistance
ro
Output resistance (see Note 7)
CMRR
MIN
TYP
MAX
0.3
10
Full range
15
25°C
260
Full range
Full range
g
TRS1 = 0.8 V
3-state mode
Common-mode rejection ratio
VIC = VICRmin,
RS = 50 Ω
VO = 0,
kSVR
Supply voltage rejection ratio (∆VCC ± /∆VIO)
Supply-voltage
VCC ± = ± 4.5 V to ± 20 V,,
VIC = 0,
No load
IIH
Enable input current
current, high
VI = 2 V
V,
IIL
Enable input current,
current low
VI = 0
0.8
8V
IOS
Short-circuit output current (see Note 8)
VO = 0,
tp ≤ 50 µs
VO = 0
0,
No load
VO = 0,
3-state mode
No load,
3 state mode
3-state
– 14
to
11.8
25°C
13
Full range
13
25°C
– 12.6
Full range
– 12.5
25°C
70
Full range
65
13.5
mV
nA
V
– 13
V
102
dB
1
25°C
UNIT
V
MΩ
1
Ω
100
kΩ
25°C
70
97
dB
25°C
70
100
dB
25°C
0.01
Full range
25°C
25°C
25°C
0.01
0.5
0.5
1
3
11
Full range
25°C
0.5
0.5
Full range
Supply current
450
500
25°C
TRS1 = 2 V,
ICC
TA†
25°C
µA
A
25
30
2.2
µA
3.5
mA
Full range
5
† Full range is – 40°C to 85°C.
NOTES: 6. OUT1 and OUT2 are connected together for all tests.
7. TRS1 voltage is measured with respect to TRS2 potential.
8. Pulse testing techniques are used to maintain the junction temperature as close to the ambient temperature as possible. Thermal
effects must be taken into account separately (tp = pulse duration time) .
6
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TLE2301
EXCALIBUR 3-STATE-OUTPUT WIDE-BANDWIDTH
POWER OPERATIONAL AMPLIFIER
SLOS131 – DECEMBER 1993
operating characteristics at specified free-air temperature, VCC± = ±5 V, CC = 15 pF, TA = 25°C
(unless otherwise noted) (see Figure 5)
PARAMETER
TEST CONDITIONS
RL = 20 Ω,
MIN
TYP
MAX
9
12
V/µs
UNIT
SR
Slew rate at unity gain (see Figure 1)
VO = ± 1.5 V,
CL = 100 pF
ts
Settling time (see Figure 1)
RL = 20 Ω,,
CL = 100 pF,,
3-V step to 30 mV (1%)
07
0.7
µs
Vn
Equivalent input noise voltage (see Figure 2)
RS = 50 Ω,
f = 1 kHz
44
nV/√Hz
THD
Total harmonic distortion
VO = 1 Vrms,
RL = 20 Ω,
f = 50 kHz,
CL = 100 pF
0.04%
B1
φm
Unity-gain bandwidth (see Figure 3)
RL = 20 Ω,
CL = 100 pF
8
Phase margin at unity gain (see Figure 3)
RL = 20 Ω,
CL = 100 pF
30°
MHz
operating characteristics at specified free-air temperature, VCC± = ±15 V, CC = 15 pF, TA = 25°C
(unless otherwise noted) (see Figure 5)
PARAMETER
TEST CONDITIONS
TYP
MAX
9
14
V/µs
UNIT
SR
Slew rate at unity gain (see Figure 1)
VO = ± 10 V,
CL = 100 pF
ts
Settling time (see Figure 1)
RL = 20 Ω,,
CL = 100 pF,,
20-V step to 200 mV (1%)
18
1.8
µs
Vn
Equivalent input noise voltage (see Figure 2)
RS = 50 Ω,
f = 1 kHz
44
nV/√Hz
THD
Total harmonic distortion
VO = 2 Vrms,
RL = 20 Ω,
f = 50 kHz,
CL = 100 pF
B1
φm
Unity-gain bandwidth (see Figure 3)
RL = 20 Ω,
CL = 100 pF
8
Phase margin at unity gain (see Figure 3)
RL = 20 Ω,
CL = 100 pF
35°
POST OFFICE BOX 655303
RL = 20 Ω,
MIN
• DALLAS, TEXAS 75265
0.08%
MHz
7
TLE2301
EXCALIBUR 3-STATE-OUTPUT WIDE-BANDWIDTH
POWER OPERATIONAL AMPLIFIER
SLOS131 – DECEMBER 1993
PARAMETER MEASUREMENT INFORMATION
5 kΩ
VCC +
_
VI
VO
+
VCC –
CL
(see Note A)
VCC +
_
VO
+
RL
VCC –
50 Ω
50 Ω
NOTE A: CL includes the fixture capacitance.
