Datasheet LT1497 Datasheet (Linear Technology)

FEATURES
Minimum Output Current: ±125mA
Maximum Supply Current per Amp: 7mA, VS = ±5V
Bandwidth: 50MHz, VS = ±15V
Slew Rate: 900V/µs, VS = ±15V
Wide Supply Range: VS = ±2.5V to ±15V (Enhanced θJA 16-Pin SO Package)
Enhanced θJA SO-8 Package for ±5V Operation
0.02% Differential Gain: AV = 2, RL = 150
0.015° Differential Phase: AV = 2, RL = 150
±13V Output Swing: IL = 100mA, VS = ±15V
±3.1V Output Swing: IL = 100mA, VS = ±5V
55ns Settling Time to 0.1%, 10V Step
Thermal Shutdown Protection
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APPLICATIONS
Twisted-Pair Drivers
Video Amplifiers
Cable Drivers
Test Equipment Amplifiers
Buffers
LT1497
Dual 125mA, 50MHz
Current Feedback Amplifier
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DESCRIPTION
The LT®1497 dual current feedback amplifier features low power, high output drive, excellent video characteristics and outstanding distortion performance. From a low 7mA maximum supply current per amplifier, the LT1497 drives ±100mA with only 1.9V of headroom. Twisted pairs can be driven differentially with – 70dBc distortion up to 1MHz for ±40mA peak signals.
The LT1497 is available in a low thermal resistance 16-pin SO package for operation with supplies up to ± 15V. For ±5V operation the device is also available in a low thermal resistance SO-8 package. The device has thermal and current limit circuits that protect against fault conditions.
The LT1497 is manufactured on Linear Technology’s complementary bipolar process. The device has charac­teristics that bridge the performance between the LT1229 and LT1207 dual current feedback amplifiers. The LT1229 has 30mA output drive, 100MHz bandwidth and 12mA supply current. The LT1207 has 250mA output drive, 60MHz bandwidth and 40mA supply current.
, LTC and LT are registered trademarks of Linear Technology Corporation.
TYPICAL APPLICATION
HDSL2 Single Pair Line Driver
560
560
1/2 LT1497
+
V
IN
560
560
1/2 LT1497
+
1:1*
*MIDCOM 671-7807
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135
1419 TA01
2nd and 3rd Harmonic Distortion of
HDSL2 Single Pair Line Driver
–40
VS = ±5V
= ±1.25V
V
IN
= ±2.5V
V
OUT
–50
–60
–70
2ND
DISTORTION (dBc)
3RD
–80
–90
100k
FREQUENCY (Hz)
1M 2M
1497 TA02
1
LT1497
WW
W
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ABSOLUTE MAXIMUM RATINGS
Total Supply Voltage (V+ to V–)
LT1497CS8.......................................................... 14V
LT1497CS............................................................ 36V
Noninverting Input Current ................................... ±2mA
Output Short-Circuit Duration (Note 1)..........Continuous
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W
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PACKAGE/ORDER INFORMATION
ORDER PART
TOP VIEW
1
OUT A 
–IN A
2
+IN A
T
JMAX
A
3
V
4
S8 PACKAGE
8-LEAD PLASTIC SO
= 150°C, θJA = 80°C/ W (NOTE 3)
8
V+ OUT B
7
–IN B
6
B
+IN B
5
NUMBER
LT1497CS8
S8 PART MARKING
1497
Operating Temperature Range (Note 2) ... – 40°C to 85°C
Specified Temperature Range ...................... 0°C to 70°C
Maximum Junction Temperature (See Below) ....... 150°C
Storage Temperature Range .................. –65°C to 150°C
Lead Temperature (Soldering, 10 sec)................... 300°C
TOP VIEW
1
V–
2
NC
3
OUT A
4
–IN A +IN A
T
JMAX
V NC V
A
5
6
7
8
S PACKAGE
16-LEAD PLASTIC SO
= 150°C, θJA = 40°C/ W (NOTE 3)
16
V–
15
NC 
+
14
V
13
OUT B
12
–IN B
B
11
+IN B
10
NC
9
V
ORDER PART
NUMBER
LT1497CS
Consult factory for Industrial and Military grade parts.
ELECTRICAL CHARACTERISTICS
VCM = 0V, ±2.5V VS ±15V (LT1497CS), ±2.5V VS ±5V (LT1497CS8), pulse tested unless otherwise noted.
