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Turn Off Snubber Design for High Frequency Modules - Microsemi

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the circuit. The diode and resistor are only used<br />

to prevent instantaneous discharge of the energy<br />

stored in the capacitor while the switch turns on.<br />

Fig.3 Chopper with turn-off snubber circuit<br />

L<br />

As a first step in analyzing the operation of the<br />

snubber, we treat the current in the load during<br />

turn–off as constant. The turn-off sequence with<br />

the snubber is shown in Figure 4.<br />

IM<br />

VC<br />

t0 tf<br />

r<br />

C<br />

D<br />

VM<br />

I CAP<br />

Fig.4 <strong>Turn</strong> off behaviour with snubber circuit<br />

connected across the switch.<br />

During the time interval t0 to tf, current in the<br />

switch decreases while current in the capacitor<br />

increases such that the sum of the currents is<br />

constant.<br />

For simplicity, let us set the time at t0 equal to<br />

zero. At the end of the turn-off time tf, the<br />

voltage across the capacitor is calculated as the<br />

area of a triangle, given by the relationship:<br />

1<br />

V i dt V<br />

tf<br />

M f<br />

Ctf = C Ctf<br />

C∫ ⋅ ⇒ =<br />

(1)<br />

t0= 0<br />

2⋅C t2<br />

I ⋅ t<br />

R<br />

Application Note<br />

APT0404<br />

December 2004<br />

At the end of the interval tf to t2, the capacitor C<br />

is charged up to the voltage VM. It is only during<br />

the last phase (t > t2) that current switches from<br />

C to the freewheeling diode.<br />

During turn-off, snubber diode D conducts, and<br />

the voltage across the capacitor equals the<br />

voltage across the switch (ignoring the small<br />

voltage drop across the snubber diode). During<br />

the interval t0 to tf the capacitor current is<br />

IM ⋅t IM⋅t iC<br />

= = .<br />

tf − t0 tf<br />

The capacitor and switch voltage is<br />

2<br />

1 IM IM⋅t C = Czero Czero<br />

C∫ ⋅ ⋅ + = +<br />

tf 2⋅C⋅tf v t dt V V<br />

where VCzero is a constant of integration that is<br />

solved <strong>for</strong> by evaluating at t = tf.<br />

2<br />

IM⋅tf IM ⋅tf<br />

C = +<br />

t t<br />

Czero = +<br />

=<br />

Czero = Ctf<br />

f 2Ct ⋅ ⋅ f<br />

2C ⋅<br />

v V V V<br />

IM ⋅ tf<br />

Since VCtf<br />

= , VCzero must be zero.<br />

2C ⋅<br />

Substituting VCtf into the equation <strong>for</strong> vC, we get<br />

2<br />

2<br />

IM⋅tf t ⎛ t ⎞<br />

C = ⋅ =<br />

2 Ctf ⎜ ⎟<br />

2C ⋅ tf<br />

⎝ tf⎠<br />

v V<br />

Current in the switch is given by the relationship<br />

⎛ t ⎞<br />

isw = IM⎜1− ⎟<br />

(2)<br />

⎝ tf<br />

⎠<br />

There<strong>for</strong>e the energy dissipated in the transistor<br />

during turn-off, derived from (1) and (2), is<br />

given by:<br />

2<br />

tf tf<br />

⎛ t ⎞ ⎛ t ⎞<br />

off ∫ sw C Ctf M<br />

0 ∫ ⎜ ⎟ ⎜ ⎟<br />

0 ⎝ tf ⎠ ⎝ tf<br />

⎠<br />

E = i ⋅v ⋅ dt = V ⋅I 1− ⋅ ⋅dt<br />

= ∫<br />

=<br />

2 ⎛ I M ⋅ t<br />

⎜<br />

⎜<br />

⎝<br />

2⋅<br />

C<br />

2<br />

I M ⋅t<br />

f<br />

⋅<br />

2⋅<br />

C<br />

tf f<br />

⎞ ⎛<br />

⎟ ⋅⎜1<br />

−<br />

⎟ ⎜<br />

⎠ ⎝<br />

APT website www.advancedpower.com – http://www.advancedpower.com<br />

2/5<br />

0<br />

1<br />

12<br />

2<br />

t<br />

t<br />

f<br />

⎞ ⎛<br />

⎟ ⋅⎜<br />

⎟ ⎜<br />

⎠ ⎝<br />

t<br />

t<br />

f<br />

2<br />

⎞<br />

⎟ . dt<br />

⎟<br />

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