Figure 2. Slew-Rate Test Circuit
Figure 3. Noise-Voltage Test Circuit
R2
10 kΩ
VI
VCC +
_
+
VCC –
CL
(see Note A)
VI –
R1
VCC +
_
VO
VO
VI +
+
R3
RL
COMP1
COMP1
Cc
15 pF
NOTE A: CL includes the fixture capacitance.
Figure 4. Gain-Bandwidth and
Phase-Margin Test Circuit
VCC –
Figure 5. Compensation Configuration
typical values
Typical values presented in this data sheet represent the median (50% point) of the device parametric
performance.
8
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TLE2301
EXCALIBUR 3-STATE-OUTPUT WIDE-BANDWIDTH
POWER OPERATIONAL AMPLIFIER
SLOS131 – DECEMBER 1993
TYPICAL CHARACTERISTICS
Table of Graphs
FIGURE
IIB
IIO
Input bias current
vs Free-air temperature
6, 7
Input offset current
vs Free-air temperature
6, 7
vs Frequency
AVD
Differential voltage amplification
VO(PP)
Maximum peak-to-peak output voltage
VOM
Maximum peak output voltage
ZθJA
Transient junction-to-ambient thermal impedance
ICC
Supply current
vs Free-air temperature
INPUT BIAS CURRENT AND
INPUT OFFSET CURRENT
vs
FREE-AIR TEMPERATURE
1000
VCC ± = ± 15 V
VIC = 0
100
IIB
10
1
– 50
IIO
– 25
0
25
50
75
TA – Free-Air Temperature – °C
100
I IO – Input Bias and Input Offset Currents – nA
IIIB
IB and IIO
I IO – Input Bias and Input Offset Currents – nA
IIIB
IB and IIO
Output impedance
9
vs Frequency
10, 11
vs Output current
12, 13
vs Supply voltage
14
vs Time
15
vs Supply voltage
16
vs Free-air temperature
Pulse response
zo
8
17
Small signal
18, 19
Large signal
20, 21
vs Frequency
22, 23
INPUT BIAS CURRENT AND
INPUT OFFSET CURRENT
vs
FREE-AIR TEMPERATURE
1000
VCC ± = ± 5 V
VIC = 0
IIB
100
10
1
0.1
– 50
IIO
– 25
0
25
50
75
TA – Free-Air Temperature – °C
Figure 6
100
Figure 7
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TLE2301
EXCALIBUR 3-STATE-OUTPUT WIDE-BANDWIDTH
POWER OPERATIONAL AMPLIFIER
SLOS131 – DECEMBER 1993
TYPICAL CHARACTERISTICS
DIFFERENTIAL VOLTAGE AMPLIFICATION
vs
FREQUENCY
ÁÁ
ÁÁ
20°
VCC ± = ± 15 V
RL = 20 Ω
CC = 100 pF
TA = 25°C
100
110
40°
80
60°
60
80°
40
100°
20
120°
0
140°
– 20
10
100
1k
10 k
100 k
1M
AVD – Differential Voltage Amplification – dB
AVD – Differential Voltage Amplification – dB
120
DIFFERENTIAL VOLTAGE AMPLIFICATION
vs
FREE-AIR TEMPERATURE
ÁÁ
ÁÁ
160°
10 M
RL = 20 Ω
100
90
VCC± = ± 5 V
80
70
60
– 50
f – Frequency – Hz
– 25
0
25
50
75
TA – Free-Air Temperature – °C
Figure 8
MAXIMUM PEAK-TO-PEAK OUTPUT VOLTAGE
vs
FREQUENCY
25
RL = 8.1 Ω
20
15
10
5
0
100
1k
10 k
100 k
f – Frequency – Hz
1M
10 M
VO(PP) – Maximum Peak-to-Peak Output Voltage – V
VO(PP) – Maximum Peak-to-Peak Output Voltage – V
VCC ± = ± 15 V
TA = 25°C
RL = 20 Ω
8
VCC ± = ± 5 V
TA = 25°C
7
6
RL = 4.3 Ω
RL = 8.1 Ω
RL = 20 Ω
5
4
3
2
1
0
100
Figure 10
10
100
Figure 9
MAXIMUM PEAK-TO-PEAK OUTPUT VOLTAGE
vs
FREQUENCY
30
VCC ± = ± 15 V
1k
10 k
100 k
f – Frequency – Hz
Figure 11
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1M
10 M
TLE2301
EXCALIBUR 3-STATE-OUTPUT WIDE-BANDWIDTH
