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A '''Colpitts oscillator''', invented in 1918 by American engineer [[Edwin H. Colpitts]],<ref>{{Citation |country-code=US |patent-number=1624537 |inventor-last=Colpitts |inventor-first=Edwin H. |title=Oscillation generator |publication-date=1 February 1918 |issue-date=12 April 1927 }}</ref> is one of a number of designs for [[LC oscillator]]s, [[electronic oscillator]]s that use a combination of [[inductor]]s (L) and [[capacitor]]s (C) to produce an oscillation at a certain frequency. The distinguishing feature of the Colpitts oscillator is that the [[feedback]] for the active device is taken from a [[voltage divider]] made of two capacitors in series across the inductor.<ref name="Gottlieb">{{cite book 
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  | last = Gottlieb
  | first = Irving Gottlieb
  | title = Practical Oscillator Handbook
  | publisher = Elsevier
  | year = 1997
  | location = US
  | pages = 151
  | url = http://books.google.com/books?id=e_oZ69GAuxAC&pg=PA151&dq=Colpitts+oscillator+%22capacitor+voltage+divider
  | doi =
  | id =
  | isbn = 0750631023}}</ref><ref name="Carr">{{cite book 
  | last = Carr
  | first = Joe
  | title = RF Components and Circuits
  | publisher = Newnes
  | year = 2002
  | location = US
  | pages = 127
  | url = http://books.google.com/books?id=V9gBTNvt3zIC&pg=PA127&dq=Colpitts+oscillator+%22capacitive+voltage+divider
  | doi =
  | id =
  | isbn = 0750648449}}</ref><ref name="Basak">{{cite book 
  | last = Basak
  | first = A.
  | title = Analogue Electronic Circuits and Systems
  | publisher = Cambridge University Press
  | year = 1991
  | location = UK
  | pages = 153
  | url = http://books.google.com/books?id=vwnMPZx7wfkC&pg=PA153&dq=Colpitts+oscillator+%22capacitive+voltage+divider%
  | doi =
  | id =
  | isbn = 0521360463}}</ref><ref name="Rohde">{{cite book 
  | last = Rohde
  | first = Ulrich L.
  | authorlink =
  | coauthors =  Matthias Rudolph
  | title = RF / Microwave Circuit Design for Wireless Applications, 2nd Ed.
  | publisher = John Wiley & Sons
  | year = 2012
  | location =
  | pages = 745–746
  | url = http://books.google.com/books?id=Y5ZiwX2Ap5cC&pg=PA745&dq=Colpitts+oscillator+%22capacitive+voltage+divider
  | doi =
  | id =
  | isbn = 1118431405}}</ref>


==Overview==
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{| align="right"
|-
| valign="top" | [[Image:Cb colp.svg|thumb|130px|Figure 1: Simple [[common base]] Colpitts oscillator (with simplified [[biasing]])]]
| valign="top" | [[Image:Cc colp2.svg|thumb|130px|Figure 2: Simple [[common collector]] Colpitts oscillator (with simplified [[biasing]])]]
|-
| colspan="2" | [[Image:NPN Colpitts oscillator collector coil.svg|thumb|300px|Figure 3: Practical common base Colpitts oscillator (with an oscillation frequency of ~50 MHz)]]
|}
The Colpitts circuit, like other LC oscillators, consists of a gain device (such as a bipolar junction [[transistor]], field effect transistor, operational amplifier, or [[vacuum tube]]) with its output connected to its input in a [[feedback loop]] containing a parallel [[LC circuit]] ([[tuned circuit]]) which functions as a [[bandpass filter]] to set the frequency of oscillation.


A Colpitts oscillator is the electrical dual of a [[Hartley oscillator]], where the feedback signal is taken from an "inductive" voltage divider consisting of two coils in series (or a tapped coil).  Fig. 1 shows the common-base Colpitts circuit. ''L'' and the series combination of ''C''<sub>1</sub> and ''C''<sub>2</sub> form the parallel resonant tank circuit which determines the frequency of the oscillator. The voltage across ''C''<sub>2</sub> is applied to the base-emitter junction of the transistor, as feedback to create oscillations.  Fig. 2 shows the common-collector version. Here the voltage across ''C''<sub>1</sub> provides feedback.  The frequency of oscillation is approximately the resonant frequency of the LC circuit, which is the series combination of the two capacitors in parallel with the inductor
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:<math>f_0 = {1 \over 2 \pi \sqrt {L \left ({ C_1 C_2 \over C_1 + C_2 }\right ) }}</math>
The actual frequency of oscillation will be slightly lower due to junction capacitances and resistive loading of the transistor.


