Colpitts振荡电路动力学特性的PSPICE仿真分析

以Colpitts振荡器电路为例,在建立Colpitts电路模型的基础上,对其进行PSpice仿真研究,观察状态变量分别在时域和频域中的变化.通过调整电路元件的参数,观察Colpitts电路中动力学行为的演变过程,得到了与理论分析相吻合的结果.可以发现,电路处于混沌态和准周期态的参数组合不是唯一的.     

基于MOSFET PDE模型的射频自治电路周期稳态算法研究

本文研究了基于MOSFET PDE模型的射频自治电路周期稳态求解算法.采用该算法仿真典型的Colpitts振荡器电路,得到电压波形和工业界公认标准器件仿真器MEDICI瞬态模拟得到电压波形具有很好的一致性.     

不同阶Colpitts混沌振荡电路的性能对比分析

宽带混沌信号拥有良好的相关特性、低截获概率和高保密性等优点.本文介绍了一种基本的混沌信号产生电路-Colpitts振荡电路,在此基础上,对该电路作了相关改进,同时通过仿真对它们的性能进行了分析比较.结果显示:对三阶Colpitts振荡电路的改进方法是可行的;三阶Colpitts振荡电路频谱较为集中,且自相关性能差,应用...     

基本电子电路

TN702,TN752.52006010724基于预设定频率分布的Colpitts混沌电路设计/史治国,冉立新,陈抗生(浙江大学信息与电子工程学系)//浙江大学学报(工学版).―2005,39(3).―402～406.为了找出Colpitts混沌电路的设计综合准则,给出基于预设定频率分布的电路主要元件参数表达式。通过引入了电路的数学模型,导出电路的归一化状态方程,在电路仿真的基础上,得到电路的频率分布特征。根据三个预设定的频率分布,计算出电路主要元件参数,使用专业的射频微波仿真软件高级设计系统(ADS)对电路进行仿真。仿真结果表明,在上限频率为100MHz～1GHz的预设定频…     

微波Colpitts混沌电路实验研究

本文首先介绍了Colpitts电路的数学模型，给出了基于预设定频谱分布的Colpitts混沌电路中主要电路参数的设计方法；然后对工作在微波频段的Colpitts混沌电路进行了实验研究，验证了给出的电路参数设计方案；最后对实验过程中的电路调试方法，电路频谱宽度的瓶颈问题，电路功耗问题以及进一步的工作进行了讨论。     

一种网格多涡卷混沌Colpitts振荡器及其电路实现

基于单涡卷混沌Colpitts振荡器模型,提出了一种网格多涡卷混沌Colpitts振荡器模型。利用阶跃函数代替单涡卷混沌Colpitts振荡器模型中的非线性函数,以及增加一个饱和函数,构造了一个能产生网格多涡卷混沌吸引子的Colpitts振荡器模型。通过数值仿真与电路实验,验证了该网格多涡卷混沌Colpitts振荡器的可行性。     

非理想信道下Colpitts混沌电路的自适应同步研究

本文研究了Colpitts混沌电路在非理想信道条件下的自适应同步问题。引入自适应控制器对输入到响应部分（response system）的衰变混沌信号进行预处理，来补偿衰落信道对于同步性能的影响。给出了系统的数学模型，对恒定信道衰变和时变信道衰变两种非理想信道条件下的混沌ColpiRs电路的自适应同步进行了数值仿真研究。仿真结果表明，对于恒定或慢变化的时变信道衰变，自适应控制器可以有效的提高Colpitts电路响应部分和驱动部分（Drive system）的同步性能。     

借助EWB仿真软件分析混沌电路

通过虚拟电子实验室EWB软件仿真了非线性系统产生的混沌现象,以Colpitts振荡器电路为例,讨论了在电路中设置不同的元件参数值时产生的不同混沌,并介绍了这种动态混沌在通信系统中作为信息载体的重要应用.     

宽带连续混沌波形信号的研究与设计

针对现代战场对信息信号低截获概率的要求,分析研究了宽带连续混沌信号的低截获性,并对失谐耦合型考必兹宽带混沌电路进行研究,并分析比较了不同耦合方式的Colpitts振荡器电路,同时对该混沌电路产生的连续混沌波形信号做出分析,最后仿真出了该混沌信号的模糊函数图。仿真结果显示该混沌信号基底分布均匀,近似于理想的"图钉型",具有良好的距离和速度分辨率的同时,也具有更强的杂波抑制能力。     

一种改进的CMOS差分LC压控振荡器

介绍了一种改进的LC振荡器设计方法.谐振回路采用非对称电容结构,与常见的振荡器结构相比,经改进后的电路结构可以获得更好的相位噪声.基于0.35μm CMOS工艺,设计了一种采用补偿Colpitts振荡器电路结构实现的差分LC压控振荡器,工作电压为2.5V.经仿真证明,在设计中通过调整非对称电容谐振回路中的电容值,可以获得最优的相位噪声.     