POWER OPERATIONAL AMPLIFIER
SLOS131 – DECEMBER 1993
TYPICAL CHARACTERISTICS
MAXIMUM NEGATIVE PEAK OUTPUT VOLTAGE
vs
OUTPUT CURRENT
VOM – – Maximum Negative Peak Output Voltage – V
VOM + – Maximum Positive Peak Output Voltage – V
MAXIMUM POSITIVE PEAK OUTPUT VOLTAGE
vs
OUTPUT CURRENT
15
TA = 25°C
12.5
VCC ± = ± 15 V
7.5
VCC ± = ± 5 V
2.5
0
0
200
800
400
600
IO – Output Current – mA
TA = 25°C
– 12.5
10
5
– 15
1000
VCC ± = ± 15 V
– 10
– 7.5
–5
ÁÁÁ
ÁÁÁ
ÁÁÁ
VCC ± = ± 5 V
– 2.5
0
0
200
TRANSIENT JUNCTION-TO-AMBIENT
THERMAL IMPEDANCE†
vs
ON TIME
MAXIMUM PEAK OUTPUT VOLTAGE
vs
SUPPLY VOLTAGE
Z θ JA – Transient Junction-to-Ambient
Thermal Impedance – °C/mW
VOM – Maximum Peak Output Voltage – V
100
RL = 20 Ω
TA = 25°C
15
VOM +
10
5
0
–5
– 10
VOM –
– 15
– 20
0
2
4
1000
Figure 13
Figure 12
20
400
600
800
IO – Output Current – mA
6
8
10 12 14 16
VCC ± – Supply Voltage – V
18
20
d = 50%
10
d = 20%
d = 10%
d = 5%
d = 2%
1
Single Pulse
0.1
0.001
0.01
Figure 14
0.1
1
10
t – On Time – s
100
1000
Figure 15
† d = duty cycle
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TLE2301
EXCALIBUR 3-STATE-OUTPUT WIDE-BANDWIDTH
POWER OPERATIONAL AMPLIFIER
SLOS131 – DECEMBER 1993
TYPICAL CHARACTERISTICS
SUPPLY CURRENT
vs
SUPPLY VOLTAGE
SUPPLY CURRENT
vs
FREE-AIR TEMPERATURE
10.8
10.7
VO = 0
No Load
10.6
10.6
I CC – Supply Current – mA
I CC – Supply Current – mA
10.8
VO = 0
No Load
TA = 25°C
10.5
10.4
10.3
10.2
10.1
VCC ± = ± 15 V
10.4
10.2
10
VCC ± = ± 5 V
9.8
9.6
10
9.9
0
2
4
6
8
10
12
14
16
18
9.4
– 50
20
– 25
VCC ± – Supply Voltage – V
Figure 16
150
10
100
VO – Output Voltage – mV
VO – Output Voltage – V
VOLTAGE FOLLOWER
SMALL-SIGNAL
PULSE RESPONSE
15
5
0
–5
VCC ± = ± 15 V
RL = 20 Ω
CL = 100 pF
TA = 25°C
0
2
4
6
8
t – Time – µs
50
0
– 50
VCC ± = ± 5 V
RL = 20 Ω
CL = 100 pF
TA = 25°C
– 100
– 15
–2
10
12
14
– 150
– 0.5
0
0.5
1
t – Time – µs
Figure 18
12
100
Figure 17
VOLTAGE FOLLOWER
SMALL-SIGNAL
PULSE RESPONSE
– 10
0
25
50
75
TA – Free-Air Temperature – °C
Figure 19
POST OFFICE BOX 655303
• DALLAS, TEXAS 75265
1.5
2
2.5
TLE2301
EXCALIBUR 3-STATE-OUTPUT WIDE-BANDWIDTH
POWER OPERATIONAL AMPLIFIER
SLOS131 – DECEMBER 1993
TYPICAL CHARACTERISTICS
VOLTAGE FOLLOWER
LARGE-SIGNAL
PULSE RESPONSE
VOLTAGE FOLLOWER
LARGE-SIGNAL
PULSE RESPONSE
3
150
VCC ± = ± 15 V
RL = 20 Ω
CL = 100 pF
TA = 25°C
2
VO – Output Voltage – V
VO – Output Voltage – mV
100
50
0
– 50
– 100
1
0
–1
VCC ± = ± 5 V
RL = 20 Ω
CL = 100 pF
TA = 25°C
–2
– 150
– 0.5
0
0.5
1
1.5
t – Time – µs
2
–3
–2
2.5
0
2
4
6
8
t – Time – µs
Figure 20
4
VCC ± = ± 15 V
TA = 25°C
3.5
AVD = 100
3
2.5
2
AVD = 10
1.5
1
VCC ± = ± 5 V
TA = 25°C
3
AVD = 100
2.5
2
1.5
AVD = 10
1
AVD = 1
AVD = 1
0.5
0.5
0
1k
14
OUTPUT IMPEDANCE
vs
FREQUENCY
z o – Output Impedance – Ω
z o – Output Impedance – Ω
3.5
12
Figure 21
OUTPUT IMPEDANCE
vs
FREQUENCY
4
10
10 k
0
1k
f – Frequency – Hz
100 k
1M
f – Frequency – Hz
Figure 22
Figure 23
100 k
1M
10 M
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10 k
