U.S. patent number 3,612,899 [Application Number 05/065,551] was granted by the patent office on 1971-10-12 for generator for short-duration high-frequency pulse signals.
This patent grant is currently assigned to Sperry Rand Corporation. Invention is credited to Joseph D. De Lorenzo, Gerald F. Ross.
United States Patent |
3,612,899 |
Ross , et al. |
October 12, 1971 |
GENERATOR FOR SHORT-DURATION HIGH-FREQUENCY PULSE SIGNALS
Abstract
Very narrow pulses of high-frequency sine wave electromagnetic
energy are formed by use of a gated or pulse modulated
continuous-wave source feeding a transmission line network having a
time-limited impulse response and adjusted to provide a series
resonance with the leakage capacity of the source gating or
modulating switch for the purpose of assuring that a maximum of the
available energy is employed to form the output and that the output
level is nulled before and after the generation of the
high-frequency pulse.
Inventors: |
Ross; Gerald F. (Lexington,
MA), De Lorenzo; Joseph D. (Sudbury, MA) |
Assignee: |
Sperry Rand Corporation
(N/A)
|
Family
ID: |
22063502 |
Appl.
No.: |
05/065,551 |
Filed: |
August 20, 1970 |
Current U.S.
Class: |
307/96;
333/20 |
Current CPC
Class: |
H03K
3/80 (20130101) |
Current International
Class: |
H03K
3/80 (20060101); H03K 3/00 (20060101); H03k
003/64 () |
Field of
Search: |
;307/106,107,108,261
;328/59,60,61,65,63,66,67 ;333/20 |
References Cited
[Referenced By]
U.S. Patent Documents
Primary Examiner: Hohauser; Herman J.
Claims
While the invention has been described in its preferred embodiment,
it is to be understood that the words which have been used are
words of description rather than of limitation, and that changes
within the purview of the appended claims may be made without
departing from the true scope and spirit of the invention in its
broader aspects.
1. Apparatus for generation of short duration high-frequency
time-limited pulses having abrupt initial rise and terminal fall
characteristics comprising:
first high-frequency transmission line means having a predetermined
characteristic impedance Z.sub.o and input and output means,
high-frequency sine wave oscillator means for supplying a train of
high-frequency sine wave cycles at said input means,
switch means having, when nonconducting, a leakage capacity
C.sub.s, for gating said oscillator means,
matched utilization means attached at said output means,
open-circuited branch transmission line means joined to said first
transmission line means at a distance d.sub.m therealong from said
input means,
said distance d.sub.m so adjusted as substantially to provoke
resonance between said input means and the leakage capacitance
C.sub.s of said switch.
2. Apparatus as described in claim 1 wherein said distance d.sub.m
is adjusted so as to make the reactance of said first transmission
line means substantially equal to the reactance of said switch
means at resonance.
3. Apparatus as described in claim 1 wherein said distance d.sub.m
is adjusted so as to make the driving point impedance of the
network comprising said first transmission line means and said
branch transmission line means substantially equal to the reactance
of said switch means at resonance.
4. Apparatus as described in claim 1 wherein the quantity d.sub.m
is defined substantially by the equation
where:
.beta.=2.pi.f.sub.o /c
and where f.sub.o is the operating frequency of said oscillator
means and c is the velocity of wave propagation is said first
transmission line means.
5. Apparatus as described in claim 1 wherein said open-circuited
branch transmission line means joined to said first transmission
line means comprises radially extending coaxial transmission line
means open-circuited at ends remote from said first transmission
line means.
6. Apparatus as described in claim 5 wherein said open-circuited
ends of said radially extending coaxial transmission line means
remote from said first transmission line are joined one to the
other in direct conductive relation.
Description
BACKGROUND OF THE INVENTION
1. Field of the Invention
The invention pertains to means for producing pulses of
high-frequency or microwave sine wave electromagnetic signals of
duration of the order of one nanosecond and more particularly to
apparatus for producing such pulse signals having abrupt initial
rise and terminal fall characteristics with substantially no energy
emission before or following the pulse.
