MOTOROLA 1N5817

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by 1N5817/D
SEMICONDUCTOR TECHNICAL DATA
. . . employing the Schottky Barrier principle in a large area metal–to–silicon
power diode. State–of–the–art geometry features chrome barrier metal,
epitaxial construction with oxide passivation and metal overlap contact. Ideally
suited for use as rectifiers in low–voltage, high–frequency inverters, free
wheeling diodes, and polarity protection diodes.
1N5817 and 1N5819 are
Motorola Preferred Devices
• Extremely Low vF
• Low Stored Charge, Majority Carrier Conduction
• Low Power Loss/High Efficiency
SCHOTTKY BARRIER
RECTIFIERS
1 AMPERE
20, 30 and 40 VOLTS
Mechanical Characteristics
• Case: Epoxy, Molded
• Weight: 0.4 gram (approximately)
• Finish: All External Surfaces Corrosion Resistant and Terminal Leads are
Readily Solderable
• Lead and Mounting Surface Temperature for Soldering Purposes: 220°C
Max. for 10 Seconds, 1/16″ from case
• Shipped in plastic bags, 1000 per bag.
• Available Tape and Reeled, 5000 per reel, by adding a “RL” suffix to the
part number
• Polarity: Cathode Indicated by Polarity Band
• Marking: 1N5817, 1N5818, 1N5819
CASE 59–04
MAXIMUM RATINGS
Rating
Symbol
1N5817
1N5818
1N5819
Unit
Peak Repetitive Reverse Voltage
Working Peak Reverse Voltage
DC Blocking Voltage
VRRM
VRWM
VR
20
30
40
V
Non–Repetitive Peak Reverse Voltage
VRSM
24
36
48
V
VR(RMS)
14
21
28
V
RMS Reverse Voltage
Average Rectified Forward Current (2)
(VR(equiv) ≤ 0.2 VR(dc), TL = 90°C,
RθJA = 80°C/W, P.C. Board Mounting, see Note 2, TA = 55°C)
IO
Ambient Temperature (Rated VR(dc), PF(AV) = 0, RθJA = 80°C/W)
TA
Non–Repetitive Peak Surge Current
(Surge applied at rated load conditions, half–wave, single phase 60 Hz,
TL = 70°C)
Operating and Storage Junction Temperature Range (Reverse Voltage applied)
Peak Operating Junction Temperature (Forward Current applied)
1.0
85
A
80
75
°C
IFSM
25 (for one cycle)
A
TJ, Tstg
–65 to +125
°C
TJ(pk)
150
°C
Symbol
Max
Unit
RθJA
80
°C/W
THERMAL CHARACTERISTICS (2)
Characteristic
Thermal Resistance, Junction to Ambient
ELECTRICAL CHARACTERISTICS (TL = 25°C unless otherwise noted) (2)
Characteristic
Maximum Instantaneous Forward Voltage (1)
(iF = 0.1 A)
(iF = 1.0 A)
(iF = 3.0 A)
Maximum Instantaneous Reverse Current @ Rated dc Voltage (1)
(TL = 25°C)
(TL = 100°C)
Symbol
1N5817
1N5818
1N5819
Unit
vF
0.32
0.45
0.75
0.33
0.55
0.875
0.34
0.6
0.9
V
IR
1.0
10
1.0
10
1.0
10
mA
(1) Pulse Test: Pulse Width = 300 µs, Duty Cycle = 2.0%.
(2) Lead Temperature reference is cathode lead 1/32″ from case.
Preferred devices are Motorola recommended choices for future use and best overall value.
Rev 3
Device
Rectifier
Motorola, Inc.
1996 Data
1
125
Reverse power dissipation and the possibility of thermal runaway
must be considered when operating this rectifier at reverse voltages
above 0.1 VRWM. Proper derating may be accomplished by use of
equation (1).
TA(max) = TJ(max) – RθJAPF(AV) – RθJAPR(AV)
(1)
where TA(max) = Maximum allowable ambient temperature
TJ(max) = Maximum allowable junction temperature
(125°C or the temperature at which thermal
runaway occurs, whichever is lowest)
PF(AV) = Average forward power dissipation
PR(AV) = Average reverse power dissipation
RθJA = Junction–to–ambient thermal resistance
Figures 1, 2, and 3 permit easier use of equation (1) by taking reverse power dissipation and thermal runaway into consideration. The
figures solve for a reference temperature as determined by equation
(2).
TR = TJ(max) – RθJAPR(AV)
(2)
TR, REFERENCE TEMPERATURE ( C)
NOTE 1 — DETERMINING MAXIMUM RATINGS
40
30
23
° 115
105
RθJA (°C/W) = 110
95
80
60
85
75
3.0
2.0
4.0 5.0
7.0
10
VR, DC REVERSE VOLTAGE (VOLTS)
15
20
Figure 1. Maximum Reference Temperature
1N5817
Substituting equation (2) into equation (1) yields:
The factor F is derived by considering the properties of the various rectifier circuits and the reverse characteristics of Schottky diodes.