10 M
13
TLE2301
EXCALIBUR 3-STATE-OUTPUT WIDE-BANDWIDTH
POWER OPERATIONAL AMPLIFIER
SLOS131 – DECEMBER 1993
APPLICATION INFORMATION
circuit for mains-line driver over 40-kHz-to-90-kHz utility band
The following application is a circuit for a mains-line driver over 40-kHz-to-90-kHz utility band and is based
around the European standard (EN56065 –1) describing utility and consumer applications. This example shows
a possible implementation for differential transmission on the mains line. This applications circuit is designed
around the requirements of a domestic electricity meter operating over a utility band of 40 kHz to 90 kHz. A
dual-rail power supply of ± 5 V is used for this design example to limit device power dissipation. The same design
principles, however, can be applied to other applications.
frequency band
The frequency band for utility applications extends over an enormous range from 3 kHz to 95 kHz. In order to
have a coupling network that is economical and implemented with readily available components, this circuit is
designed for a subband from 40 kHz to 90 kHz.
This subband is sufficiently wide to support multichannel operation; i.e., 10 channels of 5 kHz width or more if
the channel widths are smaller. To avoid transmission spillover into the next band, a guard band of 5 kHz is
allowed. The upper frequency of this circuit is set to 90 kHz, and the lower frequency is chosen for an economical
coupling network and still has sufficient bandwidth to support multichannel operation.
output drive
The impedance of the mains network at these signalling frequencies is relatively low (<1 Ω to 30 Ω). This circuit
has been designed to drive a 4-Ω mains line over the 40-kHz-to-90-kHz bandwidth.
The signalling impedance of the mains network fluctuates as different loads are switched on during the day or
over a season, and it is influenced by many factors such as:
D
D
D
Localized loading from appliances connected to the mains supply near to the connection of the
communication equipment; e.g., heavy loads such as cookers and immersion heaters and reactive loads
such as EMC filters and power factor correctors
Distributed loading from consumers connected to the same mains cable, where their collective loading
reduces the mains signalling impedance during times of peak electricity consumption; e.g., meal times
Network parameters; e.g., transmission properties of cables and the impedance characteristics of
distribution transformers and other system elements
With such a diversity of factors, the signalling environment fluctuates enormously, irregularly, and can differ
greatly from one installation to another. The signalling system should be designed for reliable communications
over a wide range of mains impedances and signalling conditions. Consequently, the transmitter must be able
to drive sufficient signal into the mains network under these loading conditions.
