High frequency realization of non-autonomous nonlinear transistor circuit

In this paper, an electronic implementation of a non-autonomous nonlinear transistor circuit is presented. This nonlinear circuit topology requires a minimal number of components, which consists of two resistors, two capacitors, and a single NPN bipolar junction transistor (BJT). This topology is of...

Full description

Bibliographic Details
Main Authors: Benjamin K. Rhea, Edmon Perkins, Robert N. Dean
Format: Article
Language:English
Published: AIP Publishing LLC 2019-06-01
Series:AIP Advances
Online Access:http://dx.doi.org/10.1063/1.5100948
id doaj-64dc67e9547e46aeb3e36409e767714c
record_format Article
spelling doaj-64dc67e9547e46aeb3e36409e767714c2020-11-25T00:59:50ZengAIP Publishing LLCAIP Advances2158-32262019-06-0196065112065112-810.1063/1.5100948052906ADVHigh frequency realization of non-autonomous nonlinear transistor circuitBenjamin K. Rhea0Edmon Perkins1Robert N. Dean2Electrical and Computer Engineering, Auburn University, Auburn, Alabama 36849, USAMechanical Engineering, Auburn University, Auburn, Alabama 36849, USAElectrical and Computer Engineering, Auburn University, Auburn, Alabama 36849, USAIn this paper, an electronic implementation of a non-autonomous nonlinear transistor circuit is presented. This nonlinear circuit topology requires a minimal number of components, which consists of two resistors, two capacitors, and a single NPN bipolar junction transistor (BJT). This topology is of interest because it is relatively simple to construct and could be used for potential applications such as random number generators (RNGs) or noise signal generators (NSGs). The transistor portion of the circuit was analyzed using the Ebers-Moll model for a BJT. Using this model, time domain and phase space plots that qualitatively match the original systems dynamics were created. This model was also used to create bifurcation diagrams of the base voltage versus both frequency and amplitude, where periodic and chaotic solutions exist. The hardware realization was built using commercial-off-the-shelf (COTS) components with two different printed circuit board (PCB) designs. This PCB included the forcing function on the board with the transistor circuit. This circuit topology functioned over a wide range of frequencies, with an upper limit of approximately 5.1 MHz. Many potential applications could benefit from this high operation frequency.http://dx.doi.org/10.1063/1.5100948
collection DOAJ
language English
format Article
sources DOAJ
author Benjamin K. Rhea
Edmon Perkins
Robert N. Dean
spellingShingle Benjamin K. Rhea
Edmon Perkins
Robert N. Dean
High frequency realization of non-autonomous nonlinear transistor circuit
AIP Advances
author_facet Benjamin K. Rhea
Edmon Perkins
Robert N. Dean
author_sort Benjamin K. Rhea
title High frequency realization of non-autonomous nonlinear transistor circuit
title_short High frequency realization of non-autonomous nonlinear transistor circuit
title_full High frequency realization of non-autonomous nonlinear transistor circuit
title_fullStr High frequency realization of non-autonomous nonlinear transistor circuit
title_full_unstemmed High frequency realization of non-autonomous nonlinear transistor circuit
title_sort high frequency realization of non-autonomous nonlinear transistor circuit
publisher AIP Publishing LLC
series AIP Advances
issn 2158-3226
publishDate 2019-06-01
description In this paper, an electronic implementation of a non-autonomous nonlinear transistor circuit is presented. This nonlinear circuit topology requires a minimal number of components, which consists of two resistors, two capacitors, and a single NPN bipolar junction transistor (BJT). This topology is of interest because it is relatively simple to construct and could be used for potential applications such as random number generators (RNGs) or noise signal generators (NSGs). The transistor portion of the circuit was analyzed using the Ebers-Moll model for a BJT. Using this model, time domain and phase space plots that qualitatively match the original systems dynamics were created. This model was also used to create bifurcation diagrams of the base voltage versus both frequency and amplitude, where periodic and chaotic solutions exist. The hardware realization was built using commercial-off-the-shelf (COTS) components with two different printed circuit board (PCB) designs. This PCB included the forcing function on the board with the transistor circuit. This circuit topology functioned over a wide range of frequencies, with an upper limit of approximately 5.1 MHz. Many potential applications could benefit from this high operation frequency.
url http://dx.doi.org/10.1063/1.5100948
work_keys_str_mv AT benjaminkrhea highfrequencyrealizationofnonautonomousnonlineartransistorcircuit
AT edmonperkins highfrequencyrealizationofnonautonomousnonlineartransistorcircuit
AT robertndean highfrequencyrealizationofnonautonomousnonlineartransistorcircuit
_version_ 1725215726997864448