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PDF MR2502 Data sheet ( Hoja de datos )

Número de pieza MR2502
Descripción (MR2502 - MR2510) Medium-Current Silicon Rectifiers
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MR2502, MR2504, MR2510
MR2504 and MR2510 are Preferred Devices
Medium-Current
Silicon Rectifiers
. . . compact, highly efficient silicon rectifiers for medium–current
applications requiring:
High Current Surge — 400 Amperes @ TJ = 175°C
Peak Performance @ Elevated Temperature — 25 Amperes @
TC = 150°C
Low Cost
Compact, Molded Package — For Optimum Efficiency in a Small
Case Configuration
Mechanical Characteristics:
Case: Epoxy, Molded
Weight: 1.8 grams (approximately)
Finish: All External Surfaces Corrosion Resistant and Terminals are
Readily Solderable
Lead Temperature for Soldering Purposes: requires a custom
temperature soldering profile
Polarity: Cathode Polarity Band
Shipped 5000 units per box
MAXIMUM RATINGS
Please See the Table on the Following Page
www.DataSheet4U.com
http://onsemi.com
MEDIUM–CURRENT
SILICON RECTIFIERS
25 AMPERES
200–1000 VOLTS
DIFFUSED JUNCTION
MICRODE BUTTON
CASE 193
MARKING DIAGRAM
MR25xx LYYWW
MR25xx = Device Code
xx = 02, 04 or 10
L = Location Code
YY = Year
WW = Work Week
ORDERING INFORMATION
Device
Package
Shipping
MR2502
Microde Button 5000 Units/Box
MR2504
Microde Button 5000 Units/Box
MR2510
Microde Button 5000 Units/Box
Preferred devices are recommended choices for future use
and best overall value.
© Semiconductor Components Industries, LLC, 2000
October, 2000 – Rev. 3
1
Publication Order Number:
MR2500/D

1 page




MR2502 pdf
MR2502, MR2504, MR2510
60
40 TJ = 25°C
20
CURRENT INPUT WAVEFORM
10
8.0
6.0
1.0
2.0 3.0 5.0 7.0 10
20 30 50 70 100
f, FREQUENCY (kHz)
Figure 10. Rectification Waveform Efficiency
RECTIFICATION EFFICIENCY NOTE
RS
RL VO
Figure 11. Single–Phase Half–Wave Rectifier Circuit
The rectification efficiency factor σ shown in Figure 10
was calculated using the formula:
σ
+
P(dc)
P(rms)
+
V2o(dc)
RL
V2o(rms)
.100%
+
V2o(dc)
V2o(ac) ) V2o(dc)
(1)
.100%
RL
For a sine wave input Vm sin (ωt) to the diode, assume
lossless, the maximum theoretical efficiency factor
becomes:
V2m
σ(sine)
+
p2RL
V2m
.100%
+
4
π2
.100%
+
40.6%
4RL
(2)
For a square wave input of amplitude Vm, the efficiency
factor becomes:
V2m
σ(square)
+
2RL
V2m
.100%
+
50%
(3)
RL
(A full wave circuit has twice these efficiencies)
As the frequency of the input signal is increased, the
reverse recovery time of the diode (Figure 9) becomes
significant, resulting in an increasing ac voltage component
across RL which is opposite in polarity to the forward
current, thereby reducing the value of the efficiency factor
σ, as shown on Figure 10.
It should be emphasized that Figure 10 shows waveform
efficiency only; it does not provide a measure of diode
losses. Data was obtained by measuring the ac component of
VO with a true rms ac voltmeter and the dc component with
a dc voltmeter. The data was used in Equation 1 to obtain
points for Figure 10.
http://onsemi.com
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