The TLE2301 amplifier has 1-A output drive capability with short-circuit protection; hence, it adequately copes
with the high current demands required for implementing mains signalling systems.
3-state facility
When transmitting, the transmitter appears as a low-impedance signal source on the mains network. If
transmitters are left in the active mode whether transmitting or not and a large number of transmitters are
installed in close proximity, their combined loading would reduce the mains impedance to unacceptable levels.
Not only would each transmitter need to drive into an extremely low mains impedance, but signals arriving from
distant transmitters would be severely attenuated.
To overcome this problem, the transmitters need to present a high impedance to the mains network when they
are not transmitting. The mains network is then only loaded by a few transmitters at any one time, and the mains
signalling impedance is not adversely affected.
14
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TLE2301
EXCALIBUR 3-STATE-OUTPUT WIDE-BANDWIDTH
POWER OPERATIONAL AMPLIFIER
SLOS131 – DECEMBER 1993
APPLICATION INFORMATION
3-state facility (continued)
The TLE2301 incorporates an output 3-state facility, removing the need for additional circuitry to achieve this
function. In addition, the TLE2301 has a low standby current in the 3-state mode, making it ideal for applications
where low power consumption is also essential.
circuit configuration
The design methodology is to minimize power dissipation in the TLE2301 by maximizing the use of the available
output voltage swing of the amplifier. The amplifier’s output can swing to within 2 V of the supply rail before
saturation begins. With a chosen supply of ± 5 V, the maximum peak-to-peak voltage swing is 6 V. To ensure
that the amplifier’s output is not likely to clip under heavy loads, the maximum output voltage swing has been
reduced by 0.5 V, giving a usable peak-to-peak output voltage swing of 5.5 V.
It is assumed that the input signal to the transmitter stage has a peak-to-peak amplitude of 2.8 V (1 Vrms) as
might be expected if the transmission signal is digitally synthesized by circuitry operating solely from the 5-V
supply. The gain of the amplifier stage is appropriately set to:
Gain
output voltage swing
+ peak-to-peak
peak-to-peak input voltage
V
+ 5.5
2.8 V
+ 1.96
An inverting amplifier configuration is chosen for this example, as the input signal source is assumed to have
a relatively low impedance in relation to the gain-setting resistors.
CF1
15 pF
CI
100 nF
RF
4.7 kΩ
11
VI
RS
3.3 Ω
16
–
1
RI
2.4 kΩ
TRS1
(3-state control)
CF2
39 pF
3
IC1
14
9
7
6
2
+
4
D1
1N4001
5
D2
1N4001
CC
470 nF
Mains
Supply
5V
–5 V
CD1
220 µF
+
+ CD2
220 µF
CD3
100 nF
CD4
100 nF
L1
P2820
0V
Figure 24. Full-Circuit Diagram for Utility Band
A noninverting amplifier configuration could be used when the input signal needs to be terminated with high
impedance, but the user should take care that the amplitude of the input signal does not exceed the
common-mode input range (– 4 V < VICM < 1.8 V at VCC = ± 5 V) for low-gain implementations.
POST OFFICE BOX 655303
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15
TLE2301
EXCALIBUR 3-STATE-OUTPUT WIDE-BANDWIDTH
POWER OPERATIONAL AMPLIFIER
SLOS131 – DECEMBER 1993
APPLICATION INFORMATION
component calculations
The following sections contain the calculations for input capacitors, gain resistors, coupling network, coupling
capacitors, transformer-leakage inductance, series resistors, decoupling, and frequency compensation.
input capacitor
The incoming signal is ac coupled to remove any incoming dc offset and to provide only unity gain for the
amplifier’s input offset voltage. The value of 100 nF is chosen for this input capacitor as it has very little influence
on the amplifier’s signal gain over the frequency band.
gain resistors
The gain-setting resistors are chosen for a gain of 1.96; i.e., choosing:
Gain
+ RRF
I
R
F
+ 4.7 kΩ and RI + 2.4 kΩ
kΩ
+ 4.7
2.4 kΩ
+ 1.96
The resistor values are low enough to ensure that the circuit does not suffer from stray capacitance and signal
pick-up problems but not too low as to significantly load the mains impedance when the amplifier is in its
high-impedance state.
coupling network
The function of the line interface is to provide isolation from the mains supply while coupling the communication
signals onto the mains network. As the mains voltage is large in comparison with the communication signals,
the mains voltage needs to be isolated from the electronic circuitry. The simple coupling network limits the
current flowing from the mains supply as well as providing a convenient point at which to implement the safety
isolation barrier between the mains supply and the communications circuitry. The transformer can easily
achieve an isolation of 4 kV between primary and secondary windings, and the capacitor provides the low
frequency roll-off to impede the mains voltage.