SYMBOL PARAMETER CONDITIONS MIN TYP MAX UNITS
V
I
I
e +i –i R
C
OS
+
IN
IN
n
n
n
IN
IN
Input Offset Voltage TA = 25°C ±3 ±10 mV
±15 mV
Input Offset Voltage Matching TA = 25°C ±1 ±3.5 mV
±5.0 mV
Input Offset Voltage Drift 10 µV/°C Noninverting Input Current TA = 25°C ±1 ±3 µA
±10 µA
Noninverting Input Current Matching TA = 25°C ±0.3 ±1.0 µA
±1.5 µA
Inverting Input Current TA = 25°C ±7 ±20 µA
±40 µA
Inverting Input Current Matching TA = 25°C ±3 ±10 µA
±15 µA
Input Noise Voltage Density f = 1kHz, RF = 1k, RG = 10, RS = 0 3 nV/Hz Noninverting Input Noise Current Density f = 1kHz, RF = 1k, RG = 10, RS = 10k 2 pA/Hz Inverting Input Noise Current Density f = 1kHz, RF = 1k, RG = 10, RS = 10k 20 pA/Hz Input Resistance VIN = ±13V, VS = ±15V 1.5 10 M
VIN = ±3V, VS = ±5V 1.5 8 M VIN = ±0.5V, VS = ±2.5V 1.5 8 M
Input Capacitance 3pF
2
LT1497
ELECTRICAL CHARACTERISTICS
VCM = 0V, ±2.5V VS ±15V (LT1497CS), ±2.5V VS ±5V (LT1497CS8), pulse tested unless otherwise noted.
SYMBOL PARAMETER CONDITIONS MIN TYP MAX UNITS
Input Voltage Range VS = ±15V ±13 ±14 V
VS = ±5V ±3.0 ±4.0 V
= ±2.5V ±0.5 ±1.5 V
V
S
CMRR Common Mode Rejection Ratio VS = ±15V, VCM = ±13V, TA = 25°C5562 dB
53 dB
VS = ±5V, VCM = ±3V, TA = 25°C5460dB
52 dB
VS = ±2.5V, VCM = ±0.5V, TA = 25°C5256 dB
50 dB
Inverting Input Current VS = ±15V, VCM = ±13V 2.0 10 µA/V Common Mode Rejection V
PSRR Power Supply Rejection Ratio VS = ±2V to ±15V, TA = 25°C6676dB
Noninverting Input Current VS = ±2V to ±15V 5 50 nA/V Power Supply Rejection V
Inverting Input Current VS = ±2V to ±15V 0.1 2 µA/V Power Supply Rejection V
A
R
V
I
I
VOL
OL
OUT
OUT
S
Large-Signal Voltage Gain VS = ±15V, V
Transresistance, V
OUT
/I
IN
Maximum Output Swing VS = ±15V, RL = 150, TA = 25°C ±12.80 ±13.15 V
Maximum Output Current RL = 1, VS = ±15V ±125 ±220 mA
Supply Current per Amplifier VS = ±2.5V to ±5V, TA = 25°C 6.0 7.0 mA
Channel Separation VS = ±15V, V
= ±5V, VCM = ±3V 2.5 10 µA/V
S
= ±2.5V, VCM = ±0.5V 3.0 10 µA/V
V
S
63 dB
VS = ±2V to ±5V, TA = 25°C6676dB
63 dB
= ±2V to ±5V 5 50 nA/V
S
= ±2V to ±5V 0.1 2 µA/V
S
= ±10V, RL = 150 66 80 dB
= ±5V, V
V
S
= ±2.5V, V
V
S
VS = ±15V, V
= ±5V, V
V
S
VS = ±2.5V, V
OUT
= ±2.5V, RL = 50 66 80 dB
OUT
= ±0.5V, RL = 50 66 80 dB
OUT
= ±10V, RL = 150 100 500 k
OUT
= ±2.5V, RL = 50 100 500 k
OUT
= ±0.5V, RL = 50 100 300 k
OUT
±12.60 V
VS = ±15V, IL = ±100mA, TA = 25°C ±12.65 ±13.0 V
±12.55 V
VS = ±5V, RL = 50, TA = 25°C ±3.20 ±3.45 V
±3.10 V
VS = ±5V, IL = ±100mA, TA = 25°C ±2.75 ±3.10 V
±2.65 V
VS = ±2.5V, RL = 50, TA = 25°C ±1.25 ±1.45 V
±1.15 V
VS = ±2.5V, IL = ±50mA, TA = 25°C ±1.00 ±1.15 V
±0.90 V
= 1, VS = ±5V ±125 ±220 mA
R
L
RL = 1, VS = ±2.5V ±140 mA
8.0 mA
VS = ±15V, TA = 25°C 7.0 9.0 mA
10.5 mA
= ±10V, RL = 150 100 120 dB
= ±5V, V
V
S
OUT
= ±2.5V, RL = 50 100 115 dB
OUT
3
LT1497
ELECTRICAL CHARACTERISTICS
VCM = 0V, ±2.5V VS ±15V (LT1497CS), ±2.5V VS ±5V (LT1497CS8), pulse tested unless otherwise noted.
