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Smart Highside High Current Power Switch

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Data Sheet BTS550P<br />

Inverse load current operation<br />

Maximum allowable load inductance for<br />

E AS = IL· L<br />

IL·RL<br />

(V<br />

2·R bb + |V OUT(CL) |) ln (1+<br />

L |V OUT(CL) | ) a single switch off<br />

L = f (I L ); T j,start = 150°C, V bb = 12 V, R L = 0 Ω<br />

V bb<br />

V<br />

bb<br />

- I L<br />

L [µH]<br />

+<br />

IN PROFET OUT<br />

100000<br />

-<br />

IS<br />

V OUT +<br />

V<br />

I IS<br />

IN<br />

10000<br />

-<br />

V IS R IS<br />

1000<br />

The device is specified for inverse load current<br />

operation (V OUT > V bb > 0V). The current sense<br />

feature is not available during this kind of operation<br />

100<br />

(I IS = 0). With I IN = 0 (e.g. input open) only the intrinsic<br />

drain source diode is conducting resulting in<br />

considerably increased power dissipation. If the<br />

10<br />

device is switched on (V IN = 0), this power<br />

dissipation is decreased to the much lower value<br />

R ON(INV) * I 2 (specifications see page 4).<br />

1<br />

Note: Temperature protection during inverse load<br />

current operation is not possible!<br />

1 10 100 1000<br />

I L [A]<br />

Inductive load switch-off energy<br />

Externally adjustable current limit<br />

dissipation<br />

If the device is conducting, the sense current can be<br />

E bb<br />

used to reduce the short circuit current and allow<br />

E AS<br />

higher lead inductance (see diagram above). The<br />

device will be turned off, if the threshold voltage of<br />

E Load T2 is reached by I<br />

V<br />

S<br />

*R IS<br />

. After a delay time defined<br />

bb<br />

by R<br />

i L(t)<br />

V<br />

*C V<br />

T1 will be reset. The device is turned on<br />

V bb<br />

again, the short circuit current is defined by I<br />

IN PROFET OUT<br />

L(SC)<br />

and<br />

the device is shut down after t d(SC)<br />

with latch<br />

E<br />

L function.<br />

IS<br />

L<br />

Z L<br />

{<br />

I IN<br />

R E<br />

V<br />

R L R<br />

bb<br />

IS<br />

V bb<br />

Energy stored in load inductance:<br />

IN PROFET OUT<br />

E L = 1 /2·L·I 2 L<br />

IS<br />

R<br />

While demagnetizing load inductance, the energy<br />

V<br />

R<br />

dissipated in PROFET is<br />

load<br />

IN<br />

E AS = E bb + E L - E R = V ON(CL)·i L (t) dt,<br />

Signal<br />

T1 C V T2<br />

R<br />

IS<br />

Signal<br />

GND<br />

<strong>Power</strong><br />

with an approximate solution for R L > 0 Ω:<br />

GND<br />

Infineon Technologies AG Page 10 2000-Mar-24

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