The transformer has two other useful properties. First, the turns ratio can be selected to provide efficient power
transfer between the TLE2301 amplifier and the mains network. Second, the transformer possesses leakage
inductance that can be tuned with the coupling capacitor to form a band-pass filter.
By altering the turns ratio, the power dissipated in the TLE2301 can be reduced while maintaining the required
voltage levels on the mains line. A turns ratio of 1.67:1 was selected in this design to apply a 120-µdBV signal
onto the mains line. The calculation for the turns ratio is not straightforward due to the presence of numerous
complex impedances. The simplest method for deriving the turns ratio is to model the circuit with an analog
simulation program such as PSpice. It is from these simulations that the 1.67:1 turns ratio has been selected.
PSpice is a registered trademark of MicroSim Corporation.
16
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TLE2301
EXCALIBUR 3-STATE-OUTPUT WIDE-BANDWIDTH
POWER OPERATIONAL AMPLIFIER
SLOS131 – DECEMBER 1993
APPLICATION INFORMATION
coupling capacitor
With such a wide frequency band, the quality factor of the coupling filter needs to be low in order to avoid
unacceptably large attenuation at the band edges and to achieve a good coupling performance that is
insensitive to a wide range of loads. For a band-pass filter of this configuration, the quality factor is proportional
to the reciprocal of the coupling capacitance. For low Q, the value of CC needs to be large.
Q
+ quality factor and CC + coupling capacitor
Q ∝ 1
C
C
Counterbalancing this need for a large value of CC creates two more considerations. First, the capacitance
should not be so large as to allow significant 50-Hz mains current through the transformer ( I = 2 × π × f × CC
× V). Second, the coupling capacitor is required to meet certain safety standards. The coupling capacitor is
actually an RFI-suppression capacitor that has been designed by the manufacturers to provide an adequate
level of protection when connected across the various conductors of the mains supply (consult the UL1283 or
UL1414 standards for RFI capacitors). These types of capacitors can be expensive, physically large, restricted
in capacitance value, and limited in the number of manufacturers.
As a reasonable compromise between all these factors, a coupling capacitor of 470 nF is chosen. This value
is multisourced, moderately priced, limits the mains current through the transformer to less than 36 mA rms, and
has sufficient capacitance to form the desired low-Q filter.
transformer leakage inductance
The transformer leakage inductance, inherent to the transformer, can be used to form an LC band-pass filter.
If the capacitor alone is used to couple onto the mains network, its capacitance value needs to be quite large
for it to have a reasonably low reactance at the signalling frequencies. Forming an LC filter greatly reduces the
value of capacitor required. The center frequency of the filter is not the same as the midband frequency of
65 kHz. Band-pass filters show a symmetrical shape only when plotted against the logarithm of frequency, so
the center frequency (fo) is given by the following formula:
fo
Ǹ
+ flower fupper
+ Ǹ(40 90 ) kHz
+ 60 kHz
The leakage inductance of the transformer, as viewed from the winding connected to the coupling capacitor,
is derived from 2 π fO = 1 / √ LC. The required leakage inductance of the transformer is:
L
+ (2πf
+ (2π
o
1
)2
C
C
1
60 kHz ) 2
470 nF
+ 15 µH
Transformer Leakage Inductance
Capacitor
Figure 25. Band-Pass Coupling Filter
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17
TLE2301
EXCALIBUR 3-STATE-OUTPUT WIDE-BANDWIDTH
POWER OPERATIONAL AMPLIFIER
SLOS131 – DECEMBER 1993
APPLICATION INFORMATION
series resistor
The series resistor, RS, is included to limit the turn-on current, the amplifier’s offset current, and the signalling
current through the filter. With dual supply rails, there is always a potential problem of large turn-on currents as
the amplifier powers up. If one supply rail turns on before the other, the output of the TLE2301 amplifier could
saturate near to the applied supply rail, causing a large current to flow through the transformer winding
(Rwinding = 0.1 Ω for the P2820 transformer). The power supply needs to be of sufficient rating to ensure that
its rails could rise to the minimum operating voltage of the amplifier, at which point the amplifier is ensured to
have returned to stable operation.
