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PDF NRVBB30H30CT-1G Data sheet ( Hoja de datos )

Número de pieza NRVBB30H30CT-1G
Descripción Switch-mode Power Rectifiers
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No Preview Available ! NRVBB30H30CT-1G Hoja de datos, Descripción, Manual

MBRB30H30CT-1G,
NRVBB30H30CT-1G,
MBR30H30CTG
Switch-mode
Power Rectifiers
30 V, 30 A
Features and Benefits
Low Forward Voltage
Low Power Loss/High Efficiency
High Surge Capacity
150°C Operating Junction Temperature
30 A Total (15 A Per Diode Leg)
Guard−Ring for Stress Protection
NRVBB Prefix for Automotive and Other Applications Requiring
Unique Site and Control Change Requirements; AEC−Q101
Qualified and PPAP Capable
These Devices are Pb−Free and are RoHS Compliant
Applications
Power Supply − Output Rectification
Power Management
Instrumentation
Mechanical Characteristics:
Case: Epoxy, Molded
Epoxy Meets UL 94 V−0 @ 0.125 in
Weight: 1.5 Grams (I2PAK) (Approximately)
1.9 Grams (TO−220) (Approximately)
Finish: All External Surfaces Corrosion Resistant and Terminal
Leads are Readily Solderable
Lead Temperature for Soldering Purposes:
260°C Max. for 10 Seconds
www.onsemi.com
SCHOTTKY BARRIER
RECTIFIER
30 AMPERES, 30 VOLTS
1
2, 4
3
4 MARKING
DIAGRAMS
1 23
I2PAK (TO−262)
CASE 418D
STYLE 3
AYWW
B30H30G
AKA
4
1
2
3
TO−220
CASE 221A
STYLE 6
AYWW
B30H30G
AKA
A = Assembly Location
Y = Year
WW = Work Week
B30H30 = Device Code
G = Pb−Free Package
AKA = Diode Polarity
ORDERING AND MARKING INFORMATION
See detailed ordering and shipping information on page 5 of
this data sheet.
© Semiconductor Components Industries, LLC, 2015
January, 2015 − Rev. 6
1
Publication Order Number:
MBRB30H30CT−1/D

1 page




NRVBB30H30CT-1G pdf
MBRB30H30CT−1G, NRVBB30H30CT−1G, MBR30H30CTG
MERCURY
SWITCH
S1
+VDD
IL 10 mH COIL
ID
DUT
VD
IL
t0
BVDUT
ID
VDD
t1 t2 t
Figure 9. Test Circuit
The unclamped inductive switching circuit shown in
Figure 9 was used to demonstrate the controlled avalanche
capability of this device. A mercury switch was used instead
of an electronic switch to simulate a noisy environment
when the switch was being opened.
When S1 is closed at t0 the current in the inductor IL ramps
up linearly; and energy is stored in the coil. At t1 the switch
is opened and the voltage across the diode under test begins
to rise rapidly, due to di/dt effects, when this induced voltage
reaches the breakdown voltage of the diode, it is clamped at
BVDUT and the diode begins to conduct the full load current
which now starts to decay linearly through the diode, and
goes to zero at t2.
By solving the loop equation at the point in time when S1
is opened; and calculating the energy that is transferred to
the diode it can be shown that the total energy transferred is
equal to the energy stored in the inductor plus a finite amount
of energy from the VDD power supply while the diode is in
breakdown (from t1 to t2) minus any losses due to finite
component resistances. Assuming the component resistive
Figure 10. Current−Voltage Waveforms
elements are small Equation (1) approximates the total
energy transferred to the diode. It can be seen from this
equation that if the VDD voltage is low compared to the
breakdown voltage of the device, the amount of energy
contributed by the supply during breakdown is small and the
total energy can be assumed to be nearly equal to the energy
stored in the coil during the time when S1 was closed,
Equation (2).
EQUATION (1):
ǒ ǓWAVAL [
1
2
LI
2
LPK
BVDUT
BVDUT–VDD
EQUATION (2):
WAVAL
[
1
2
LI
2
LPK
ORDERING INFORMATION
Device
MBRB30H30CT−1G
NRVBB30H30CT−1G
MBR30H30CTG
Package
TO−262
(Pb−Free)
TO−262
(Pb−Free)
TO−220
(Pb−Free)
Shipping
50 Units / Rail
50 Units / Rail
50 Units / Rail
www.onsemi.com
5

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