MR752RLG

MR750 SERIES
http://onsemi.com
4
Figure 5. Maximum Current Ratings
T
L
, LEAD TEMPERATURE (°C)
0
8.0
I
F(AV)
0
12
20
28
40 80 120 160 200
Figure 6. Maximum Current Ratings
0 8.0
4.0
0
16 24 32
I
F(AV)
, AVERAGE FORWARD CURRENT (AMPS)
P
F(AV)
Figure 7. Power Dissipation
, POWER DISSIPATION (WATTS)
5/8"
, AVERAGE FORWARD CURRENT (AMPS)
CAPACITANCE LOADS
8.0
12
16
RESISTIVE INDUCTIVE
LOADS
T
A
, AMBIENT TEMPERATURE (°C)
0
1.0
I
F(AV)
0
2.0
3.0
4.0
40 80 120 160 200
Figure 8. Steady State Thermal Resistance
f = 60 Hz
, AVERAGE FORWARD CURRENT (AMPS)
RESISTIVE INDUCTIVE LOADS
CAPACITANCE LOADS − 1 & 3
20
6
1 & 3
20 I
avg
T
A(A)
T
A(K)
T
L(A)
T
C(A)
T
J
T
C(K)
T
L(K)
P
F
R
S(A)
R
L(A)
R
J(A)
R
J(K)
R
L(K)
R
S(K)
Use of the above model permits junction to lead thermal resistance for
any mounting configuration to be found. Lowest values occur when one
side of the rectifier is brought as close as possible to the heat sink as
shown below. Terms in the model signify:
T
A
= Ambient Temperature T
C
= Case Temperature
T
L
= Lead Temperature T
J
= Junction Temperature
R
S
= Thermal Resistance, Heat Sink to Ambient
R
L
= Thermal Resistance, Lead to Heat Sink
R
J
= Thermal Resistance, Junction to Case
P
F
= Power Dissipation
(Subscripts A and K refer to anode and cathode sides, respectively.)
Values for thermal resistance components are:
R
L
= 40°C/W/in. Typically and 44°C/W/in Maximum.
R
J
= 2°C/W typically and 4°C/W Maximum.
Since R
J
is so low, measurements of the case temperature, T
C
, will be
approximately equal to junction temperature in practical lead mounted
applications. When used as a 60 Hz rectifierm the slow thermal response
holds T
J(PK)
close to T
J(AVG)
. Therefore maximum lead temperature may
be found from: T
L
= 175°−R
JL
P
F
. P
F
may be found from Figure 7.
The recommended method of mounting to a P.C. board is shown on the
sketch, where R
JA
is approximately 25°C/W for a 1−1/2" x 1−1/2" copper
surface area. Values of 40°C/W are typical for mounting to terminal strips
or P.C. boards where available surface area is small.
Board Ground Plane
Recommended mounting for half wave circuit
24
28
32
0 1/4
5.0
0
1/2 3/4 1.0
L, LEAD LENGTH (INCHES)
R
JL
, THERMAL RESISTANCE,
SINGLE LEAD TO HEAT SINK,
INSIGNIFICANT HEAT FLOW
THROUGH OTHER LEAD
10
15
20
25
30
35
40
24
16
4.0
20 60 100 140 180
4.0 12 20 28
1/8 3/8 5/8 7/8
θ
JUNCTION−TO−LEAD( C/W)
°
BOTH LEADS TO HEAT
SINK WITH LENGTHS
AS SHOWN
3/8"
1/4"
L = 1/8"
20 60 100 140 180
5.0
6.0
7.0
I
(pk)
= 5 I
avg
I
(pk)
= 10 I
avg
I
(pk)
= 20 I
avg
10 I
avg
I
(pk)
= 5 I
avg
RESISTIVE − INDUCTIVE LOADS
BOTH LEADS TO HEAT
SINK, EQUAL LENGTH
6 (I
PK
/I
AVE
= 6.28)
SEE NOTE
R
JA
= 40°C/W
SEE NOTE
R
JA
= 25°C/W
NOTES
THERMAL CIRCUIT MODEL
(For Heat Conduction Through The Leads)
MR750 SERIES
http://onsemi.com
5
Figure 9. Rectification Efficiency Figure 10. Reverse Recovery Time
REPETITION FREQUENCY (kHz)
2.01.0
100
50
30
20
703.0 5.0 100
RELATIVE EFFICIENCY (%)
