MMDF2C03HDR2 ON Semiconductor, MMDF2C03HDR2 Datasheet - Page 7

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MMDF2C03HDR2

Manufacturer Part Number
MMDF2C03HDR2
Description
MOSFET N/P-CH 30V 3A 8-SOIC
Manufacturer
ON Semiconductor
Datasheet

Specifications of MMDF2C03HDR2

Fet Type
N and P-Channel
Fet Feature
Logic Level Gate
Rds On (max) @ Id, Vgs
70 mOhm @ 3A, 10V
Drain To Source Voltage (vdss)
30V
Current - Continuous Drain (id) @ 25° C
4.1A, 3A
Vgs(th) (max) @ Id
3V @ 250µA
Gate Charge (qg) @ Vgs
16nC @ 10V
Input Capacitance (ciss) @ Vds
630pF @ 24V
Power - Max
2W
Mounting Type
Surface Mount
Package / Case
8-SOIC (3.9mm Width)
Configuration
Dual Dual Drain
Transistor Polarity
N and P-Channel
Resistance Drain-source Rds (on)
0.07 Ohms
Forward Transconductance Gfs (max / Min)
3.6 S
Drain-source Breakdown Voltage
30 V
Gate-source Breakdown Voltage
+/- 20 V
Continuous Drain Current
4.1 A, - 3 A
Power Dissipation
2 W
Maximum Operating Temperature
+ 150 C
Mounting Style
SMD/SMT
Fall Time
23 ns, 194 ns
Minimum Operating Temperature
- 55 C
Rise Time
65 ns, 18 ns
Lead Free Status / RoHS Status
Contains lead / RoHS non-compliant
Other names
MMDF2C03HDR2OSTR

Available stocks

Company
Part Number
Manufacturer
Quantity
Price
Part Number:
MMDF2C03HDR2G
Manufacturer:
ON/安森美
Quantity:
20 000
are very important in systems using it as a freewheeling or
commutating diode. Of particular interest are the reverse
recovery characteristics which play a major role in
determining switching losses, radiated noise, EMI and RFI.
the body diode itself. The body diode is a minority carrier
device, therefore it has a finite reverse recovery time, t
to the storage of minority carrier charge, Q
the typical reverse recovery wave form of Figure 15. It is this
stored charge that, when cleared from the diode, passes
through a potential and defines an energy loss. Obviously,
repeatedly forcing the diode through reverse recovery
further increases switching losses. Therefore, one would
like a diode with short t
minimize these losses.
amount of radiated noise, voltage spikes, and current
ringing. The mechanisms at work are finite irremovable
circuit parasitic inductances and capacitances acted upon by
The switching characteristics of a MOSFET body diode
System switching losses are largely due to the nature of
The abruptness of diode reverse recovery effects the
3.0
2.5
2.0
1.5
1.0
0.5
0
0.5
Figure 10. Diode Forward Voltage versus Current
T
V
J
GS
= 25°C
0.55
= 0 V
V
SD
, SOURCE−TO−DRAIN VOLTAGE (VOLTS)
0.6
rr
N−Channel
0.65
and low Q
DRAIN−TO−SOURCE DIODE CHARACTERISTICS
0.7
RR
0.75
specifications to
RR
, as shown in
0.8
http://onsemi.com
MMDF2C03HD
rr
, due
0.85
7
high di/dts. The diode’s negative di/dt during t
controlled by the device clearing the stored charge.
However, the positive di/dt during t
diode characteristic and is usually the culprit that induces
current ringing. Therefore, when comparing diodes, the
ratio of t
abruptness and thus gives a comparative estimate of
probable noise generated. A ratio of 1 is considered ideal and
values less than 0.5 are considered snappy.
low voltage MOSFETs, high cell density MOSFET diodes
are faster (shorter t
reverse recovery characteristic. The softness advantage of
the high cell density diode means they can be forced through
reverse recovery at a higher di/dt than a standard cell
MOSFET diode without increasing the current ringing or the
noise generated. In addition, power dissipation incurred
from switching the diode will be less due to the shorter
recovery time and lower switching losses.
1.6
1.2
0.8
0.4
Compared to ON Semiconductor standard cell density
2
0
0.5
Figure 10. Diode Forward Voltage versus Current
T
V
J
GS
= 25°C
0.7
b
= 0 V
/t
V
a
SD
serves as a good indicator of recovery
, SOURCE−TO−DRAIN VOLTAGE (VOLTS)
0.9
rr
), have less stored charge and a softer
1.1
P−Channel
1.3
b
is an uncontrollable
1.5
a
1.7
is directly
1.9

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