MBR1100
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3
Figure 5. Typical Capacitance
20 400
VR, REVERSE VOLTAGE (VOLTS)
150
50
40
30
20
15
30
C, CAPACITANCE (pF)
50 10060
100
10 70 80 90
70
60
90
80
TJ = 25°C
fTEST = 1 MHz
NOTE 1 — MOUNTING DATA:
Data shown for thermal resistance junction-to-ambient
(RJA) for the mounting shown is to be used as a typical
guideline values for preliminary engineering or in case the
tie point temperature cannot be measured.
Typical Values for RJA in Still Air
Mountin
Lead Length, L (in)
u
Method 1/8 1/4 1/2 3/4 RJA
1 52 65 72 85 °C/W
2 67 80 87 100 °C/W
3 — 50 °C/W
Mounting Method 1
P.C. Board with
1-1/2 ″ x 1-1/2″
copper surface.
Mounting Method 3
P.C. Board with
1-1/2 ″ x 1-1/2″
copper surface.
BOARD GROUND
PLANE
VECTOR PIN MOUNTING
Mounting Method 2
LL
LL
L = 3/8″
NOTE 2 — THERMAL CIRCUIT MODEL:
(For heat conduction through the leads)
TA(A) TA(K)
TL(A) TC(A) TJTC(K) TL(K)
PD
RS(A) RL(A) RJ(A) RJ(K) RL(K) RS(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 heat sink.
Terms in the model signify:
TA = Ambient Temperature TC = Case Temperature
TL = Lead Temperature TJ = Junction Temperature
RS = Thermal Resistance, Heat Sink to Ambient
RL = Thermal Resistance, Lead to Heat Sink
RJ = Thermal Resistance, Junction to Case
PD = Power Dissipation
(Subscripts A and K refer to anode and cathode sides,
respectively.) Values for thermal resistance components are:
RL = 100°C/W/in typically and 120°C/W/in maximum.
RθJ = 36°C/W typically and 46°C/W maximum.
NOTE 3 — HIGH FREQUENCY OPERATION:
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 5)
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 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.