SYMBOL PARAMETER CONDITIONS MIN TYP MAX UNITS
SR Slew Rate VS = ±15V, TA = 25°C (Note 4) 500 900 V/µs
VS = ±5V, TA = 25°C (Note 4) 200 350 V/µs
BW Small-Signal Bandwidth VS = ±15V, RF = RG = 560, RL = 100 50 MHz
VS = ±5V, RF = RG = 560, RL = 100 35 MHz VS = ±2.5V, RF = RG = 560, RL = 100 30 MHz
t
r
t
s
Small-Signal Rise Time VS = ±15V, RF = RG = 560, RL = 100 7.5 ns
Overshoot VS = ±15V, RF = RG = 560, RL = 100 15 %
Propagation Delay VS = ±15V, RF = RG = 560, RL = 100 6.8 ns
Settling Time VS = ±15V, 10V Step, 0.1%, AV = –1 55 ns
Differential Gain (Note 5) VS = ±15V, RF = RG = 510, RL = 150 0.02 %
Differential Phase (Note 5) VS = ±15V, RF = RG = 510, RL = 150 0.015 Deg
V
= ±5V, RF = RG = 560, RL = 100 9.5 ns
S
VS = ±2.5V, RF = RG = 560, RL = 100 11 ns
V
= ±5V, RF = RG = 560, RL = 100 12 %
S
VS = ±2.5V, RF = RG = 560, RL = 100 10 %
VS = ±5V, RF = RG = 560, RL = 100 8.4 ns V
= ±2.5V, RF = RG = 560, RL = 100 9.7 ns
S
VS = ±5V, 5V Step, 0.1%, AV = –1 50 ns
VS = ±15V, RF = RG = 510, RL = 50 0.19 % VS = ±5V, RF = RG = 510, RL = 150 0.08 % V
= ±5V, RF = RG = 510, RL = 50 0.41 %
S
VS = ±15V, RF = RG = 510, RL = 50 0.235 Deg VS = ±5V, RF = RG = 510, RL = 150 0.045 Deg V
= ±5V, RF = RG = 510, RL = 50 0.310 Deg
S
400 V/µs
150 V/µs
The denotes specifications which apply over the full operating temperature range.
Note 1: Applies to short circuits to ground only. A short circuit between the output and either supply may damage the part when operated on supplies greater than ±10V
Note 2: The LT1497 is designed, characterized and expected to operate over the temperature range of –40°C to 85°C, but is not tested at –40°C and 85°C. Guaranteed industrial grade parts are available, consult factory.
Note 3: Thermal resistance varies depending upon the amount of PC board metal attached to the device. θ covered with 2oz copper on both sides.
is specified for a 2500mm2 test board
JA
Note 4: Slew rate is measured between ±5V on a ±10V output signal while operating on ±15V supplies with R On ±5V supplies slew rate is measured between ±1V on a ±3V output signal. The slew rate is much higher when the input is overdriven and when the amplifier is operated inverting. See the Applications Information section.
Note 5: NTSC composite video with an amplifier output level of 2V peak.
= 453, RG = 49.9 and RL = 150.