A study of phase noise in colpitts and LC-tank CMOS oscillators

This paper presents a study of phase noise in CMOS Colpitts and LC-tank oscillators. Closed-form symbolic formulas for the 1/f/sup 2/ phase-noise region are derived for both the Colpitts oscillator (either single-ended or differential) and the LC-tank oscillator, yielding highly accurate results under very general assumptions. A comparison between the differential Colpitts and the LC-tank oscillator is also carried out, which shows that the latter is capable of a 2-dB lower phase-noise figure-of-merit (FoM) when simplified oscillator designs and ideal MOS models are adopted. Several prototypes of both Colpitts and LC-tank oscillators have been implemented in a 0.35-/spl mu/m CMOS process. The best performance of the LC-tank oscillators shows a phase noise of -142dBc/Hz at 3-MHz offset frequency from a 2.9-GHz carrier with a 16-mW power consumption, resulting in an excellent FoM of /spl sim/189 dBc/Hz. For the same oscillation frequency, the FoM displayed by the differential Colpitts oscillators is /spl sim/5 dB lower.     

Improved chaotic Colpitts oscillator for ultrahigh frequencies

A novel version of the Colpitts oscillator is presented generating chaotic oscillations at gigahertz frequencies. In contrast to the standard oscillator the inductor is moved from the collector circuit of the transistor to the base circuit. PSpice simulations demonstrate chaos at the fundamental frequencies of 0.5, 1 and 2 GHz employing transistors with a threshold frequency of 9 GHz.     

Two-stage chaotic Colpitts oscillator

A novel version of the chaotic Colpitts oscillator is proposed. It contains two bipolar junction transistors coupled in series. The resonance loop consists of an inductor and three capacitors. The two-stage oscillator, compared with the classical circuit, enables the fundamental frequency of chaotic oscillations to be increased by a factor of three. The PSpice simulations performed with 9 GHz threshold frequency transistors demonstrate that the highest fundamental frequencies of chaotic behaviour are 1 and 3 GHz for the classical and the two-stage Colpitts oscillator, respectively     

基于考毕兹振荡器的宽带混沌电路设计

针对某些雷达、通信等系统在应用中对混沌信号频域带宽的要求,设计了一种基于考毕兹振荡器电路的宽带混沌信号发生器。该混沌信号产生电路由考毕兹振荡器为基本谐振电路、级联若干容阻串并联单元的选频网络构成,混沌信号的上下限频率分别由基本谐振电路和第一节容阻串并联网络参数决定,通带频谱的平坦性受其他级联选频网络影响。根据初步分析和仿真试验,该混沌电路组成结构简单,能够产生带宽超过60MHz较为平坦的宽带混沌信号。     

Feasibility of Analog Realization of a Sliding-Mode Observer: Application to Data Transmission

One of the main contributions of this paper is to highlight the feasibility of analog realization of a chaotic observer-based communication system. The system is composed of a chaotic Colpitts oscillator considered as transmitter and a sliding-mode observer used as receiver. The method used in this realization is based on the synchronization of two chaotic systems (transmitter-receiver). Moreover, another originality of this work is the application of a sliding-mode observer to a Colpitts oscillator, which has a totally different structure with respect to it. Nevertheless, the proposed structure of the observer is designed particularly for this type of oscillator. Only one of the states of the transmitter (chosen according to theoretical criteria) is sent to the receiver which is designed to reconstruct all of the states of the transmitter knowing only the transmitted state. In order to show an application of this work, a message signal is injected into the transmitter using the so-called inclusion method. The message is then recovered by the receiver once all of the transmitter states are reconstructed. Thus, the so-called left inversion problem is resolved experimentally. The whole system (transmitter-observer) is realized using simple and standard analog components, and practical results close to simulations are obtained.     

Common-mode oscillation in capacitivecoupled differential Colpitts oscillators

A simple approach to the realisation of a differential Colpitts oscillator is to connect the grounded capacitor in the feedback network of two single-ended Colpitts oscillators together in series. As the output signals are expected to be differential, it is proved in this Letter that, this is not always the case. In certain circumstances, this topology exhibits a common-mode output signal, or even worse, a combination between differential-mode and common-mode waveforms. Design criteria for avoiding these undesirable oscillating behaviours are derived by considering the start-up characteristic of the oscillator.     

A Differential Two-Pin Crystal Oscillator—Concept, Analysis, and Implementation

This brief presents the concept, analysis, design, and measurement results of a differential integrated crystal oscillator (XTO). The XTO requires only two package pins and is connected parallel to the crystal and to the load capacitor, but the amount of negative oscillator resistance R_oscR_osc is defined as the negative real part of the impedance (Z2 in Fig. 1) seen by the series resonance circuit inside the crystal: R_osc=-Re(Z₂). is similar to that of three-pin XTOs such as Pierce or Colpitts. The basic idea is to use three small integrated capacitors and two differential transconductance stages to construct an impedance similar to that of Pierce or Colpitts XTOs     

基于高次谐波体声波谐振器的微波振荡器设计

基于高次谐波体声波谐振器(HBAR)的高品质因数(Q)值和多模谐振特性,设计了Colpitts和Pierce两种形式的微波振荡器。采用HBAR与LC元件组成谐振回路的方法,与放大电路构成反馈环路直接基频输出微波频段信号。Colpitts振荡器输出信号频率为980 MHz,信号输出功率为-4.92dBm,信号相位噪声达-119.64dBc/Hz@10kHz;Pierce振荡电路输出信号频率达到2.962GHz,信号输出功率为-9.77dBm,信号相位噪声达-112.30dBc/Hz@10kHz。