With a series resistor of 3.3 Ω and assuming the output saturates at the maximum peak-to-peak voltage
excursion of 3 V, this turn-on current is limited to less than the device’s 1-A rating ( Itransient = 3 V / 3.3 Ω
= 0.91 A). Further reduction of this turn-on current by raising the value of the series resistor deteriorates the
filter’s performance into low signalling impedances on the mains network.
Alternatively, this turn-on current could be blocked by means of a series capacitor, but for this frequency band
the capacitor has to be large in value ( ≥ 3.3 µF ) so as not to adversely affect the filter. A nonpolarized capacitor
of this value is relatively expensive, and the resistor is still required to fulfill other functions.
Another way of preventing overcurrent at power up is to use the TLE2301 3-state mode. As the TRS2 control
line is intended to be tied to the microprocessor’s 0-V rail, the TRS1 control line must be taken high to activate
the 3-state mode, which implies that the positive rail is required to turn on first. Other schemes could be devised
to take TRS2 below the 0-V rail until the power supply has stabilized if the negative rail turns on first. Instead
of relying on a definite power-supply sequence or elaborate control circuitry, it is simpler to limit the current either
with a series resistor or capacitor.
The second function of the series resistor is to limit the dc current flow through the transformer winding due to
the dc offset at the amplifier’s output, which is caused by its input offset voltage. For a worst case input offset
of 20 mV, the output offset is also 20 mV as the dc gain of the circuit is unity. Offsets due to input bias currents
are negligible since the values of the gain-setting resistors are low. The dc current through the transformer is
therefore less than 7 mA (20 mV/3.3 Ω). This low level of dc current does not appreciatively increase the power
dissipation of the amplifier or noticeably diminish the harmonic performance of the transformer.
The final function of the series resistor is to limit the signalling current in the event that the mains impedance
might appear as solely reactive; i.e., without a resistive component. As a rough estimate, the peak signal current
from the amplifier is:
I
OM
where:
V
18
O (PP)
I
OM
+
V
O (PP)
R
S
ǒ Ǔ+
+
5.5 V
2
3.3 Ω
833 mA
+ Peak-to-peak output voltage swing
+ Peak-output-signalling current from amplifier
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TLE2301
EXCALIBUR 3-STATE-OUTPUT WIDE-BANDWIDTH
POWER OPERATIONAL AMPLIFIER
SLOS131 – DECEMBER 1993
APPLICATION INFORMATION
series resistor (continued)
Again, the value of the series resistor is sufficient to limit the peak-signal current below the device’s maximum
rating. This calculation does not take into account other resistive impedances in the signal path, which would
further reduce the peak signal current from the amplifier.
decoupling
Power-supply decoupling for the amplifier is provided by a 220-µF electrolytic capacitor and a 100-nF ceramic
capacitor per supply rail located close to the supply terminals of the TLE2301 device.
The decoupling capacitors for the negative supply should be connected to a pair of VCC – terminals (4 and 5 or
12 and 13), whichever pair is most convenient from a printed-circuit-board (PCB) layout point of view. In order
to minimize parasitic lead inductances, these capacitors should be located as close as possible to the device
terminals to which they are connected. As the VCC+ terminals are not adjacent on the package, the decoupling
capacitors should be connected to one terminal with a thick PCB track going to the other terminal.
The 220-µF electrolytic capacitor is chosen to provide good decoupling performance (less than 25-mV ripple
under the worst-case loading for the utility circuit). This value could be reduced to 100 µF for higher-frequency
consumer bands. The level of ripple depends on the source impedance of the power supply and the equivalent
series resistance of the chosen decoupling capacitors. The 100-nF ceramic capacitor provides high-frequency
decoupling for the amplifier.