F
4
LT1497
SUPPLY VOLTAGE (±V)
0
0
–3dB BANDWIDTH (MHz)
10
30
40
50
12
90
1497 G03
20
618
10
416
8
214
60
70
80
PEAKING 1dB PEAKING 5dB
RF = 470
R
F
= 560
RF = 750
RF = 1k
GAIN = 2 R
L
= 100
W
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SMALL-SIGNAL BANDWIDTH
VS = ±15V, Peaking 1dB
A
V
–1 150 560 560 59.2
1 150 560 57.0
2 150 510 510 59.1
10 150 270 30 43.4
R
L
R
F
R
G
50 560 560 43.1 20 620 620 30.0
50 560 42.7 20 560 30.3
50 560 560 41.7 20 620 620 20.7
50 270 30 30.9 20 270 30 19.0
–3dB BW (MHz)
VS = ±5V, Peaking 1dB
A
V
–1 150 510 510 45.0
1 150 510 44.3
2 150 510 510 41.7
10 150 270 30 28.1
UW
TYPICAL PERFORMANCE CHARACTERISTICS
Voltage Gain and Phase vs Frequency, Gain = 6dB
9 8 7 6 5
4 3
VOLTAGE GAIN (dB)
2 1
RL = 100Ω
0
= RG = 560
R
F
–1
0.1
PHASE
GAIN
1 10 100
FREQUENCY (MHz)
±5V
±5V
±15V
±15V
1497 G01
0 45 90
PHASE SHIFT (DEG)
135 180
225 270
–3dB Bandwidth vs Supply Voltage
90
80
70
60
50
40
30
–3dB BANDWIDTH (MHz)
20
10
0
PEAKING 1dB PEAKING 5dB
RF = 470
416
214
0
SUPPLY VOLTAGE (±V)
R
= 560
F
RF = 750
RF = 1k
618
10
8
12
R
L
R
F
R
G
–3dB BW (MHz)
50 560 560 32.0 20 560 560 23.2
50 560 31.7 20 560 22.9
50 560 560 30.4 20 560 560 21.9
50 270 30 21.9 20 270 30 14.6
–3dB Bandwidth vs Supply Voltage
GAIN = 2
= 1k
R
L
1497 G02
28 26 24 22 20
18 16
VOLTAGE GAIN (dB)
14 12 10
8
0.1
Voltage Gain and Phase vs Frequency, Gain = 20dB
0
PHASE
RL = 100Ω
= 270Ω
R
F
= 30
R
G
1 10 100
FREQUENCY (MHz)
GAIN
±5V
±5V
±15V
±15V
1497 G04
45 90
PHASE SHIFT (DEG)
135 180
225 270
–3dB Bandwidth vs Supply Voltage
90
80
70
60
50
40
30
–3dB BANDWIDTH (MHz)
20
10
0
PEAKING 1dB PEAKING 5dB
416
214
0
SUPPLY VOLTAGE (±V)
–3dB Bandwidth vs Supply Voltage
GAIN = 10
= 1k
R
L
= 270
R
F
RF = 560
618
8
RF = 430
RF = 750
RF = 1k
10
12
1497 G05
90
80
70
60
50
40
30
–3dB BANDWIDTH (MHz)
20
10
0
PEAKING 1dB PEAKING 5dB
RF = 560
618
416
214
0
SUPPLY VOLTAGE (±V)
GAIN = 10
= 100
R
L
RF = 430
RF = 750
8
RF = 270
RF = 1k
10
12
1497 G06
5
LT1497
FEEDBACK RESISTOR (k)
10
CAPACITIVE LOAD (pF)
1000
10000
023
1497 G09
1
1
100
RL = 1k A
V
= 2
PEAKING 5dB 
VS = ±5V
V
S
= ±15V
TEMPERATURE (°C)
–50
200
250
350
0
25 75
1497 G15
150
100
–25 0
50 100 125
50
300
OUTPUT SHORT-CIRCUIT CURRENT (mA)
VS = ±15V R
L
= 1
SINKING
SOURCING
UW
TYPICAL PERFORMANCE CHARACTERISTICS
Differential Phase vs Supply Voltage
0.5 RF = RG = 510
= 2
A
V
AMPLIFIER OUTPUT = 2V PEAK
0.4
0.3
0.2
DIFFERENTIAL PHASE (DEG)
0.1 RL = 150
0
7
5
9
SUPPLY VOLTAGE (±V)
Output Saturation Voltage vs Junction Temperature, ±15V
+
V
VS = ±15V
= 50mA
I
–1
–2
IL = 125mA
–3
3
IL = 125mA
2
1
OUTPUT SATURATION VOLTAGE (V)
V
–50
–25 0
L
IL = 100mA
IL = 100mA
IL = 50mA
25 75
TEMPERATURE (°C)
RL = 50
RL = 1k
11
13
15
1497 G07
IL = 75mA
IL = 75mA
50 100 125
1497 G10
Differential Gain vs Supply Voltage
0.5
0.4
0.3
0.2
DIFFERENTIAL GAIN (%)
0.1
0
5
RF = RG = 510
= 2
A
V
AMPLIFIER OUTPUT = 2V PEAK
RL = 1k
7
9
SUPPLY VOLTAGE (±V)
Output Saturation Voltage vs Junction Temperature, ±5V
+
V
VS = ±5V
= 50mA
I
–1
–2
IL = 125mA
–3
3