70
7.0 10 20 30 50
T
J
= 25°C
CURRENT INPUT WAVEFORM
I
R
/I
F
, RATIO OF REVERSE TO FORWARD CURRENT
0.20.1
20
7.0
5.0
2.0
1.0
7.00.3 0.5 10
3.0
t
rr
, REVERSE RECOVERY TIME ( s)
10
0.7 1.0 2.0 3.0 5.0
T
J
= 25°C
I
F
= 5 A
3 A
1 A
I
F
0
I
R
t
rr
Figure 11. Junction Capacitance Figure 12. Forward Recovery Time
V
R
, REVERSE VOLTAGE (VOLTS)
1.0 3.0
500
300
200
100
70
50
2.0
C, CAPACITANCE (pF)
10 20 1007.05.0 5030
T
J
= 25°C
1.0
I
F
, FORWARD PULSE CURRENT (AMP)
0.7
0.5
0.3
0.2
0.1
2.0
, FORWARD RECOVERY TIME ( s)t
fr
5.03.0
1.0
7.0 10
fr
= 1.0 V
T
J
= 25°C
fr
f
t
fr
T
J
= 175°C
30
700
1000
30
20
10
70
fr
= 2.0 V
R
S
R
L
V
O
Figure 13. Single−Phase Half−Wave
Rectifier Circuit
The rectification efficiency factor σ shown in Figure 9
was calculated using the formula:
σ +
P
(dc)
P
(rms)
+
V
2
o
(dc)
R
L
V
2
o
(rms)
R
L
.
100%+
V
2
o
(dc)
V
2
o
(ac)
) V
2
o
(dc)
.
100%
(1
)
For a sine wave input V
m
sin (wt) to the diode, assumed
lossless, the maximum theoretical efficiency factor becomes:
σ
(sine)
+
V
2
m
2
R
L
V
2
m
4R
L
.
100% +
4
π
2
.
100% + 40.6% (2)
For a square wave input of amplitude V
m
, the efficiency
factor becomes:
σ
(square)
+
V
2
m
2
R
L
V
2
m
R
L
.
100% + 50% (3)
(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 10) becomes
significant, resulting in an increasing AC voltage
component across R
L
which is opposite in polarity to the
forward current, thereby reducing the value of the efficiency
factor σ, as shown on Figure 9.
It should be emphasized that Figure 9 shows waveform
efficiency only; it does not provide a measure of diode
losses. Data was obtained by measuring the AC component
of V
o
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 9.
MR750 SERIES
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6
ORDERING INFORMATION
Device Package Shipping
MR750 Axial Lead
1000 Units / Box
MR750G Axial Lead
(Pb−Free)
MR750RL Axial Lead
800 / Tape & Reel
MR750RLG Axial Lead
(Pb−Free)
MR751 Axial Lead
1000 Units / Box
MR751G Axial Lead
(Pb−Free)
MR751RL Axial Lead
800 / Tape & Reel
MR751RLG Axial Lead
(Pb−Free)
MR752 Axial Lead
1000 Units / Box
MR752G Axial Lead
(Pb−Free)
MR752RL Axial Lead
800 / Tape & Reel
MR752RLG Axial Lead
(Pb−Free)
MR754 Axial Lead
1000 Units / Box
MR754G Axial Lead
(Pb−Free)
MR754RL Axial Lead
800 / Tape & Reel
MR754RLG Axial Lead
(Pb−Free)
MR756 Axial Lead
1000 Units / Box
MR756G Axial Lead
(Pb−Free)
MR756RL Axial Lead
800 / Tape & Reel
MR756RLG Axial Lead
(Pb−Free)
MR760 Axial Lead
1000 Units / Box
MR760G Axial Lead
(Pb−Free)
MR760RL Axial Lead
800 / Tape & Reel
MR760RLG Axial Lead
(Pb−Free)
For information on tape and reel specifications, including part orientation and tape sizes, please refer to our Tape and Reel Packaging
Specifications Brochure, BRD8011/D.

MR752RLG

Mfr. #:
Manufacturer:
ON Semiconductor
Description:
Rectifiers 200V 6A Silicon
Lifecycle:
New from this manufacturer.
Delivery:
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