LT1497CS8#TRPBF

7
LT1497
Settling Time to 10mV
vs Output Step
Spot Noise Voltage and Current
vs Frequency
SETTLING TIME (ns)
0
OUTPUT STEP (V)
2
6
10
80
1497 G16
–2
–6
0
4
8
–4
–8
–10
20
40
60
100
A
V
= –1
A
V
= –1
A
V
= 1
A
V
= 1
V
S
= ±15V
R
F
= 560
FREQUENCY (Hz)
10 100
1
SPOT NOISE (nV/Hz OR pA/Hz)
10
100
1k 10k 100k
1497 G18
–i
n
+i
n
e
n
Settling Time to 1mV
vs Output Step
SETTLING TIME (ns)
0
OUTPUT STEP (V)
2
6
10
200
1497 G17
–2
–6
0
4
8
–4
–8
–10
50
100
150
250
175
25
75
125
225
A
V
= –1
A
V
= –1
A
V
= 1
A
V
= 1
V
S
= ±15V
R
F
= 560
TYPICAL PERFORMANCE CHARACTERISTICS
UW
Total Harmonic Distortion
vs Frequency
2nd and 3rd Harmonic Distortion
vs Frequency
FREQUENCY (Hz)
10 100
0.001
TOTAL HARMONIC DISTORTION (%)
0.01
0.10
1k 10k 100k
1497 G19
V
S
= ±15V
R
L
= 100
R
F
= R
G
= 560
V
OUT
= 2V
RMS
V
OUT
= 7V
RMS
FREQUENCY (MHz)
0.1
–100
DISTORTION (dBc)
–90
–80
–70
–60
–20
110
1497 G20
–50
–40
–30
A
V
= 1
2ND
V
S
= ±15V
V
OUT
= 5V
P-P
R
L
= 50
R
F
= 560
A
V
= –1
3RD
A
V
= –1
2ND
A
V
= 1
3RD
3rd Order Intercept vs Frequency
FREQUENCY (MHz)
0
3RD ORDER INTERCEPT (dBm)
15
20
25
30
40
5
10 15 20
1497 G21
25 30
35
10
V
S
= ±15V
R
L
= 50
R
F
= 270Ω
R
G
= 30Ω
PO1 = PO2 = 4dBm
Power Supply Rejection
vs Frequency
Amplifier Crosstalk vs Frequency
Output Impedance vs Frequency
FREQUENCY (Hz)
10k 100k
0.01
OUTPUT IMPEDANCE ()
1
100
1M 10M 100M
1497 G22
0.1
10
V
S
= ±15V
R
F
= R
G
= 1.5k
R
F
= R
G
= 560
FREQUENCY (Hz)
20
POWER SUPPLY REJECTION (dB)
40
50
70
80
10k 1M 10M 100M
1497 G23
0
100k
60
30
10
V
S
= ±15V
R
L
= 50
R
F
= R
G
= 560
POSITIVENEGATIVE
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
V
S
= ±15V
A
V
= 10
R
L
= 100
R
F
= 560Ω
R
G
= 62
8
LT1497
APPLICATIONS INFORMATION
WUU
U
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 imped-
ance 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). Alterna-
tively, 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 ampli-
fier 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 invert-
ing 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) tempera-
ture. 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 con-
stants of the package and the amount of copper on the
board under the package. Raising the ambient tempera-
ture 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 electri-
cally 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
9
LT1497
or power plane layer either inside or on the opposite side
of the board. Copper board stiffeners and plated through-
holes 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 appli-
cation 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
TOTAL θ
JA
θ
JA
TOPSIDE BACKSIDE COPPER AREA (16-LEAD) (8-LEAD)
2500mm
2
2500mm
2
5000mm
2
40°C/W 80°C/W
1000mm
2
2500mm
2
3500mm
2
46°C/W 92°C/W
600mm
2
2500mm
2
3100mm
2
48°C/W 96°C/W
180mm
2
2500mm
2
2680mm
2
49°C/W 98°C/W
180mm
2
1000mm
2
1180mm
2
56°C/W 112°C/W
180mm
2
600mm
2
780mm
2
58°C/W 116°C/W
180mm
2
300mm
2
480mm
2
59°C/W 118°C/W
180mm
2
100mm
2
280mm
2
60°C/W 120°C/W
180mm
2
0mm
2
180mm
2
61°C/W 122°C/W
Calculating Junction Temperature
The junction temperature can be calculated from the
equation:
T
J
= (P
D
)(θ
JA
) + T
A
T
J
= Junction Temperature
T
A
= Ambient Temperature
P
D
= Power Dissipation
θ
JA
= 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 net-
work. Both amplifiers are in a gain of –1.
The dissipation for each amplifier is:
P
D
= (1/2)(86.4mA)(30V) – (10V)
2
/(200||560) = 0.62W
The total dissipation is 1.24W. When a 2500mm
2
PC
board with 2oz copper on top and bottom is used, the
thermal resistance is 40°C/W. The junction temperature
T
J
is:
T
J
= (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 junc-
tion temperature becomes:
T
J
= (1.24W)(61°C/W) + 85°C = 161°C
which is above the maximum junction temperature indi-
cating that the heat sinking capability of the board is
inadequate and should be increased.
APPLICATIONS INFORMATION
WUU
U
COPPER AREA (2oz)
560
15V
560
+
560
560
86.4mA
15V
200
200
1497 F01
+
A
10V
10V
f = 2MHz
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,

LT1497CS8#TRPBF

Mfr. #:
Manufacturer:
Analog Devices Inc.
Description:
High Speed Operational Amplifiers Dual 125mA 50MHz current feedback Amp
Lifecycle:
New from this manufacturer.
Delivery:
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