IL = 125mA
2
1
OUTPUT SATURATION VOLTAGE (V)
V
–50
–25 0
L
IL = 100mA
IL = 100mA
IL = 50mA
25 75
TEMPERATURE (°C)
RL = 50
RL = 150
11
13
1497 G08
IL = 75mA
IL = 75mA
50 100 125
1497 G11
Maximum Capacitive Load vs Feedback Resistor
15
Output Saturation Voltage vs Junction Temperature, ±2.5V
+
V
VS = ±2.5V
–1
–2
–3
3
2
1
OUTPUT SATURATION VOLTAGE (V)
V
–50
–25 0
IL = 25mA
IL = 50mA
IL = 75mA
IL = 25mA
50 100 125
25 75
TEMPERATURE (°C)
IL = 75mA
IL = 50mA
1497 G12
Supply Current vs Ambient Temperature
8.5
8.0
7.5
7.0
6.5
6.0
5.5
SUPPLY CURRENT PER AMPLIFIER (mA)
5.0
–50
6
VS = ±15V
VS = ±5V
–25 0
TEMPERATURE (°C)
VS = ±2.5V
50 100 125
25 75
1497 G13
Input Common Mode Limit vs Junction Temperature
+
V
–0.5
–1.0
–1.5
1.5
1.0
COMMON MODE RANGE (V)
0.5
V
–50
–25 0
V+ = 2V TO 18V
V– = –2V TO –18V
TEMPERATURE (°C)
50 100 125
25 75
Output Short-Circuit Current vs Junction Temperature
1497 G14
UW
FREQUENCY (Hz)
–80
OUTPUT TO INPUT CROSSTALK (dB)
–60
–40 –50
–20
–10
–90
–70
–30
10k 1M 10M 100M
1497 G24
–100 –110
100k
VS = ±15V A
V
= 10
R
L
= 100
R
F
= 560Ω
R
G
= 62
TYPICAL PERFORMANCE CHARACTERISTICS
LT1497
Settling Time to 10mV vs Output Step
10
8 6 4 2 0
–2
OUTPUT STEP (V)
–4 –6 –8
–10
AV = –1
20
0
AV = 1
SETTLING TIME (ns)
40
A
V
AV = –1
Total Harmonic Distortion vs Frequency
0.10 VS = ±15V
= 100
R
L
= RG = 560
R
F
0.01
TOTAL HARMONIC DISTORTION (%)
0.001 10 100
V
OUT
V
OUT
1k 10k 100k
FREQUENCY (Hz)
60
= 1
= 7V
= 2V
VS = ±15V
= 560
R
F
80
1497 G16
RMS
RMS
1497 G19
100
Settling Time to 1mV vs Output Step
10
VS = ±15V
8
= 560
R
F
6
A
= 1
V
4 2 0
–2
OUTPUT STEP (V)
–4
AV = 1
–6 –8
–10
25
0
AV = –1
AV = –1
50
100
75
SETTLING TIME (ns)
125
150
2nd and 3rd Harmonic Distortion vs Frequency
–20
VS = ±15V
= 5V
= 50 = 560
2ND
3RD
P-P
110
FREQUENCY (MHz)
AV = 1
3RD
V
OUT
–30
R
L
R
F
–40
–50
–60
AV = 1
–70
DISTORTION (dBc)
–80
AV = –1
–90
–100
0.1
175
200
AV = –1 2ND
225
1497 G17
1497 G20
250
Spot Noise Voltage and Current vs Frequency
100
10
SPOT NOISE (nV/Hz OR pA/Hz)
1
10 100
1k 10k 100k
FREQUENCY (Hz)
3rd Order Intercept vs Frequency
40
35
30
25
20
3RD ORDER INTERCEPT (dBm)
15
10
0
10 15 20
5
FREQUENCY (MHz)
VS = ±15V
= 50
R
L
= 270Ω
R
F
= 30Ω
R
G
PO1 = PO2 = 4dBm
–i
n
e
n
+i
n
25 30
1497 G18
1497 G21
Output Impedance vs Frequency
100
VS = ±15V
10
1
RF = RG = 1.5k
0.1
OUTPUT IMPEDANCE ()
RF = RG = 560
0.01 10k 100k
1M 10M 100M
FREQUENCY (Hz)
1497 G22
Power Supply Rejection vs Frequency
80
70
60
50
40
30
20
POWER SUPPLY REJECTION (dB)
10
0
10k 1M 10M 100M
100k
FREQUENCY (Hz)
VS = ±15V
= 50
R
L
= RG = 560
R
F
POSITIVENEGATIVE
Amplifier Crosstalk vs Frequency
1497 G23
7
LT1497
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WUU
APPLICATIONS INFORMATION
The LT1497 is a dual current feedback amplifier with high output current drive capability. Bandwidth is maintained over a wide range of voltage gains by the appropriate choice of feedback resistor. These amplifiers will drive low impedance loads such as cables with excellent linearity at high frequencies.
