State / push-pull input L6374
10/19
10 State / push-pull input
The input 3st/Pp is instead intended for a digital incoming signal. It has an internal threshold
set at 1.26 V; an internal bias circuit (10 mA typical) simulates a high level (three-state) if the
pin is disconnected.
Figure 4. Equivalent input circuit
Figure 5. Input comparator threshold
V
ref
V
i
V
s
V
out
H
ys2
H
ys2
22
D94IN073
L6374 The switching of the output stage
11/19
11 The switching of the output stage
The cross conduction of the two transistors of an output stage of the L6374 would be
significantly noisy, because the transistors here can carry peak currents in excess of
100 mA, and even more in the few nanoseconds before the current limiting circuits are really
effective.
Consequently the device has been designed so as to avoid such cross conduction. At every
switching transition, first of all the transistor in conduction is turned OFF. Then, after a safe
interval of around 200 ns, the other transistor is turned on.
When analyzing the switching cycle, and the associated switching times, it is useful to
identify some subsequent phases:
delay from the input pin to the output reaction;
OFF transition in the output stage;
dead time
on transition in the output stage.
Figure 6. V
S
= 35 V, 350 connected to V
S
/2.
Figure 6 helps understand such sequence. In fact, with a purely resistive load connected to
V
s
/2 no parasitic elements interfere significantly. The waveform can be significantly less
easy to in terpret if the load has not the perfect symmetry of that case, as showed below.
For instance, it is enough to connect the resistive load to ground, or to V
s
– as Figure 7 and
Figure 8 – show to hide some of the switching phases described.
If the load is connected to ground, the waveform stays stuck to ground as long as the output
stage is in high impedance; viceversa when the load is connected to Vs the waveform will
linger close to the supply voltage as long as possible.
If an output load made of an inductor and a resistor in series is used, the inductive kick at
the beginning of every output transition generates the equivalent effect of an "anticipated"
The switching of the output stage L6374
12/19
switching when the inductor can discharge; while the switching looks "delayed" if the output
transition tends to initiate a charging phase (see Figure 9). With a load almost free from
parasitic elements, the waveforms resemble the ones of the purely resistive cases.
With a real, more composite load, the effect of the inductive kick in comparison to the
resistive load, would be more apparent.
With a capacitor and a resistor in parallel as a load, another type of waveform can be seen
(reported in Figure 10).
As long as the output stage stays in the transient high impedance state, the output voltage
will follow the classic exponential law of an RC relaxation.
As soon as the other transistor is switched on and takes charge, the waveform is quickly
forcibly brought to its steady state value.
From the above it is possible to see how the switching times, inherently very fast, of the
output stages, may be difficult to identify in a waveform if the output load is not accurately
taken into consideration.
Figure 11 show typical switching waveform for inputs and outputs.
Figure 7. V
S
= 35 V, 350 connected to ground

L6374FP013TR

Mfr. #:
Manufacturer:
STMicroelectronics
Description:
Buffers & Line Drivers Industrial Quad Line
Lifecycle:
New from this manufacturer.
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