2. Description of the Prior Art
The literature describes several prior art attempts to devise
systems for generation of very short pulses of high-frequency or
microwave signals. Generally, one method has involved synthetic
generation of such pulse signals by the excitation of a
pulse-forming network with an abrupt step function voltage. Various
networks have been used to transform the incident step wave to a
rectangular impulse.
As use of increasingly higher carrier frequencies is made,
especially at C-band and above, the output pulse waveform for such
prior systems degrades with increasing severity. The degeneration
is traced to the increasing production of higher order mode
propagation at network junctions and to increasing losses and
accompanying dispersion in the network transmission lines. A
further barrier to successful extension of the technique is the
generally inversely proportional relation between microwave
generator output signal level and increasing frequency.
Systems for generating pulse outputs not requiring carrier phase
synchronization with respect to the pulse envelope have also been
realized. For example, a switch in series with a continuous wave
oscillator may simply be rapidly opened and rapidly closed to
produce the desired short duration impulse signal. However, the
leakage capacities of available switches are finite and severely
limit the off-on ratio of the output pulses. In addition, equally
abrupt initial rise times and terminal fall times are desired for
the pulse waveform and switches generally available at reasonable
cost do not open and close at the same rates and therefore from
undesirably asymmetric output pulses.
SUMMARY OF THE INVENTION
The present invention is an apparatus for generating
pulse-modulated, high-frequency carrier signals having pulse
durations of the order of a nanosecond and having sharply
rectangular envelopes. The invention preferably employs excitation
of TEM-mode electromagnetic wave propagation in a novel
pulse-forming network having time-limited response characteristics
in response to a gated pulse or step modulated high-frequency input
wave.
BRIEF DESCRIPTION OF THE DRAWINGS
FIG. 1 is a schematic circuit representation of one form of the
invention.
FIG. 2 is an explanatory graph used in understanding FIG. 1.
FIGS. 3, 4, and 5 are graphs showing output waveforms generated by
variously adjusting the circuit of FIG. 1.
FIGS. 6 and 7 are equivalent circuits used in explaining the
operation of the circuit of FIG. 1.
FIG. 8 is, like FIG. 1, a schematic circuit representation of one
form of the invention.
FIG. 9 is a partially schematic top view of one preferred form of
the invention.
FIG. 10 is a partially sectioned top view of a presently preferred
form of the invention.
DESCRIPTION OF THE PREFERRED EMBODIMENTS OF THE INVENTION
The invention is a high-frequency transmission line circuit for
generating impulse modulated signals having an impulse envelope
duration of the order of a nanosecond. The generator employs a
pulse forming network having a time-limited response driven by a
source of step modulated high-frequency energy. Passive properties
inherent in the network may be employed to cause sharp terminal
fall of the impulse for production of a sharply rectangular pulse
envelope. In order better to understand the novel signal generator,
consider first the network of FIG. 1. A lossless two-wire
transmission line 3, 31 having a surge or characteristic impedance
Z.sub.0, extends a distance D between impedance reference planes 4
and 5. At the midplane 6 of the first or main transmission line 3,
3a is conductively attached to a two-wire stub lossless
transmission line 7, 7a which extends a distance L from line 3, 3a
and which is open-circuited at its outer terminal ends 8, 8a. Stub
transmission line 7, 7a has a surge impedance Z.sub.a and forms a
pulse-forming network 10 in cooperation with the main transmission
line 3, 3a. Various known types of low loss, nondispersive
transmission lines may be used to form lines 3, 3a and 7, 7a,
including transmission lines that propagate traveling
high-frequency or microwave signals in nondispersive modes, such as
in the TEM mode. The normalized surge or characteristic impedance
Z.sub.0 of transmission line 3, 3a may be 1 ohm, while that of line
7, 7a must have a characteristic impedance one-half that of line 3,
or 0.5 ohms.