Feedback Resistor Selection
The optimum value for the feedback resistor is a function of the operating conditions of the device, the load imped­ance and the desired flatness of frequency response. The Small-Signal Bandwidth table gives the values which result in the highest bandwidth with less than 1dB of peaking for various gains, loads and supply voltages. If this level of flatness is not required, a higher bandwidth can be obtained by use of a lower feedback resistor. The characteristic curves of Bandwidth vs Supply Voltage indicate feedback resistors for peaking up to 5dB. These curves use a solid line when the response has less than 1dB of peaking and a dashed line when the response has 1dB to 5dB of peaking. Note that in a gain of 10 peaking is always under 1dB for the resistor ranges shown. Reducing the feedback resistor further than 270 in a gain of 10 will increase the bandwidth, but it also loads the amplifier and reduces the maximum current available to drive the load.
Capacitive Loads
The LT1497 can drive capacitive loads directly when the proper value of feedback resistor is used. The graph of Maximum Capacitive Load vs Feedback Resistor should be used to select the appropriate value. The graph shows feedback resistor values for 5dB frequency peaking when driving a 1k load at a gain of 2. This is a worst-case condition. The amplifier is more stable at higher gains and driving heavier loads (smaller load resistors). Alterna­tively, a small resistor (10 to 20) can be put in series with the output to isolate the capacitive load from the amplifier output. This has the advantage in that the ampli­fier bandwidth is only reduced when the capacitive load is present, and the disadvantage that the gain is a function of the load resistance.
Capacitance on the Inverting Input
Current feedback amplifiers require resistive feedback from the output to the inverting input for stable operation. Take care to minimize the stray capacitance between the output and the inverting input. Capacitance on the invert­ing input to ground will cause peaking in the frequency response (and overshoot in the transient response), but it does not degrade the stability of the amplifier.
Power Supplies
The LT1497 will operate on single or split supplies from ±2V (4V total) to ±15V (30V total). It is not necessary to use equal value split supplies, however, the offset voltage and inverting input bias current will change. The offset voltage changes about 1mV per volt of supply mismatch. The inverting bias current can change as much as 10µA per volt of supply mismatch, though typically the change is less than 2.5µA per volt.
Thermal Considerations
The LT1497 contains a thermal shutdown feature that protects against excessive internal (junction) tempera­ture. If the junction temperature of the device exceeds the protection threshold, the device will begin cycling between normal operation and an off state. The cycling is not harmful to the part. The thermal cycling occurs at a slow rate, typically 10ms to several seconds, depending upon the power dissipation and the thermal time con­stants of the package and the amount of copper on the board under the package. Raising the ambient tempera­ture until the device begins thermal shutdown gives a good indication of how much margin there is in the thermal design.
For surface mount devices heat sinking is accomplished by using the heat spreading capabilities of the PC board and its copper traces. Experiments have shown that the heat spreading copper layer does not need to be electri­cally connected to the leads of the device. The PCB material can be very effective at transmitting heat between the pad area attached to V– pins of the device and a ground
8
LT1497
560
–15V
560
+
560
560
86.4mA
15V
200
200
1497 F01
+
A
–10V
10V
f = 2MHz
U
WUU
APPLICATIONS INFORMATION
or power plane layer either inside or on the opposite side of the board. Copper board stiffeners and plated through­holes can also be used to spread the heat generated by the device. Table 1 lists the thermal resistance for several different board sizes and copper areas. All measurements were taken in still air on 3/32" FR-4 board with 2oz copper. This data can be used as a rough guideline in estimating thermal resistance. The thermal resistance for each appli­cation will be affected by thermal interactions with other components as well as board size and shape.
Table 1. Fused 16-lead and 8-lead SO Packages
COPPER AREA (2oz)
TOPSIDE BACKSIDE COPPER AREA (16-LEAD) (8-LEAD)
600mm 300mm 100mm
0mm
2
2
2
2
2
2
2
2
2
2500mm22500mm 1000mm22500mm
600mm22500mm 180mm22500mm 180mm21000mm
2
180mm
2
180mm
2
180mm
2
180mm
TOTAL θ
780mm 480mm 280mm 180mm
2
2
2
2
2
2
2
2
2
5000mm 3500mm 3100mm 2680mm 1180mm
JA
40°C/W 80°C/W 46°C/W 92°C/W 48°C/W 96°C/W 49°C/W 98°C/W 56°C/W 112°C/W 58°C/W 116°C/W 59°C/W 118°C/W 60°C/W 120°C/W 61°C/W 122°C/W
θ
JA
thermal resistance is 40°C/W. The junction temperature TJ is:
TJ = (1.24W)(40°C/W) + 85°C = 135°C
The maximum junction temperature for the LT1497 is 150°C, so the heat sinking capability of the board is adequate for the application.
