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參數(shù)資料
| 型號(hào)： | MIC4422CN |
| 廠商： | MICREL INC |
| 元件分類： | 功率晶體管 |
| 英文描述： | 9A-Peak Low-Side MOSFET Driver Bipolar/CMOS/DMOS Process |
| 中文描述： | 9 A BUF OR INV BASED MOSFET DRIVER, PDIP8 |
| 封裝： | PLASTIC, DIP-8 |
| 文件頁數(shù)： | 9/10頁 |
| 文件大?。?/td> | 110K |
| 代理商： | MIC4422CN |
MIC4421/4422
Micrel
5-50
April 1998
Transition Power Dissipation
Transition power is dissipated in the driver each time its
output changes state, because during the transition, for a
very brief interval, both the N- and P-channel MOSFETs in
the output totem-pole are ON simultaneously, and a current
is conducted through them from V
S
to ground. The transition
power dissipation is approximately:
P
T
= 2 f V
S
(As)
where (As) is a time-current factor derived from the typical
characteristic curve “Crossover Energy vs. Supply Voltage.”
Total power (P
D
) then, as previously described is just
P
D
= P
L
+ P
Q
+ P
T
Definitions
C
L
=
Load Capacitance in Farads.
D = Duty Cycle expressed as the fraction of time the
input to the driver is high.
f =
Operating Frequency of the driver in Hertz
I
H
= Power supply current drawn by a driver when both
inputs are high and neither output is loaded.
I
L
=
Power supply current drawn by a driver when both
inputs are low and neither output is loaded.
I
D
= Output current from a driver in Amps.
P
D
=
Total power dissipated in a driver in Watts.
P
L
=
Power dissipated in the driver due to the driver’s
load in Watts.
P
Q
= Power dissipated in a quiescent driver in Watts.
P
T
=
Power dissipated in a driver when the output
changes states (“shoot-through current”) in Watts.
NOTE: The “shoot-through” current from a dual
transition (once up, once down) for both drivers is
stated in Figure 7 in ampere-nanoseconds. This
figure must be multiplied by the number of repeti-
tions per second (frequency) to find Watts.
R
O
= Output resistance of a driver in Ohms.
V
S
=
Power supply voltage to the IC in Volts.
Capacitive Load Power Dissipation
Dissipation caused by a capacitive load is simply the energy
placed in, or removed from, the load capacitance by the
driver. The energy stored in a capacitor is described by the
equation:
E = 1/2 C V
2
As this energy is lost in the driver each time the load is
charged or discharged, for power dissipation calculations the
1/2 is removed. This equation also shows that it is good
practice not to place more voltage in the capacitor than is
necessary, as dissipation increases as the square of the
voltage applied to the capacitor. For a driver with a capacitive
load:
P
L
= f C (V
S
)
2
where:
f = Operating Frequency
C = Load Capacitance
V
S
= Driver Supply Voltage
Inductive Load Power Dissipation
For inductive loads the situation is more complicated. For the
part of the cycle in which the driver is actively forcing current
into the inductor, the situation is the same as it is in the
resistive case:
P
L1
= I
2
R
O
D
However, in this instance the R
O
required may be either the
on resistance of the driver when its output is in the high state,
or its on resistance when the driver is in the low state,
depending on how the inductor is connected, and this is still
only half the story. For the part of the cycle when the inductor
is forcing current through the driver, dissipation is best
described as
P
L2
= I V
D
(1 – D)
where V
D
is the forward drop of the clamp diode in the driver
(generally around 0.7V). The two parts of the load dissipation
must be summed in to produce P
L
P
L
= P
L1
+ P
L2
Quiescent Power Dissipation
Quiescent power dissipation (P
Q
, as described in the input
section) depends on whether the input is high or low. A low
input will result in a maximum current drain (per driver) of
≤
0.2mA; a logic high will result in a current drain of
≤
3.0mA.
Quiescent power can therefore be found from:
P
Q
= V
S
[D I
H
+ (1 – D) I
L
]
where:
I
H
= quiescent current with input high
I
L
=
quiescent current with input low
D = fraction of time input is high (duty cycle)
V
S
=
power supply voltage
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