Networks 10 may be excited at its input terminals in plane 4 by an
impulse or repetitive train of impulses furnished at said input by
a known type of impulse generator 11 having an internal resistance
indicated by resistor 12 of R.sub.g ohms. A normalized value of 1
ohm may be chosen for the parameter R.sub.g. An impulse supplied by
generator 11 travels through pulse-forming network 10 to a
resistive or terminating load 15 which may be a radiating antenna
or other matched utilization device. Load 15 has a resistance
R.sub.L which may also have a normalized value of 1 ohm.
It has been shown that when the network 10 is excited by such an
impulsive signal, the output response a(t) of network 10 across a
load resistor or termination 10 having a 1 ohm value is two
impulses 20 and 21 of the same sign and area, as illustrated in
FIG. 2. Impulse 20 is located in time D/c seconds after the time
the input impulse reaches plane 4, the symbol c representing the
propagation velocity of energy along transmission line 3, 3a.
Impulse 20 and 21 are separated by a time interval T=2L/c seconds.
Such properties of the network 10 are discussed by G. F. Ross in
the paper "A New Microwave Phase Equalizer Network," found in pages
647 to 650 of the Nov. 1967 issue of the I.E.E.E. Transactions on
Microwave Theory and Techniques.
Under the above impulse excitation conditions, network 10 can be
spoken of as having a time-limited impulse response, the value a(t)
being zero for all times t>D+T=D+(2L/c). The significance of
such a type of time-limited response becomes evident upon
examination of the output of pulse-forming network 10 for a
step-modulated excitation having a nominal carrier frequency f
centered at f.sub.o, where f.sub.o may take values such as
and where k is an integer. As shown in FIGS. 3, 4, and 5, the
output of network 10 for t>T seconds is identically zero,
regardless of the starting phase of the sinusoidal input
impulse.
FIG. 3, for example, represents the situation for a signal of
nominal center frequency f.sub.o =1/2T, wherein an output pulse is
formed of duration T. The time period following the end of interval
T represents a forbidden era in which the input wave cannot
contribute energy to an output signal. FIG. 4, like FIG. 3,
represents a pattern in which the exciting pulse starts with zero
phase, but the value of f.sub.o is now 9/2T. The same forbidden
region is represented by dotted line waveforms. FIG. 5 is similar,
but with f.sub.o =3/2T and a starting phase other than zero and
therefore represents a more general case. Again, the time period
following the end of time interval T represents a forbidden era and
there is no output signal.
When the value of k in the quantity (2k-1) 2T is not an integer,
the step modulated response of network 10 for t>T is no longer
zero and the output signal is no longer an impulse. On the other
hand, for any integral value of k, an impulse output waveform of
desired envelope shape appears across termination 15. Where k is an
integer much greater than unity, there will be many high-frequency
cycles present within the envelopes of the output impulse signal.
The larger the value of k, the more closely spaced are the
permitted output frequencies; e.g., for a given pulse duration
T=2L/c seconds and k>>1, there is a number of discrete
frequencies at which the equality f.sub.o T=(2k-1)/2 can be
substantially satisfied.
The foregoing discussion of the operation of pulse-forming network
10 has been somewhat idealized in the sense that certain practical
considerations have been neglected. Most important, particularly
for frequencies above those lying in the X-band, the leakage
capacity of the gating switch within generator 11 which controls
the start and stop of the pulse emanating form signal source 11 has
been neglected. According to the present invention, the effects of
switch leakage are recognized and are beneficially used.
Reference may be had to FIG. 6 for analysis of the effects of
leakage of the modulating switch 22. In FIG. 6, pulse forming
network 10 is connected to the sine wave generator 11a when switch
22 is open through the generator's source resistance 12 and the
leakage capacity of switch 22, which capacitance may be represented
by a capacitor 23 of value C.sub.s. The output voltage a(t) from
network 10 appearing across matched termination 15 is zero
regardless of the values of C.sub.s and V.sub.s because of the
effective short circuit imposed by stub transmission line 3, 3a at
f=f.sub.o. However, the magnitude and carrier phase of the output
pulse depends critically on the steady state voltage V.sub.s across
leakage capacitor 23 at the time at which switch 22 is to be
closed.
