Search Images Maps Play YouTube News Gmail Drive More »
Sign in
Screen reader users: click this link for accessible mode. Accessible mode has the same essential features but works better with your reader.

Patents

  1. Advanced Patent Search
Publication numberUS3124678 A
Publication typeGrant
Publication dateMar 10, 1964
Filing dateMay 28, 1959
Publication numberUS 3124678 A, US 3124678A, US-A-3124678, US3124678 A, US3124678A
InventorsMartin Masonson
Export CitationBiBTeX, EndNote, RefMan
External Links: USPTO, USPTO Assignment, Espacenet
Agent
US 3124678 A
Abstract  available in
Images(1)
Previous page
Next page
Claims  available in
Description  (OCR text may contain errors)

March 10, 1964 M. MASONSON 3,

GAUSSIAN WAVEFORM GENERATOR Filed May 28, 1959 Le -I (U a T v l *1 m w l i INVENTOR. I u MART/IV MASONSOA/ 7 T WNW A GEN T United States Patent 3,124,678 GAUSSIAN WAVEFORM GENERATOR Martin Masonson, Nutley, N.J., assignor to International Telephone and Telegraph Corporation, Nutley, N.J., a corporation of Maryland Filed May 28, 1959, Ser. No. 816,583 2 Claims. (Ci. 235-197) This invention relates to waveform generators and more particularly to a waveform generator for producing Gaussian-shaped waveshape.

In certain types of pulse transmitters it is desirable to utilize a minimum spectrum of minimum rise time for the radiated signal oonsistant with the transmission of the desired information. Examples of systems utilizing minimum spectrum are pulse code modulation systems, radar and loran transmitters, certain types of aerial navigation systems, certain types of frequency shift keying systems, and certain types of facsimile links. It is desirable in most of these systems to have a minimum pulse rise time with minimum output signal bandwidth. pulse shape having minimum bandwidth for the minimum pulse rise time is that shape defined by the Gaussian distribution. Heretofore the prior art schemes for producing Guassian waveforms have generally related to the use of filters to act on square wave or similar type pulse to produce an output therefrom having a shape defined substantially by the Guassian distribution. These prior art schemes have certain disadvantages. One disadvantage is that to obtain a reasonable approximation of the Gaussian error curve many filter sections are required, and the resulting pulse is only approximately of Gaussian shape. Also, the use of filters cause a time delay.

One object of the present invention is to provide an improved waveform generator to produce a waveform more substantially of Gaussian shape then heretofore obtainable.

Another object of the present invention is to provide a Waveform generator employing simple circuitry for producing a substantially Gaussian shaped waveform.

Still another object of the present invention is to provide a waveform generator for producing Gaussian pulses from a source of sawtooth voltage.

A feature of the present invention is a Gaussian waveform generator comprising means to produce a sawtooth waveform signal, and means coupled to the waveform signal producing means to modify the sawtooth waveform signal to produce a Gaussian waveform output signal.

Another feature of the present invention is a Gaussian waveform generator of the type described where the modifying means includes at least a multiplier and an integrator.

Still another feature of the present invention is a Gaussian waveform generator of the type described including a feedback path coupled between the output of the integrator and the multiplier.

The above mentioned and other features and objects of this invention will become more apparent by reference to the following description taken in conjunction with the accompanying drawings, in which:

FIG. 1 is a schematic diagram of an embodiment for producing a Gaussian shaped Waveform in accordance with the principles of this invention;

FIG. 2 is a series of waveforms useful in explaining the operation of the embodiment of FIG. 1.

It is known that a Gaussian pulse may be represented by the expression 1 (t-T) e where 0' is defined as the standard deviation, t is defined as time, e is the base of the natural logarithm, T is the time at which it is desired to peak the Gaussian pulse, and g(t) is the general symbol for a quantity as a function of time. A Gaussian distribution of current (i) may then be expressed as m) =Ke (2) where K is a constant equal to It is to be noted that i (t) still represents the expression for a Gaussian current pulse and represents a linear variation of current with time. Therefore, it can be said from an examination of Equation 4 that a Gaussian pulse may be produced by multiplying a linear variation of current with time, such as a sawtooth signal, with a Gaussian variation of current with time and integrating the product of the two currents.

Referring to FIG. 1, a Gaussian waveform generator is shown comprising means 1 to produce a sawtooth waveform signal, and means 2 coupled to signal producing means 1 to modify the sawtooth waveform signal therefrom to produce a Gaussian waveform output signal.