CF1
15 pF
CF2
39 pF
16
11
–
1
3
IC1
14
7
2
+
6
15
10
13
12
VCC +
5
4
220 µF
+
100 nF
VCC –
220 µF
+
100 nF
0V
Figure 26. Amplifier Decoupling and Compensation
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19
TLE2301
EXCALIBUR 3-STATE-OUTPUT WIDE-BANDWIDTH
POWER OPERATIONAL AMPLIFIER
SLOS131 – DECEMBER 1993
APPLICATION INFORMATION
frequency compensation
The TLE2301 amplifier requires one compensation capacitor. However, when driving heavy loads, stability can
be increased by connecting VCC – terminals 10 and 15 to VCC – terminals 12 and 13 and using another capacitor
between COMP2 and the outputs. The circuit included in this application has been designed with two
compensation capacitors. The component values chosen are:
+ 15 pF
C
+ 33 pF
F2
C
F1
These component values could be adjusted if the amplifier is used for higher-frequency applications.
power dissipation
The impedance of the mains network fluctuates greatly for many reasons, but its impedance at the supplydistribution transformer is typically very low, less than 1 Ω, whereas the mains impedance in a house commonly
has a higher value, from 4 Ω to 40 Ω. For utility-metering applications, a master transmitter may be sited at the
supply-distribution transformer and would need to deliver more power into the mains network than the
household transmitter when generating comparable signal amplitudes.
NE thermally-enhanced dual in-line package
14 mm
d
5 mm
d
TLE2301
Z θJA – Junction-to-Ambient Thermal Impedance – °C/W
The TLE2301 utilizes the four center terminals of the dual-in-line package (NE) to transfer heat to a copper area
on the PCB. A copper area of 1290 mm2 provides a junction-to-ambient thermal impedance, ZθJA, of 34°C / W,
allowing the device to dissipate up to 1.9 W at 85°C for a junction temperature of 150°C or up to 1.5 W at 85°C
for a junction temperature of 135°C.
JUNCTION-TO-AMBIENT THERMAL
IMPEDANCE
vs
DIMENSIONS
50
45
40
35
30
25
20
0
10
20
30
d – Dimensions – mm
NOTE: When d = 25 mm, ZθJA = 34°C/ W
Figure 27. PCB Heatsink
20
POST OFFICE BOX 655303
• DALLAS, TEXAS 75265
40
50
TLE2301
EXCALIBUR 3-STATE-OUTPUT WIDE-BANDWIDTH
POWER OPERATIONAL AMPLIFIER
SLOS131 – DECEMBER 1993
APPLICATION INFORMATION
power dissipation in amplifier
Ǔ)ǒ
Ǔ
For sinusoidal waveforms, the dissipation in the amplifier, PAMP , is:
P
where:
+
AMP
ǒ
2
2
V
CC
I
V
CC
CC
π
I
OM
– P
O
+ AmplifierȀs quiescent current
I
+ Peak-output-signalling current from amplifier
OM
P + Output power consumed by coupling network and load
O
I
CC
The power dissipated in the amplifier is minimized if the amplifier’s peak output current, IOM, is minimized. Since
the output power consumed by the coupling and load is a function of current and voltage ( PO ≈ IO × VO ), the
amplifier’s peak output current can be minimized by maximizing the amplifier’s output voltage swing.
circuit parts list
The associated parts list is:
REFERENCE
FIGURE
COMPONENT
DESCRIPTION
IC1
Figure 24, Figure 26
TLE2301 operational amplifier
Texas Instruments TLE230INE
L1
Figure 24
1.67:1, 15-µH leakage transformer
Electronics Techniques P2820 (European manufacturer)
CC
Figure 24
470-nF capacitor
Metalized paper, safety standards UL1414
CI
Figure 24
100-nF capacitor
Ceramic, general purpose
CF1
Figure 24, Figure 26
15-pF capacitor
Ceramic, general purpose
CF2
Figure 24, Figure 26
39-pF capacitor
Ceramic, general purpose
CD1, CD2
Figure 24
220-µF, 10-V min capacitors
Aluminum electrolytic, general purpose
CD3, CD4
Figure 24
100-nF capacitors
Ceramic, general purpose
RF
Figure 24
4.7-kΩ, 0.125-W min resistor
Metal film, general purpose
RI
Figure 24
2.4-kΩ, 0.125-W min resistor
Metal film, general purpose
RS
Figure 24
3.3-kΩ, 1-W min, resistor
D1, D2
Figure 24
1N4001 series, 1-A min diodes
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21
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