The above-mentioned relations may better be understood by reference
to FIG. 7. Upon closure of switch 22, the effective resistance
r.sub.s of the switch drops suddenly to zero, so the voltage across
condenser 23 must drop to zero (the voltage between points A and B
drops to zero). Such is equivalent to the abrupt insertion of a
generator source 24 of equal potential V.sub.s ' and opposite sign
in series with voltage V.sub.s.
As noted previously, the steady state output appearing across
termination 15 is zero regardless of the value of V.sub.s. Thus,
the response due to voltage E.sub.g in series with voltage V.sub.s
is zero. On the other hand, the output response instantly after
t=D/c must be due directly to the fact that V.sub.s '=V.sub.s.
Thus, to maximize the pulse output voltage, the value of V.sub.s
must be maximized, since it indeed determines the amplitude of
output signal a(t).
A maximum value for factor V.sub.s may be achieved by making use of
a series resonance effect, for example, when the steady state
driving point impedance Z.sub.dp (FIG. 7) of pulse-forming network
10 is inductive and the following relationship is satisfied at
frequency f=f.sub.o :
Z.sub.dp = X.sub.L = X.sub.s (1) In equation (1), Z.sub.dp is
defined as the steady state sinusoidal driving point impedance as
measured at the input port of the pulse forming network at any
frequency f. The quantity X.sub.c is the capacitive reactance of
the switch in its normally open mode at frequency f=f.sub.o. Third,
X.sub.L is the inductive reactance presented at the input port of
the pulse forming network when f=f.sub.o. The quantity Z.sub.dp is
purely inductive and equal to X.sub.L only at f=f.sub.o. It is seen
that the desired relationship between the respective line and
switch reactances X.sub.L and X.sub.s and the factor Z.sub.dp is
met by proper selection of the value of distance d (FIG. 1) between
reference plane 4 and plane 6 where stub branch line 7, 7a forms
its junction with line 3, 3a. This results in resonance between the
network input and the leakage capacity C.sub.s of the switch 22 and
results because the stub branch line 7, 7a junction represents an
effective short circuit.
Under the above circumstances, the value of the steady state
driving point impedance Z.sub.dp for network 10 is:
Z.sub.dp =jZ.sub.o tan .beta.d (2)
where:
.beta.=2.pi.f.sub.o /c
The required maximizing value d.sub.m of distance d is found from
equations (1) and (2) as follows:
or:
If we define Q as:
Then:
d.sub.m =(1/.beta.) tan.sup..sup.-1 Q (3)
Here, the factor Q is the conventional quality factor of the
resonating circuit. Under the above conditions, the voltage V.sub.s
is given by:
V.sub.s =- jQE.sub.g (4)
By inspection of FIGS. 1 and 2, it is seen that the peak output
during the era of the output pulse across termination 15 is:
a(t).sub.peak = V.sub.s /4 (5)
In general, the signal a(t).sub. peak closely resembles the pulse
wave shown in FIG. 5.
It is seen from the analysis of FIGS. 1 to 7 that the invention may
be practiced in any of several ways. For example, the
unsynchronized step modulated sine wave generator 11 of FIG. 1 may
be any convenient relatively stable high-frequency oscillator, and
it may internally include a series connected controlling or gating
switch 22 which may be either a single-pole, single throw
mercury-wetted mechanical switch or a voltage controlled
semiconductor switch of conventional nature. Switches suitable for
such applications are illustrated, for example, in the pending G.
F. Ross Pat. application Ser. No. 843,945, entitled "High Frequency
Switch" and filed July 23, 1969, now U.S. Pat. No. 3,569,877,
issued Mar. 9, 1971, as well as in the H. C. Maguire Pat.
application Ser. No. 852,656, entitled "Coaxial Line Reed Switch
for Fast Rise Signal Generator With Attenuation Means Forming Outer
Section of the Line" and filed Aug. 25, 1969, now Pat. No.
