Gate driving circuit for power semiconductor switch

Miscellaneous active electrical nonlinear devices – circuits – and – Signal converting – shaping – or generating – Having specific delay in producing output waveform

Reexamination Certificate

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Details

C327S428000, C327S438000

Reexamination Certificate

active

06268754

ABSTRACT:

BACKGROUND OF THE INVENTION
1. Field of the Invention
The present invention relates to a gate driving circuit for a power semiconductor switch, and more particularly to a pulse driving circuit for driving abruptly or steeply a power semiconductor switch into a conductive state at a very high speed.
2. Description of the Related Art
In the power energy field, there has been developed a pulse power technique. In the pulse power technique, energy is first stored at a very slow rate, and then the stored energy is instantaneously discharged within an extremely short time period such as 100 nano-seconds to obtain extremely high power not less than 10
8
Watts. In order to discharge a large amount of energy as fast as possible, it is required to provide a high speed switching element which can operate at a high voltage. To this end, there have been proposed to utilize gap switch and thyratron. However, these switches could not be operated at a sufficiently high frequency and a life time of these switches is rather short.
Recently there have been developed various kinds of power semiconductor switching elements such as thyristor, static induction thyristor, gate turn-off thyristor (GTO) and insulated-gate bipolar transistor (IGBT), which have a high speed switching property at a rather high voltage and a relatively large current. These power semiconductor switching elements have been practically used. Particularly, a series circuit of these power semiconductor switching elements could be utilized as a high voltage power semiconductor switch for the pulse power application.
In order to drive the above mentioned power semiconductor switch in a pulse mode, the switch has to be turn-on as fast as possible. To this end, upon triggering, a large current raising very sharply must flow into a gate of the power semiconductor switch for an initial short time period of several tens nano-seconds (ns), and then an on-current of about 1 A has to be flown continuously for about 50 micro-seconds (&mgr;s). There have been proposed several gate driving circuits which can drive the power semiconductor switch in the pulse mode just explained above.
FIG. 1
is an example of known gate driving circuits for driving a power semiconductor switch in a pulse mode. A first DC voltage source
1
for turning-on a semiconductor switch and a second DC voltage source
2
for turning-off a semiconductor switch are provided. A series circuit of a resistor
3
and a capacitor
4
is connected across the turn-on DC voltage source
1
, and a junction point between the resistor
3
and the capacitor
4
is coupled with a gate G of a power semiconductor switch
6
by means of a turn-on switching element
5
. A stray inductance contained in a circuit portion from the DC voltage source to the gate G of the power semiconductor switch
6
is represented as an inductor
7
which is connected between the turn-on switching element
5
and the gate G of the power semiconductor switch
6
.
The above mentioned resistor
3
serves not only as a charging resistor for the capacitor
4
but also as a resistor for supplying a current to the gate G of the power semiconductor switch
6
for maintaining the power semiconductor switch in the conducting state. A cathode K of the power semiconductor switch
6
is connected to a negative terminal of the turn-on DC voltage source
1
, and a junction point between the turn-on switching element
5
and the inductor
7
is coupled with a negative terminal of the turn-off DC voltage source
2
by means of a turn-off switching element
8
. The turn-on and turn-off switching elements
5
and
8
are controlled by a control circuit
9
.
Now the operation of the known gate driving circuit illustrated in
FIG. 1
will be explained with reference to signal waveforms shown in FIG.
2
. When the power semiconductor switch
6
is in the non-conducting state, the turn-on switching element
5
(SW
5
) is made off and the turn-off switching element
8
(SW
8
) is made on under the control of the control circuit
9
. Therefore, the capacitor
4
is charged by the turn-on DC voltage source
1
by means of the resistor
3
to a voltage E
1
which is equal to the output voltage of the turn-on DC voltage source
1
.
At a time instant t
0
, the turn-on switching element
5
is switched from “off” to “on”, and then energy stored in the capacitor
4
flows through the turn-on switching element
5
to the gate G of the power semiconductor switch
6
, and further flows to the cathode K of the semiconductor switch. A maximum value of the current flowing from the gate G to the cathode K of the power semiconductor switch
6
is denoted as I
2
in FIG.
2
. Since the large current I
2
flows to the gate G of the power semiconductor switch
6
, this switch is turned-on and a large current flows through the anode-cathode A-K path by means of main DC voltage supply source not shown. After that, the power semiconductor switch
6
is kept conductive as long as the current flows into the gate G of the power semiconductor switch. At an instant t
1
, the turn-on switching element
5
is turned-off and the turn-off switching element
8
is turned-on by the control circuit
9
, and then the power semiconductor switch
6
is turned-off.
A raising rate (di
G
/dt) of the gate current I
G
flowing into the gate G of the power semiconductor switch
6
when the turn-on switching element
5
is made on, is determined by the voltage E
1
of the turn-on DC voltage source
1
and the stray inductance L
S
denoted by the inductor
7
in FIG.
1
. That is to say, the raising rate (di
G
/dt) can be expressed by di
G
/dt=E
1
/L
S
. Usually the stray inductance L
S
is about 100 nH and the raising rate (di
G
/dt) of the gate current is required not less than 3000 A/&mgr;s. Therefore, the voltage E
1
of the turn-on DC voltage source
1
has to be not lower than 300 V.
An amount of charge Q to be supplied to the gate G of the power semiconductor switch
6
for turning-on the power semiconductor switch at a high speed is determined by respective switches. This amount of charge Q is identical with an amount of charge stored in the capacitor
4
, and its energy is represented by ½×QE
1
. An energy loss in the resistor
3
for storing such energy is also expressed by ½×QE
1
. Therefore, the turn-on DC voltage source
1
has to supply a sum of these energy and is equal to QE
1
.
Now it is assumed that the capacitor
4
has a capacitance of 0.5 &mgr;F and a pulse repetition frequency is 2 KHz. Then the turn-on DC voltage source
1
must supply a power of 90 W. Since the turn-on DC voltage source
1
must supply the current for keeping the power semiconductor switch
6
conductive for 50 &mgr;s, and this current amounts to a power of 30 W. Therefore, the turn-on voltage source
1
must supply a sum of these powers which amounts to a very large value of 120 W.
SUMMARY OF THE INVENTION
The present invention has for its object to provide a novel and useful gate driving circuit for a power semiconductor switch, in which the above mentioned drawbacks of the known gate driving circuits and the semiconductor switch can be driven in the pulse mode by flowing abruptly a large current to a gate of the power semiconductor switch.
According to the invention, a gate driving circuit for driving a power semiconductor switch in a pulse mode comprises:
a DC voltage source having first and second output terminals, said first output terminal being connected to a main electrode of a power semiconductor switch;
a series circuit of a reactor and a first switching element, said series circuit being connected across the main electrode and a gate of the power semiconductor switch;
a second switching element connected across the gate of the power semiconductor switch and said second output terminal of the DC voltage source; and
a control circuit for controlling said first and second switching elements such that said power semiconductor switch is kept in non-conductive by making said first and second switching elements in off-state and in on-state, re

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