If the copper area on the PC board is reduced to 180mm
2
the thermal resistance increases to 61°C/W and the junc­tion temperature becomes:
TJ = (1.24W)(61°C/W) + 85°C = 161°C
which is above the maximum junction temperature indi­cating that the heat sinking capability of the board is inadequate and should be increased.
Calculating Junction Temperature
The junction temperature can be calculated from the equation:
TJ = (PD)(θJA) + T
A
TJ = Junction Temperature TA = Ambient Temperature PD = Power Dissipation
θJA = Thermal Resistance (Junction-to-Ambient)
As an example, calculate the junction temperature for the circuit in Figure 1 assuming an 85°C ambient temperature.
The device dissipation can be found by measuring the supply currents, calculating the total dissipation and then subtracting the dissipation in the load and feedback net­work. Both amplifiers are in a gain of –1.
The dissipation for each amplifier is:
The total dissipation is 1.24W. When a 2500mm2 PC board with 2oz copper on top and bottom is used, the
PD = (1/2)(86.4mA)(30V) – (10V)2/(200||560) = 0.62W
Figure 1. Thermal Calculation Example
Slew Rate
Unlike a traditional op amp, the slew rate of a current feedback amplifier is not independent of the amplifier gain configuration. There are slew rate limitations in both the input stage and the output stage. In the inverting mode and for higher gains in the noninverting mode, the signal amplitude on the input pins is small and the overall slew rate is that of the output stage. The input stage slew rate is related to the quiescent current in the input devices.
Referring to the Simplified Schematic, for noninverting applications the two current sources in the input stage slew the parasitic internal capacitances at the bases of Q3 and Q4. Consider a positive going input at the base of Q1 and Q2. If the input slew rate exceeds the internal slew rate,
9
LT1497
U
WUU
APPLICATIONS INFORMATION
the normally active emitter of Q2 will turn off as the entire current available from the current source is used to slew the base of Q3. The base of Q4 is driven by Q1 without slew limitation. When the differential input voltage exceeds two diode drops (about 1.4V) the extra clamp emitter on Q1 turns on and drives the base of Q3 directly. Once the base of Q3 has been driven within 1.4V of its final value, the clamp emitter of Q1 turns off and the node must finish slewing using the current source.
This effect can be seen in Figure 2 which shows the large signal behavior in a gain of 1 on ±15V supplies. The clamping action enhances the slew rate beyond the input limitation, but always leads to slew overshoot after the clamps turn off. Figure 3 shows that for higher gain
configurations there is much less slew rate enhancement because the input only moves 2V, barely enough to turn on the input clamps. In inverting configurations as shown in Figure 4 the noninverting input does not move so there is no input slew rate limitation. Slew overshoot is due to capacitance on the inverting input and can be reduced with a larger feedback resistor.
The output slew rate is set by the value of the feedback resistors and the internal capacitance. Larger feedback resistors will reduce the slew rate as will lower supply voltages, similar to the way the bandwidth is reduced. The larger feedback resistors will also cut back on slew overshoot.
AV = 1 V
= ±15V
S
R
= 560
F
= 100
R
L
1497 F02
Figure 2. Large-Signal Response
WW
SI PLIFIED SCHE ATIC
+IN
= ±15V
S
R
= 560
F
R
= 100
L
RG = 62
AV = 10 V
Figure 3. Large-Signal Response
One Amplifier
Q5
Q3
Q2
–IN
Q1
Q4
Q10
Q6
Q11
Q7
Q8
Q9
Q12
1497 F03
R
AV = –1 V
= ±15V
S
= RG = 560
F
R
= 100
L
Figure 4. Large-Signal Response
+
V
Q13
V
OUT
Q14
V
1497 SS
1497 F04
10
U
TYPICAL APPLICATIONS
LT1497
Differential Input/Differential Output Power Amp (AV = 2)
V
IN
+
1/2 LT1497
V
OUT
560
1.1k
560
–V
1497 TA03
OUT
–V
1/2 LT1497
IN
+
U
PACKAGE DESCRIPTION
0.010 – 0.020
(0.254 – 0.508)
0.008 – 0.010
(0.203 – 0.254)
*
DIMENSION DOES NOT INCLUDE MOLD FLASH. MOLD FLASH  
SHALL NOT EXCEED 0.006" (0.152mm) PER SIDE
**
DIMENSION DOES NOT INCLUDE INTERLEAD FLASH. INTERLEAD  FLASH SHALL NOT EXCEED 0.010" (0.254mm) PER SIDE  
× 45°
0.016 – 0.050
0.406 – 1.270
0°– 8° TYP
Dimensions in inches (millimeters) unless otherwise noted.