As with any oscillator, the amplification of the active component should be marginally larger than the attenuation of the capacitive voltage divider, to obtain stable operation. Thus, a Colpitts oscillator used as a [[variable frequency oscillator]] (VFO) performs best when a variable inductance is used for tuning, as opposed to tuning one of the two capacitors. If tuning by variable capacitor is needed, it should be done via a third capacitor connected in parallel to the inductor (or in series as in the [[Clapp oscillator]]).
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===Practical example===
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Fig. 3 shows a working example with component values. Instead of [[bipolar junction transistor]]s, other active components such as [[field effect transistors]] or  [[vacuum tube]]s, capable of producing gain at the desired frequency, could be used.


==Theory==
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{{cleanup|section|date=April 2008}}
[[Image:Colpitts ideal model.svg|thumb|right|250px|Colpitts oscillator model used in analysis at left.]]


One method of oscillator analysis is to determine the input impedance of an input port neglecting any reactive components. If the impedance yields a [[negative resistance]] term, oscillation is possible. This method will be used here to determine conditions of oscillation and the frequency of oscillation.
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An ideal model is shown to the right. This configuration models the common collector circuit in the section above. For initial analysis, parasitic elements and device non-linearities will be ignored. These terms can be included later in a more rigorous analysis. Even with these approximations, acceptable comparison with experimental results is possible.
 
Ignoring the inductor, the input [[Electrical impedance|impedance]] can be written as
 
:<math>Z_{in} = \frac{v_1}{i_1}</math>
 
Where <math>v_1</math> is the input voltage and <math>i_1</math> is the input current. The voltage <math>v_2</math> is given by
 
:<math>v_2 = i_2 Z_2</math>
 
Where <math>Z_2</math> is the impedance of <math>C_2</math>. The current flowing into <math>C_2</math> is <math>i_2</math>, which is the sum of two currents:
 
:<math>i_2 = i_1 + i_s</math>
 
Where <math>i_s</math> is the current supplied by the transistor. <math>i_s</math> is a dependent current source given by
 
:<math>i_s = g_m \left ( v_1 - v_2 \right )</math>
 
Where <math>g_m</math> is the [[transconductance]] of the transistor. The input current <math>i_1</math> is given by
 
:<math>i_1 = \frac{v_1 - v_2}{Z_1}</math>
 
Where <math>Z_1</math> is the impedance of <math>C_1</math>. Solving for <math>v_2</math> and substituting above yields
 
:<math>Z_{in} = Z_1 + Z_2 + g_m Z_1 Z_2</math>
 
The input impedance appears as the two capacitors in series with an interesting term, <math>R_{in}</math> which is proportional to the product of the two impedances:
 
:<math>R_{in} = g_m \cdot Z_1 \cdot Z_2</math>
 
If <math>Z_1</math> and <math>Z_2</math> are complex and of the same sign, <math>R_{in}</math> will be a [[negative resistance]]. If the impedances for <math>Z_1</math> and <math>Z_2</math> are substituted, <math>R_{in}</math> is
 
:<math>R_{in} = \frac{-g_m}{\omega ^ 2 C_1 C_2}</math>
 
If an inductor is connected to the input, the circuit will oscillate if the magnitude of the negative resistance is greater than the resistance of the inductor and any stray elements. The frequency of oscillation is as given in the previous section.
 
