Models AV-1010-B,
and AV-1015-B were
designed to function as general-purpose laboratory work horses, as production line test equipment, and as
state-of-the-art research lab equipment. These units provide peak output amplitudes of 50 or 100 Volts with rise
times of 10 ns. A few typical applications are described below in order to demonstrate that these instruments are
cost-effective, multi-purpose user-friendly units that belong in your instrument inventory. For faster rise time
applications (100 ps and 1 ns) see Applications Note No. 2A. Give Avtech a call at
1-800-265-6681 or e-mail at info@avtechpulse.com if you need help with your applications.
LASER DIODE DRIVERS
General guidelines for obtaining 1 Amp, 2 Amp, 4 Amp and 8 Amp pulses are given in the AV-1010-B and
AV-1015-B data sheets. For example, Model AV-1010-B
will provide up to 2 Amp pulses in the pulse width ranges of 50 ns to 10 ms,
and with the AVX-MRB6 accessory transformer will provide up to 8 Amps
with pulses as wide as 10 us. Model AV-1015-B will
provide 1 Amp pulses at pulse repetition frequencies as high as 10 MHz.
THE DELAY GENERATOR MODE
Models AV-1010-B
and AV-1015-B all
will operate in a delay generator mode as shown in Fig. 1. In this mode, the separation between the input TTL pulse
and the output pulse is controlled by the delay controls while the output pulse amplitude and pulse width are
controlled by the Amp and PW controls. The delays can be as low as 100 ns and as high as 10 ms.
Fig. 1
PULSE DRIVER-AMPLIFIER (PWOUT= PWIN)
The AV-1010-B
and AV-1015-B can
be triggered externally in the familiar mode where the output pulse width is controlled by the front-panel
pulse width controls. However, these units can also operate in a mode where the output pulse width is equal to the
input trigger pulse width, and only the output pulse amplitude is controlled by the front panel controls (or by an
externally applied 0 to 10 VDC control voltage). In effect the units can act as pulse driver-amplifiers with peak
outputs as high as 100 Volts. The TTL trigger pulse can be provided by your computer, a TTL IC, or by a low-power
waveform generator.
Fig. 2
PULSE DRIVER-AMPLIFIER (VOUT = K VDC)
The output pulse amplitude for Models AV-1010-B and
AV-1015-B can be controlled either by the front panel
controls (and by the IEEE 488 GPIB interface)
or by an externally applied 0 to +10V DC control voltage. This electronic
control function (EA) will function either when the unit is triggered internally or externally (including the PWOUT
= PWIN mode described in the preceding section). The input impedance to the EA port is greater than 10 kilohms, so
the VDC control signal can be provided by your computer or by an ADC or from a power supply.
Fig. 3
THE DOUBLE PULSE MODE
Models AV-1010-B
and AV-1015-B all
will operate in a double-pulse mode as shown in Fig. 4. In this mode, the separation between the two pulses is
controlled by the delay controls (which control the separation between the SYNC pulse and main output pulse in the
single pulse mode). This is a convenient feature for varied applications such as testing the performance of radar
receivers, high-speed gating circuits, and mode locking applications.
Fig. 3
DC OFFSET
Many applications require a fast pulse to be superimposed on a DC level as shown in Fig. 5. Avtech's Model
AVX-TD bias insertion unit (see page 98) may be used to add a DC offset to the
output of Models AV-1010-B
and AV-1015-B.
DC offsets as high as ±50 Volts may be employed with pulse widths as high as 100 us. The AV-1010-B is also available with a built-in offset function (the
-OT option).
Fig. 4
TRANSISTOR SWITCHING TIME TESTS
Model AV-1010-B
can provide pulsed output currents as high as 2 Amperes with output
impedances as low as 2 Ohms, or output currents as high as 1 Amperes with an output impedance of 50 Ohms. With such
high output capability (and 10 ns rise & fall times) this model is well suited for tests such as pulsing the
collector (or drain) of medium power bipolar and mosfet transistors as shown in Fig. 6, or pulsing the base (or
gate) of very high power bipolar (or mosfet) transistors as shown in Fig. 7. The low output impedance feature (as
low as 2 Ohms) allows the unit to serve as a pulsed power supply for collector or drain biasing, and to provide
switching times far less than 50 Ohms sources when used to pulse the base or gate of a power transistor. Avtech's
line of bias insertion units (models AVX-TC and AVX-TD) may be used to add a DC offset to the pulse, if required. For testing applications
requiring drive switching times of less than 1 ns, see the model AVR-D2-C, which is specifically designed to perform MIL-S-19500 tests.
Fig. 6 | Fig. 7 |
TRR AND TL TESTS FOR HIGH-SPEED RECTIFIER DIODES
The characteristic current waveform for a diode TRR (and TL) test is shown in Fig. 8,
along with a definition of IF, IR, IRR, and TL. Fig. 9 illustrates a
test circuit commonly specified for testing of medium and high current fast-recovery diodes. The specification
often calls for a pulse generator source impedance of 10 Ohms. Avtech Model AV-1010-B will
satisfy the requirement if operated in the 100 Volt range and approximately 8 Ohms is placed in series with the
output. The pulser will provide an IR as high as 2 Amperes. Model AV-1015-B can also be used for applications requiring IR as high as 1 Amp.
For diode switching tests requiring rise and fall times of less than 1 ns, see our AVR-EB series, which was specifically designed to perform many tests specified in
MIL-STD-750C. For microwave diode TT and TL tests refer to Application
Note 2A.
Figs. 8 and 9
PULSE TRANSFORMER TESTING (ET CONSTANT AND PRIMARY INDUCTANCE)
Pulse generators such as the AV-1010-B and AV-1015-B along with an oscilloscope and current and voltage probes may be used to determine the ET constant of a pulse transformer using the arrangement shown in Fig. 10. The pulse width is increased until such time as the magnetizing current increases by 50% relative to the straight-line extension. The product of the applied pulse width (in ms) and amplitude (in Volts) gives the ET constant. This arrangement may also be used to determine the primary inductance. The pulse generator should be set in the low output impedance mode (ZOUT ≤ 2 Ohms) and the slope of linear portion of the magnetizing current time plot may then be used to compute the inductance as follows:
LP = EIN T1 / E1, approximately
Fig. 10
PULSE-MODE TESTING OF GUNN DIODES
The AV-1010-B
should be considered for Gunn diode pulsing, with pulse widths as low as 50
ns or as wide as 10 ms. These pulsers can source up to 2.0 Amps and feature a source impedance of less than 2 Ohms
(when the amplitude range switch is in the 100 V range).
MISMATCHED LOADS, HIGH DUTY CYCLE OPERATION
The versatile AV-1010-B was specifically designed to drive loads in the range of 50 Ohms to open
circuits. If the load impedance is less than 50 Ohms and the output current exceeds 120% of the rated maximum, the
output stage is automatically turned off (to protect the unit). If the load impedance is 50 Ohms but the average
output power exceeds the rated maximum (because the rated duty cycle is exceeded), the unit also shuts down. When
the units are driving high impedance loads, the units may be operated at duty cycles at least as high as 80%. The
source impedance may be set at 2 Ohms or 50 Ohms and this feature may be used to eliminate ringing when driving
high impedance loads (without loss of peak amplitude). When 50 Ohm back matching is employed with a 50 Ohm load,
the peak output voltage amplitude is reduced by one half (bottom trace Fig. 11B).
Fig. 11A. RS = 2 Ohm RL = 100 kilohms 24" cable |
Fig. 11B RS = 50 Ohm RL = 100 kilohm (top) RL = 50 Ohm (bottom) |