8-Lead Plastic Small Outline (Narrow 0.150)
0.053 – 0.069
(1.346 – 1.752)
0.014 – 0.019
(0.355 – 0.483)
Paralleling Both Amplifiers for Guaranteed 250mA Output Drive
S8 Package
(LTC DWG # 05-08-1610)
0.004 – 0.010
(0.101 – 0.254)
0.050
(1.270)
TYP
V
IN
0.228 – 0.244
(5.791 – 6.197)
560
560
+
1/2 LT1497
560
+
1/2 LT1497
560
0.189 – 0.197* (4.801 – 5.004)
7
8
1
2
6
3
3
3
1497 TA04
5
0.150 – 0.157** (3.810 – 3.988)
4
SO8 0996
V
OUT
0.010 – 0.020
(0.254 – 0.508)
0.008 – 0.010
(0.203 – 0.254)
*
DIMENSION DOES NOT INCLUDE MOLD FLASH. MOLD FLASH  
SHALL NOT EXCEED 0.006" (0.152mm) PER SIDE
**
DIMENSION DOES NOT INCLUDE INTERLEAD FLASH. INTERLEAD  FLASH SHALL NOT EXCEED 0.010" (0.254mm) PER SIDE  
× 45°
0.016 – 0.050
0.406 – 1.270
(1.346 – 1.752)
0° – 8° TYP
(0.355 – 0.483)
0.053 – 0.069
0.014 – 0.019
Information furnished by Linear Technology Corporation is believed to be accurate and reliable. However, no responsibility is assumed for its use. Linear Technology Corporation makes no represen­tation that the interconnection of its circuits as described herein will not infringe on existing patent rights.
S Package
16-Lead Plastic Small Outline (Narrow 0.150)
(LTC DWG # 05-08-1610)
16
1
0.050
(1.270)
TYP
0.004 – 0.010
(0.101 – 0.254)
(5.791 – 6.197)
0.228 – 0.244
0.386 – 0.394* (9.804 – 10.008)
13
14
15
3
2
12
11 10
5
4
6
7
9
0.150 – 0.157** (3.810 – 3.988)
S16 0695
8
11
LT1497
TYPICAL APPLICATION
±4A Current Boosted Power Amp (AV = 10) Frequency Response of Current Boosted Power Amp
U
15V
3
0.033
Q1 D45VH4
V
OUT
6.2
V
IN
200
+
1/2 LT1497
0.01µF
+
V
1.8K
200
+
1/2 LT1497
6.2
V
1.8k
–15V
3
0.01µF
1497 TA05
Q2 D44VH4
0.033
22 21 20 19 18
17 16
VOLTAGE GAIN (dB)
VS = ±15V
15
= 10
A
V
14
= 1.8k
R
F
= 200Ω
R
G
13
= 6V
V
OUT
12
10k
RL = 50
RL = 2.5
P-P
100k 1M 10M
FREQUENCY (Hz)
1497 TA06
RELATED PARTS
PART NUMBER DESCRIPTION COMMENTS
LT1206 Single 250mA, 60MHz Current Feedback Amplifier Shutdown Function, Stable with CL = 10,000pF,
900V/µs Slew Rate
LT1207 Dual 250mA, 60MHz Current Feedback Amplifier Dual Version of LT1206 LT1210 Single 1A, 30MHz Current Feedback Amplifier Higher Output Version of LT1206 LT1229/LT1230 Dual/Quad 100MHz Current Feedback Amplifiers 30mA Output Current, 1000V/µs Slew Rate LT1363/LT1364/LT1365 Single/Dual/Quad 70MHz, 1000V/µs, C-LoadTM Amplifiers 50mA Output Current, 1.5mV Max VOS, 2µA Max I C-Load is a trademark of Linear Technology Corporation.
B
12
Linear Technology Corporation
1630 McCarthy Blvd., Milpitas, CA 95035-7417 ● (408) 432-1900 FAX: (408) 434-0507
TELEX: 499-3977 ● www.linear-tech.com
1497f LT/TP 1097 4K • PRINTED IN USA
LINEAR TECHNOLOGY CORPORATION 1997
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