For the example oscillator above, the emitter current is roughly 1 [[Ampere|mA]]. The transconductance is roughly 40 [[Siemens (unit)|mS]]. Given all other values, the input resistance is roughly
 
:<math>R_{in} = -30 \ \Omega</math>
 
This value should be sufficient to overcome any positive resistance in the circuit. By inspection, oscillation is more likely for larger values of transconductance and smaller values of capacitance.  A more complicated analysis of the common-base oscillator reveals that a low frequency amplifier voltage gain must be at least four to achieve oscillation.<ref>Razavi, B.  Design of Analog CMOS Integrated Circuits. McGraw-Hill. 2001.</ref>  The low frequency gain is given by:
 
:<math>A_v = g_m \cdot R_p  \ge 4</math>
 
If the two capacitors are replaced by inductors and magnetic coupling is ignored, the circuit becomes a [[Hartley oscillator]]. In that case, the input impedance is the sum of the two inductors and a negative resistance given by:
 
:<math>R_{in} = -g_m \omega ^ 2 L_1 L_2</math>
 
In the Hartley circuit, oscillation is more likely for larger values of transconductance and larger values of inductance.
 
===Oscillation amplitude===
The amplitude of oscillation is generally difficult to predict, but it can often be accurately estimated using the [[describing function]] method.
 
For the common-base oscillator in Figure 1, this approach applied to a simplified model predicts an output (collector) voltage amplitude given by:<ref>Trade-Offs in Analog Circuit Design: The Designer's Companion, Part 1
By Chris Toumazou, George S. Moschytz, Barrie Gilbert [http://books.google.com/books?id=VoBIOvirkiMC&lpg=PA568&ots=MD4aYrSVjr&dq=the%20tank%20voltage%20amplitude%20is%20calculated%20to%20be&pg=PA568#v=onepage&q=the%20tank%20voltage%20amplitude%20is%20calculated%20to%20be&f=false]</ref>
 
:<math>
V_C = 2 I_C R_L \frac{C_2}{C_1 + C_2}
</math>
 
where <math>I_C</math> is the bias current, and <math>R_L</math> is the load resistance at the collector.
 
This assumes that the transistor does not saturate, the collector current flows in narrow pulses, and that the output voltage is sinusoidal (low distortion).
 
This approximate result also applies to oscillators employing different active device, such as [[MOSFET]]s and [[vacuum tubes]].
 
==External links==
* [http://www.falstad.com/circuit/e-colpitts.html Java Simulation of a Colpitts oscillator]
 
==References==
{{reflist}}
* Lee, T. The Design of CMOS Radio-Frequency Integrated Circuits. Cambridge University Press. 2004.
* Ulrich L. Rohde, Ajay K. Poddar, Georg Böck "The Design of Modern Microwave Oscillators for Wireless Applications ", John Wiley & Sons, New York, NY, May, 2005, ISBN 0-471-72342-8.
* George Vendelin, Anthony M. Pavio, Ulrich L. Rohde " Microwave Circuit Design Using Linear and Nonlinear Techniques ",  John Wiley & Sons, New York, NY, May, 2005, ISBN 0-471-41479-4.
 
{{Electronic oscillators}}
 
{{DEFAULTSORT:Colpitts Oscillator}}
[[Category:Oscillators]]
[[Category:Electronic design]]

Latest revision as of 11:07, 12 October 2014

The initiation of the X games and their rising popularity in China, surprisingly has been a result of a number of businessmen seeking new business opportunities in sports. They do not realize that it is actually a trap for fools because the gold could only be mined by those who held the key. Several of the well-known villains from the series consist of Venom, Carnage, Squid and Sinister Six. They choose the 'bad guy' amongst themselves, bikes become horses or motorcycles, and the purpose of the game is to track down or hunt the enemy.

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After a bit longer the game will be complete and enter the debugging phase. These peasants and soldiers don't work for free though (what happened to forced labor. The world of Dominion is about to get way darker and more sinister in Dominion: Intrigue, the first standalone expansion for the hit card game that took the world by storm. They also incorporate other features which include, collection of ammunition, tracing the ammunitions, armors and other puzzle machinery.
Information that can hopefully be obtained easily is what type of games console they have. The Nikon 7216 Action binoculars have a close focus advantage for viewing in the backyard and they're great for butterfly watching too. The differences between Orochi, Black Chrome and Blade are only visual:. Each one of these rules by itself may be enough to turn losing into winning. It can make no distinction whether you use an overlapping, interlocking, or ten-finger grip.
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