3,564,277, issued Feb. 16, 1971, both inventions being assigned to
the Sperry Rand Corporation.
FIG. 8 represents schematically the form of a two-wire transmission
line system in a practical instrumentation of the invention and is
further to be discussed in connection with the apparatus of FIG. 9
which is illustrated in the form of a coaxial transmission line
system. FIG. 8 is significantly similar to part of FIG. 1, and
corresponding parts are identified by similar reference numerals.
For example, two-wire transmission line 3, 3a extends between
impedance reference planes 4 and 5 and has branching from it a
two-wire open-circuited transmission line 7, 7a of length L whose
junction with line 3, 3a is located in reference plane 6 a distance
d from plane 4, as previously defined. The value d is again
adjusted substantially to the m d.sub.m called for by equation (3).
The pulse forming network 10a of FIG. 8 now includes a second
branching two-wire open circuited transmission line 17, 17a, also
of length L and whose junction with line 3, 3a is located also in
reference plane 6 coincident with the junction of branch line 7, 7a
and at reference plane 6 a distance d.sub.m from reference plane 4.
For one practical application, lines 3, 3a and branch lines 7, 7a
and 17, 17a may all have characteristic impedances of 50 ohms. It
is seen that network 10a, with a factor d.sub.m of proper value,
will operate substantially in the same manner as will the
arrangement of FIG. 1 when connected to impulse generator 11 and
termination 15 of FIG. 1.
One practical embodiment of the invention is shown in FIG. 9 as
having an internally impulse modulated generator 111 similar to
generator 11 of FIG. 1 and coupled at a reference plane 104 to a
coaxial transmission line network 110a whose output impulse wave
a(t) is coupled at reference plane 105 to matched termination 115.
For convenience, parts of network 110a corresponding to parts of
network 10a of FIG. 8 have similar reference numerals with the
factor of 100 added to them.
In FIG. 9, the network 110a is conveniently formed of readily
available coaxial transmission line components to form a
cross-shaped configuration. It includes a main coaxial transmission
line 103, 103a whose center conductor 103 is connected to generator
111 and to terminal load 115. The opposite lead of generator 111
and of load 115 are grounded, as is the outer conductor 103a of
line 103, 103a. The network is formed with radially or oppositely
branching coaxial lines 107, 107a and 117, 117a. The latter are
shown cut away at junction 125 lying in plane 106 to emphasize the
joint connection at point 125 of inner conductors 107 and 117 to
inner conductor 103 of the main transmission line 103, 103a. Outer
coaxial conductors 107a and 117a, being electrically connected to
outer conductor 103a as indicated by dotted lines, are also at
ground potential. Again, the distance between planes 104 and 106,
which planes correspond to reference planes 4 and 6, is adjusted
substantially to the value d.sub.m defined above.
FIG. 10 represents a modification 110b of the network 110a of FIG.
9 having additional features desirable in certain applications. The
structure is electrically equivalent to that of FIG. 9, but
radially extending coaxial lines 107, 107a and 117, 117a, which may
be in the from of flexible coaxial cables, are bent into a
generally circular loop. Then, the respective open-circuited ends
123 and 123a of lines 107, 107a and 117, 117a are directly joined
in conductive relation, as in the plane 126 of FIG. 10. It is
understood that part of the loop lies above the plane of the
drawing of FIG. 10.
Operation of FIGS. 9 and 10 is similar, since all signals again
travel the same distances in both embodiments. Those signals which
return to junction 125 in FIG. 9 from the stub lines along the same
paths as they originally left it, return thereto in FIG. 10 along
the opposite branch transmission line. In the apparatus of FIGS. 9
and 10, all transmission line elements may conveniently be
commercially standard 50-ohm components. An additional advantage of
the FIG. 10 structure is that the output pulse duration is
dependent upon the length of a single continuous cable loop.
FUrther, no leadage of energy can occur because of an imperfect
open circuit 123 or 123a and counterflowing signals must travel
over equal paths.
* * * * *