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MRF157 Datasheet, PDF (5/7 Pages) Motorola, Inc – MOS LINEAR RF POWER FET
D2 R10
R1
D.U.T
.
C3 R12 C7
R14
C13
L3
+
50 V
-
OUTPUT
22āpF
C9
L1
C14
T1
L2
L2
R15
-
BIAS 36-50 V
+
R4
10
12
11
13
D3
R2
R5
2 3 R6
4
7 65
D1
C1 R3
R8
C2
R9
C8
R11
T2
C4 R13
D.U.T.
C1 — 1000 pF Ceramic Disc Capacitor
C2, C3, C4 — 0.1 µF Ceramic Disc Capacitor
R7 C5 — 0.01 µF Ceramic Chip Capacitor
C6, C12 — 0.1 µF Ceramic Chip Capacitor
C7, C8 — Two 2200 pF Ceramic Chip Capacitors in Parallel
C7, C8 — Each
C9 — 820 pF Ceramic Chip Capacitor
C10, C11 — 1000 pF Ceramic Chip Capacitor
C13 — 0.47 µF Ceramic Chip Capacitor or Two Smaller
C13 —Values in Parallel
C14 — Unencapsulated Mica, 500 V. Two 1000 pF Units
C14 — in Series, Mounted Under T2
D1 — 1N5357A or Equivalent
D2, D3 — 1N4148 or Equivalent.
IC1 — MC1723 (723) Voltage Regulator
L1, L2 — 15 ηH, Connecting Wires to R14 and R15,
L1, L2 — 2.5 cm Each #20 AWG
C10
C11
C12
L3 — 10 µH, 10 Turns #12 AWG Enameled Wire on
L3 — Fair–Rite Products Corp. Ferrite Toroid #5961000401 or Equivalent
R1, R2 — 1.0K Single Turn Trimpots
R3 — 10K Single Turn Trimpot
R4 — 470 Ohms, 2.0 Watts
R5 — 10 Ohms
R6, R12, R13 — 2.0K Ohms
R7 — 10K Ohms
R8 — Exact Value Depends on Thermistor R9 used
R8 — (Typically 5.0–10K)
R9 — Thermistor, Keystone RL1009–5820–97–D1 or
R9 — Equivalent
R10, R11 — 100 Ohms, 1.0W Carbon
R14, R15 — EMC Technology Model 5308 or KDI
R14, R15 — Pyrofilm PPR 870–150–3 Power Resistors,
R14, R15 — 25 Ohms
T1, T2 — 9:1 and 1:9 Impedance Ratio RF Transformers
Unless otherwise noted, all resistors are 1/2 watt metal film type. All chip capacitors except C13 are ATC type 100/200B or Dielectric Laboratories type C17.
Figure 11. 2.0 to 50 MHz, 1.0 kW Wideband Amplifier
RF POWER MOSFET CONSIDERATIONS
MOSFET CAPACITANCES
The physical structure of a MOSFET results in capacitors
between the terminals. The metal oxide gate structure deter-
mines the capacitors from gate–to–drain (Cgd), and gate–to–
source (Cgs). The PN junction formed during the fabrication
of the TMOS® FET results in a junction capacitance from
drain–to–source (Cds).
These capacitances are characterized as input (Ciss), out-
put (Coss) and reverse transfer (Crss) capacitances on data
sheets. The relationships between the interterminal capaci-
tances and those given on data sheets are shown below. The
Ciss can be specified in two ways:
1. Drain shorted to source and positive voltage at the gate.
2. Positive voltage of the drain in respect to source and zero
volts at the gate. In the latter case the numbers are lower.
However, neither method represents the actual operat-
ing conditions in RF applications.
Cgd
GATE
Cgs
DRAIN
Cds
SOURCE
REV 1
5
Ciss = Cgd + Cgs
Coss = Cgd + Cds
Crss = Cgd
LINEARITY AND GAIN CHARACTERISTICS
In addition to the typical IMD and power gain data pres-
ented, Figure 5 may give the designer additional information
on the capabilities of this device. The graph represents the
small signal unity current gain frequency at a given drain cur-
rent level. This is equivalent to fT for bipolar transistors.
Since this test is performed at a fast sweep speed, heating of
the device does not occur. Thus, in normal use, the higher
temperatures may degrade these characteristics to some ex-
tent.
DRAIN CHARACTERISTICS
One figure of merit for a FET is its static resistance in the
full–on condition. This on–resistance, VDS(on), occurs in the
linear region of the output characteristic and is specified un-
der specific test conditions for gate–source voltage and drain
current. For MOSFETs, VDS(on) has a positive temperature
coefficient and constitutes an important design consideration
at high temperatures, because it contributes to the power
dissipation within the device.
GATE CHARACTERISTICS
The gate of the TMOS FET is a polysilicon material, and is
electrically isolated from the source by a layer of oxide. The
input resistance is very high — on the order of 109 ohms —
resulting in a leakage current of a few nanoamperes.
Gate control is achieved by applying a positive voltage
slightly in excess of the gate–to–source threshold voltage,
VGS(th).