EXAMPLE: Find TA(max) for 1N5818 operated in a 12–volt dc supply
using a bridge circuit with capacitive filter such that IDC = 0.4 A (IF(AV) =
0.5 A), I(FM)/I(AV) = 10, Input Voltage = 10 V(rms), RθJA = 80°C/W.
125
TR, REFERENCE TEMPERATURE ( C)
TA(max) = TR – RθJAPF(AV)
(3)
Inspection of equations (2) and (3) reveals that TR is the ambient
temperature at which thermal runaway occurs or where TJ = 125°C,
when forward power is zero. The transition from one boundary condition to the other is evident on the curves of Figures 1, 2, and 3 as a
difference in the rate of change of the slope in the vicinity of 115°C. The
data of Figures 1, 2, and 3 is based upon dc conditions. For use in common rectifier circuits, Table 1 indicates suggested factors for an equivalent dc voltage to use for conservative design, that is:
(4)
VR(equiv) = Vin(PK) x F
°
40
105
23
RθJA (°C/W) = 110
80
95
60
85
75
Step 1. Find VR(equiv). Read F = 0.65 from Table 1,
Step 1. Find ∴ VR(equiv) = (1.41)(10)(0.65) = 9.2 V.
Step 2. Find TR from Figure 2. Read TR = 109°C
Step 1. Find @ VR = 9.2 V and RθJA = 80°C/W.
Step 3. Find PF(AV) from Figure 4. **Read PF(AV) = 0.5 W
30
115
3.0
4.0
5.0
7.0
10
15
20
VR, DC REVERSE VOLTAGE (VOLTS)
30
Figure 2. Maximum Reference Temperature
1N5818
125
TR, REFERENCE TEMPERATURE ( C)
I(FM)
@
= 10 and IF(AV) = 0.5 A.
I(AV)
°
Step 4. Find TA(max) from equation (3).
Step 4. Find TA(max) = 109 – (80) (0.5) = 69°C.
**Values given are for the 1N5818. Power is slightly lower for the
1N5817 because of its lower forward voltage, and higher for the
1N5819.
40
30
23
115
105
RθJA (°C/W) = 110
80
95
60
85
75
4.0
5.0
7.0
10
15
20
VR, DC REVERSE VOLTAGE (VOLTS)
30
40
Figure 3. Maximum Reference Temperature
1N5819
Table 1. Values for Factor F
Half Wave
Circuit
Load
Resistive
Sine Wave
0.5
Square Wave
0.75
*Note that VR(PK) ≈ 2.0 Vin(PK).
2
Full Wave, Bridge
Capacitive*
Resistive
Capacitive
Full Wave, Center Tapped* †
Resistive
Capacitive
1.3
0.5
0.65
1.0
1.3
1.5
0.75
0.75
1.5
1.5
† Use line to center tap voltage for Vin.
Rectifier Device Data
PF(AV) , AVERAGE POWER DISSIPATION (WATTS)
R θ JL, THERMAL RESISTANCE, JUNCTION–TO–LEAD (°C/W)
90
BOTH LEADS TO HEATSINK,
EQUAL LENGTH
80
70
60
MAXIMUM
50
TYPICAL
40
30
20
10
1
1/8
1/4
3/8
1/2
5/8
3/4
1.0
7/8
5.0
Sine Wave
I(FM) = π (Resistive Load)
2.0 I(AV)
5
Capacitive
10
1.0
Loads
20
0.7
0.5
3.0
{
SQUARE WAVE
0.3
TJ ≈ 125°C
0.2
0.1
0.07
0.05
0.2
0.4
0.6 0.8 1.0
2.0
IF(AV), AVERAGE FORWARD CURRENT (AMP)
L, LEAD LENGTH (INCHES)
Figure 4. Steady–State Thermal Resistance
r(t), TRANSIENT THERMAL RESISTANCE (NORMALIZED)
dc
4.0
Figure 5. Forward Power Dissipation
1N5817–19
1.0
0.7
0.5
0.3
ZθJL(t) = ZθJL • r(t)
0.2
0.1
Ppk
tp
Ppk
TIME
0.07
0.05
DUTY CYCLE, D = tp/t1
PEAK POWER, Ppk, is peak of an
equivalent square power pulse.
t1
∆TJL = Ppk • RθJL [D + (1 – D) • r(t1 + tp) + r(tp) – r(t1)]
where
∆TJL = the increase in junction temperature above the lead temperature
r(t) = normalized value of transient thermal resistance at time, t, from Figure 6, i.e.:
r(t) = r(t1 + tp) = normalized value of transient thermal resistance at time, t1 + tp.
0.03
0.02
0.01
0.1
0.2
0.5
1.0
2.0
5.0
10
20
50
100
200
500
1.0k
2.0k
5.0k
10k
t, TIME (ms)
Figure 6. Thermal Response
P.C. Board with
1–1/2″ x 1–1/2″
copper surface.
P.C. Board with
1–1/2″ x 1–1/2″
copper surface.