A sawtooth waveform generator 1, which for purposes of illustration is shown as a phantastron circuit, produces a sawtooth output signal as illustrated by curve A, FIG. 2. The sawtooth signal has a period of 2T and a slope of so that the expression for the linear relationship is the desired term Briefly, the operation of the Gaussian waveform generator is as follows. The output signal from sawtooth wave-form generator 1 is coupled to multiplier 3. The output of multiplier 3 is coupled to integrator 4 to provide the desired Gaussian shaped pulse. The output of integrator 4 is fed back to multiplier 3 along feedback means 5 for multiplication with the sawtooth waveform to sustain the Gaussian output of integrator 4.

A more detailed explanation can be obtained by considering the initial cycle of the sawtooth signal. At time zero, the expression for a Gaussian pulse defined by Equation 2 becomes This value of current is extremely small in comparison with the peak value of the Gaussian pulse, and may be initially produced by means of a small charge on capacitor 4a. This initial current which is present at time ero is applied to multiplier 3 along feedback means 5 and is multiplied by the initial value of the sawtooth wave from generator 1. The product of this multiplication of initial sawtooth signal with initial Gaussian signal is then integrated by integrator 4 which results in an output signal which is the integral of the product of a linear signal with a Gaussian signal, and therefore Gaussian in form. The Gaussian output signal from integrator 4 is also fed back along feedback path 5 to be multiplied with the increasing value of sawtooth signal as time (t) increases.

'As the sawtooth signal from generator 1 increases it is continually being multiplied with the Gaussian signal from feedback path 5 to produce a signal from multiplier 3 which when integrated, becomes a Gaussian shaped pulse. When time equals T, the sawtooth signal illustrated by curve A, FIG. 2 passes through a zero value and the Gaussian output pulse from integrator 4 reaches a peak value. As time continues to increase the sawtooth signal continues to rise in value and the Gaussian output pulse decreases in valueuntil time equals 2T, at which time the sawtooth signal will recycle and the Gaussian output pulse has decreased to the initial value expressed by Equation 6. The operation of the circuit of FIG. 1 for continued cycles of sawtooth signal is the same as has been described hereinabove. Relating the embodiment of FIG. 1 with the desired Gaussian Equation 4, it is seen that feedback means 5 is a source of Gaussian signal i(t) and sawtooth generator 1 is a source of linear signal Multiplier 3 produces the product signal and integrator 4 performs the necessary integration of the product signal to produce an output signal substantially equal to fli'l ll 0 pulse width or deviation 0' is determined by the slope of the sawtooth waveform from source 1 and the peak of the pulse occurs at the zero crossing of the sawtooth signal. If it is desired to peak the Gaussian wave at T, the sawtooth generator 1 should recycle in accordance with a time 2T.

While I have described above the principles of my invention in connection with specific apparatus, it is to be clearly understood that this description is made only by way of example and not as a limitation to the scope of my invention as set forth in the objects thereof and in the accompanying claims.

I claim:

1. A Gaussian waveform generator comprising:

a sawtooth generator;

a multiplier having one of its inputs coupled to the output of said generator;

a single integrator coupled to the output of said multiplier; and

substantially linear means coupling the output of said integrator to the input of said multiplier.

2. A Gaussian waveform generator comprising:

means to produce a sawtooth waveform signal;

means, including a multiplier to one input of which said sawtooth signal is applied, responsive to said sawtooth signal and to a Gaussian pulse for producing a waveform that is the derivative of a Gaussian pulse;

a single integrator responsive to said derivative to produce a Gaussian output pulse; and

a substantially linear feedback path coupled between the output of said single integrator and the input of said multiplier means.

References Cited in the file of this patent UNITED STATES PATENTS 2,230,926 Biugley Feb. 4, 1941 2,872,109 Smith Feb. 3, 1959 2,878,383 Yando Mar. 17, 1959 OTHER REFERENCES

Patent Citations
Cited PatentFiling datePublication dateApplicantTitle
US2230926 *Apr 13, 1939Feb 4, 1941Philco Radio & Television CorpTiming signal circuits
US2872109 *Oct 29, 1953Feb 3, 1959Smith Jr Blanchard DMultiplier-integrator circuit
US2878383 *Aug 9, 1956Mar 17, 1959Sylvania Electric ProdControl signal generator
Referenced by
Citing PatentFiling datePublication dateApplicantTitle
US3870872 *Feb 1, 1974Mar 11, 1975Abbott LabProbability analog function computer
US3937945 *Jun 25, 1974Feb 10, 1976The United States Of America As Represented By The United States National Aeronautics And Space Administration Office Of General Counsel-Code GpApparatus for simulating optical transmission links
US4207772 *Jul 11, 1977Jun 17, 1980Mediscan, Inc.Electronic drive system and technique for ultrasonic transducer
Classifications
U.S. Classification708/845, 327/100, 327/355
International ClassificationH04L25/03, H03K5/01
Cooperative ClassificationH03K5/01, H04L25/03834
European ClassificationH03K5/01, H04L25/03E1