H-bridge shoot-through

ID: h-bridge-shoot-through

H-bridge shoot-through is unintended conduction directly between the supply rails through devices in the same bridge leg. It differs from the intended load-current path through opposite legs of an H-bridge. Overlapping device conduction during switching can create that rail-to-rail path even when the intended logical states never command it. The manufacturer application note explicitly identifies cross-conduction as shorting the supply and introduces nonoverlap timing to prevent it.[ref]
An original lumped fault-loop model shows why a short overlap can matter. Let a previously unenergized parasitic loop have electrical resistance , inductance and constant supply electric potential difference . During overlap,
so
For , the initial ramp is ; the steady resistive value is not reached instantaneously.
Take stipulated , and , giving . An overlap lasting reaches about . The supply delivers
Some of this energy remains in the loop's magnetic field at turn-off; it should not all be labeled heat dissipated in one switch. A overlap in the same ideal model reaches about , illustrating the nonlinear dependence on duration. Device and supply behavior can invalidate these constant-parameter assumptions.
Bridge switching dead time addresses timing overlap by allowing one conduction path to cease before the complementary one starts. An inductive load still needs a recirculation path while the controlled devices are off. TI's primary bridge lesson illustrates current paths during that interval.[ref]
A proposed diagnostic compares actual device control waveforms and supply-current transients with load current during transitions, using a limited-energy test arrangement. A large load current by itself does not identify shoot-through; the timing and path establish the mechanism. The calculated fault-loop pulse is an original model, not an asserted device rating.

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