L = 3/8″
L
TYPICAL VALUES FOR RθJA IN STILL AIR
Mounting
Method
Mounting Method 3
Mounting Method 1
NOTE 2 — MOUNTING DATA
Data shown for thermal resistance junction–to–ambient (RθJA) for
the mountings shown is to be used as typical guideline values for preliminary engineering, or in case the tie point temperature cannot be
measured.
L
Lead Length, L (in)
3/4
RθJA
72
85
°C/W
87
100
°C/W
1/8
1/4
1/2
1
52
65
2
67
80
3
50
Mounting Method 2
BOARD GROUND
PLANE
°C/W
L
L
VECTOR PIN MOUNTING
Rectifier Device Data
3
NOTE 3 — THERMAL CIRCUIT MODEL
(For heat conduction through the leads)
RθS(A)
RθL(A)
RθJ(A)
RθJ(K)
TA(A)
RθL(K)
RθS(K)
TA(K)
PD
TL(A)
TC(A)
TJ
TL(K)
TC(K)
Use of the above model permits junction to lead thermal resistance
for any mounting configuration to be found. For a given total lead
length, lowest values occur when one side of the rectifier is brought
as close as possible to the heatsink. Terms in the model signify:
(Subscripts A and K refer to anode and cathode sides, respectively.)
Values for thermal resistance components are:
RθL = 100°C/W/in typically and 120°C/W/in maximum
RθJ = 36°C/W typically and 46°C/W maximum.
TA = Ambient Temperature
TC = Case Temperature
TL = Lead Temperature
TJ = Junction Temperature
RθS = Thermal Resistance, Heatsink to Ambient
RθL = Thermal Resistance, Lead to Heatsink
RθJ = Thermal Resistance, Junction to Case
PD = Power Dissipation
IFSM, PEAK SURGE CURRENT (AMP)
125
20
10
5.0
TC = 100°C
3.0
1 Cycle
TL = 70°C
f = 60 Hz
105
95
85
Surge Applied at
Rated Load Conditions
2.0
25°C
75
1.0
2.0
3.0
20
5.0 7.0 10
NUMBER OF CYCLES
1.0
30
40
70 100
Figure 8. Maximum Non–Repetitive Surge Current
0.7
0.5
30
20
0.3
I R, REVERSE CURRENT (mA)
i F, INSTANTANEOUS FORWARD CURRENT (AMP)
7.0
115
0.2
0.1
0.07
0.05
0.03
0.02
0.1
TJ = 125°C
15
100°C
5.0
3.0
2.0
75°C
1.0
0.5
0.3
0.2
25°C
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1.0 1.1
vF, INSTANTANEOUS FORWARD VOLTAGE (VOLTS)
0.05
0.03
1N5817
1N5818
1N5819
0
4.0
8.0
12
16
20
24
28
32
36
40
VR, REVERSE VOLTAGE (VOLTS)
Figure 7. Typical Forward Voltage
4
Figure 9. Typical Reverse Current
Rectifier Device Data
NOTE 4 — HIGH FREQUENCY OPERATION
200
C, CAPACITANCE (pF)
Since current flow in a Schottky rectifier is the result of majority carrier conduction, it is not subject to junction diode forward and reverse recovery transients due to minority carrier injection and stored charge.
Satisfactory circuit analysis work may be performed by using a model
consisting of an ideal diode in parallel with a variable capacitance. (See
Figure 10.)
Rectification efficiency measurements show that operation will be
satisfactory up to several megahertz. For example, relative waveform
rectification efficiency is approximately 70 percent at 2.0 MHz, e.g., the
ratio of dc power to RMS power in the load is 0.28 at this frequency,
whereas perfect rectification would yield 0.406 for sine wave inputs.
However, in contrast to ordinary junction diodes, the loss in waveform
efficiency is not indicative of power loss: it is simply a result of reverse
current flow through the diode capacitance, which lowers the dc output
voltage.
100
1N5817
70
1N5818
50
1N5819
30
TJ = 25°C
f = 1.0 MHz
20
10
0.4 0.6 0.8 1.0
2.0
4.0 6.0 8.0 10
VR, REVERSE VOLTAGE (VOLTS)
20
40
Figure 10. Typical Capacitance
Rectifier Device Data
5
PACKAGE DIMENSIONS
B
NOTES:
1. ALL RULES AND NOTES ASSOCIATED WITH
JEDEC DO–41 OUTLINE SHALL APPLY.
2. POLARITY DENOTED BY CATHODE BAND.
3. LEAD DIAMETER NOT CONTROLLED WITHIN F
DIMENSION.
D
K
A
DIM
A
B
D
K
MILLIMETERS
MIN
MAX
5.97
6.60
2.79
3.05
0.76
0.86
27.94
–––
INCHES
MIN
MAX
0.235
0.260
0.110
0.120
0.030
0.034
1.100
–––
K
CASE 59–04
ISSUE M
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6
◊
1N5817/D
Rectifier Device
Data