Application Hints
POWER SUPPLY DECOUPLING
The method of supply bypassing is not critical for stability of
the LM6121 series buffers. However, their high current output combined with high slew rate can result in significant
voltage transients on the power supply lines if much inductance is present. For example, a slew rate of 900 V/µs into a
50Ω load produces a di/dt of 18 A/µs. Multiplying this by a
wiring inductance of 50 nH (which corresponds to approximately 1
1
⁄2" of 22 gauge wire) result in a 0.9V transient. To
minimize this problem use high quality decoupling very close
to the device. Suggested values are a 0.1 µF ceramic in parallel with one or two 2.2 µF tantalums.A ground plane is recommended.
LOAD IMPEDANCE
The LM6121 is stable to any load when driven by a 50Ω
source. As shown in the
Overshoot vs Capacitive Load
graph, worst case is a purely capacitive load of about
1000 pF. Shunting the load capacitance with a resistor will
reduce overshoot.
SOURCE INDUCTANCE
Like any high frequency buffer, the LM6121 can oscillate at
high values of source inductance. The worst case condition
occurs at a purely capacitive load of 50 pF where up to
100 nH of source inductance can be tolerated. With a 50Ω
load, this goes up to 200 nH. This sensitivity may be reduced
at the expense of a slight reduction in bandwidth by adding a
resistor in series with the buffer input. A100Ω resistor will ensure stability with source inductances up to 400 nH with any
load.
OVERVOLTAGE PROTECTION
The LM6121 may be severely damaged or destroyed if the
Absolute Maximum Rating of 7V between input and output
pins is exceeded.
If the buffer’s input-to-output differential voltage is allowed to
exceed 7V, a base-emitter junction will be in
reverse-breakdown, and will be in series with a
forward-biased base-emitter junction. Referring to the
LM6121 simplified schematic, the transistors involved are
Q1 and Q3 for positive inputs, and Q2 and Q4 for negative
inputs. If any current is allowed to flow through these junctions, localized heating of the reverse-biased junction will occur, potentially causing damage. The effect of the damage is
typically increased offset voltage, increased bias current,
and/or degraded AC performance. Furthermore, this will defeat the short-circuit and over-temperature protection circuitry. Exceeding
±
7V input with a shorted output will de-
stroy the device.
The device is best protected by the insertion of the parallel
combination of a 100 kΩ resistor (R1) and a small capacitor
(C1) in series with the buffer input, and a 100 kΩ resistor
(R2) from input to output of the buffer (see
Figure 1
). This
network normally has no effect on the buffer output. However,if the buffer’s current limit orshutdown is activated,and
the output has a ground-referred load of significantly less
than 100 kΩ, a large input-to-output voltage may be present.
R1 and R2 then form a voltage divider, keeping the
input-output differential below the 7V Maximum Rating for input voltages up to 14V. This protection network should be
sufficient to protect the LM6121 from the output of nearly any
op amp which is operated on supply voltages of
±
15V or
lower.
Application Hints
HEATSINK REQUIREMENTS
A heatsink may be required with the LM6321 depending on
the maximum power dissipation and maximum ambient temperature of the application. Under all possible operating conditions, the junction temperature must be within the range
specified under Absolute Maximum Ratings.
To determine if a heatsink is required, the maximum power
dissipated by the buffer, P(max), must be calculated. The formula for calculating the maximum allowable power dissipation in any application is P
D
=
(T
J
(max)−TA)/θJA. For the
simple case of a buffer driving a resistive load asin
Figure 2
,
the maximum DC power dissipation occurs when the output
is at half the supply. Assuming equal supplies, the formula is
P
D
=
I
S
(2V+)+V+2/2 RL.
The next parameter which must be calculated is the maximum allowable temperature rise, T
R
(max). This is calculated
by using the formula:
T
R
(max)=TJ(max) − TA(max)
where: T
J
(max) is the maximum allowable junction tem-
perature
T
A
(max) is the maximum ambient temperature
Using the calculated values for T
R
(max) and P(max), the re-
quired value for junction-to-ambient thermal resistance,
θ
(J–A)
, can now be found:
θ
(J–A)
=
T
R
(max)/P(max)
DS009223-6
FIGURE 1. LM6121 with Overvoltage Protection
DS009223-8
FIGURE 2.
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