LC Oscillator: Circuit Working, Types, and Applications

Oscillators are devices that convert a supply voltage, i.e., DC input, into a waveform, the AC output. Often, you will find the output waveform in different frequencies and shapes such as triangular, square, or sawtooth. Further, the waveform shapes can be complex or just a simple sine wave, depending on the application area. 

In this article, we will focus on an LC oscillator, which is a type of oscillator. It is also known as an LC tuned circuit or an LC resonant circuit.

In addition, the article gives an overview of further divisions of the LC oscillators alongside the circuit working.

What is LC Oscillator?

The term LC comes from the tank circuit having an inductor 'L' and capacitor 'C. 

An LC Oscillator is an oscillator type whereby you use an inductor-capacitor (LC) tank circuit to give positive feedback. The feedback is important in maintaining a stable oscillation. 

Almost always, you can comprehend an LC oscillator using an active device like Op-Amps, BJT, MOSFETs, or FET. Other times, they can generate high-frequency signals hence making them RF oscillators. Additionally, they are applicable in a wide range of electronic devices such as tuner capacitors and RF signal generators. 

LC oscillator circuit 

Types of LC Oscillators

• Tuned Collector Oscillator

A tuned collector oscillator is the most basic LC oscillator. It has a capacitor and transformer with a parallel connection crossway to the oscillator's collector circuit. Also, the capacitor and primary of the transformer form the tank circuit. Then, the secondary of the transformer gives a portion of oscillation feedback to the transistor's base. 

A tuned collector oscillator circuit 

• Tuned Base Oscillator

For the tuned base oscillator, you will find the tuned circuit between the ground and base of the transistor. The capacitor and a transformer's primary coil form the tuned circuit. Then, the secondary coil of the transformer gives the feedback signal. 

Tuned base oscillator circuit 

• Hartley Oscillator

Ralph Hartley invented the Hartley oscillator in 1915. For the tank circuit, he placed one capacitor and two inductors. Further, the inductors have a series connection while the capacitor is parallel to the inductors' series combination. Often, its operating oscillation frequency ranges from 20KHz to 20MHz, and you can realize it using Op-Amps, FET, and BJT. 

Hartley oscillator circuit 

• Colpitts Oscillator

The Colpitts oscillator is a type of LC oscillator, invented by Scientist Edwin Colpitts in 1918. Its tank circuit comprises an inductor and two capacitors. The capacitors have a series connection, whereas the inductor has a parallel connection to the capacitor series. Its operating range is approximately 20KHz to MHz. And contrary to the Hartley oscillator, its frequency stability is better and reliable. 

Colpitts oscillator circuit 

• Clapp Oscillator

We consider the Clapp oscillator as a modification of the Colpitts oscillator. Thus, you will find an additional capacitor in the tank circuit falling under the inductor series. The added capacitor varies in variable frequency applications. It also functions to isolate the two existing capacitors from transistor parameter effects such as junction capacitance. What’s more, the extra capacitor heightens frequency stability. 

A Clapp oscillator circuit 

LC Oscillator Application circuit

• LC oscillator with Crystal

Before proceeding to the mechanism of action, let's consider the circuit below.

LC oscillator with crystal circuit 

The large Q in the crystal oscillator minimizes the frequency drift that DC voltage fluctuations and the temperature has triggered. 

Moreover, crystal-controlled oscillators produce less noise than the traditional LC tank-based oscillator circuits, making them reliable in output signals. 

In-circuit 1a, there's a configuration of three feedback circuits with an NPN BJT-based amplifier.

Circuit 1buses C2, C1, and L1 to make up a comparative circuit built. 

Note; The two crystal oscillator circuits above use a minimum of an inductor and two capacitors. The crystal is an element of the feedback circuit.

• C2 and C1 comprise junction capacitance and residual transistor. Besides, C2 is analogous to a parallel network of a capacitor and an inductor. 
• Then, C2 and C1 pair is the third overtone selector of the crystal. It is because it shows capacitive nature mainly at the overtone frequency of the crystal. Also, it exhibits inductive property at the crystal’s fundamental frequency. 
• Thus, the C2 inductor hinders the crystal's fundamental frequency of oscillations. 
• An oscillator circuit requires a limiting factor which is a boundary at the oscillator’s output. The limiting factor complements its feedback and amplification. Majorly, the limitation should occur when the input signal rise doesn’t cause an output signal rise.
• The Colpitts crystal-controlled oscillator has tuning specifications and stringent load. Conversely, the pair of semi-isolated models require less input and are better for general-purpose applications. 
• When it comes to preferences in LC oscillator working, a Pierce crystal oscillator often gives an accurate output frequency. A Butler circuit, on the other hand, oscillates without a crystal. 

• General Colpitts oscillators

Colpitts oscillator circuit 

We have two variations of the Colpitts crystal-controlled oscillator, i.e., the semi-isolated and standard variations. Also, specifications of the load and crystal resistance determine the classic circuit. In addition, the output power has less than 50 % restriction of the crystal's power dissipation but is still efficient. 

• R3, R2, and R1 offer transistor Q1 the DC bias. 
• Potentiometer R2 yields approximately 1.5 mA of the emitter current. 
• C6, C4, and C3 function as bypass elements for the RF at the working frequency of XTAL1.
• C2 is the feedback base circuit.
• C5 and L1 display a net capacitive reactance when the circuit's operating at the operating frequency of XTAL1. Thus, they function as the collector circuit feedback capacitor.
• If you use overtone crystals, C5 and L1 act like an overtone selector, preventing oscillation at the crystal's fundamental frequency. 
• C1, the adjustable trimmer, often tweaks L1 (the feedback component). The oscillator's output frequency will increase while the C1 value decreases.

• Simple LC RF Oscillator

You can build an oscillator with a capacitor network, transistor, and resistor. And so, as you proceed, you'll only use the collector and emitter while leaving the transistor base terminal unconnected. 

The simple LC oscillator circuit figure below often works at approximately 100kHz to 50MHz or sometimes higher.

LC RF oscillator circuit 

• Transistor TR1 has a source follower configuration. 
• Then, the tiny coupling through the T1 inductor winding generates a +ve feedback. Also, it can step up the voltage needed for oscillation maintenance.
• C3 and T1 primary winding form the LC tuned circuit. As a result, there's an establishment of the LC oscillator circuit operating frequency.
• At the supplied Direct Current, R1 is the source load for TR1. AC via C2 bypasses the TR1 hence leading to T1 coupling winding that forms TR1 source load.  
• Afterward, you can derive the oscillator output signal through the TR1 source via C1, the DC blocking capacitor. 
• C4 is the supply decoupling capacitor. 
• If you need to adjust the tuning oscillator, you can replace C3 with a variable capacitor. Alternatively, use a mixture of variable and fixed capacitors to allow the wanted tuning range.
• What's more, you can incorporate ready-made coils when constructing high and medium-frequency LC oscillators. Often, they'll provide more accurate frequency outputs compared to the home-wound waves. 
• When constructing T1 as a DIY project, wind two sets of coils, that is, 6 to 1, and 8 to 9. One set should be below the other around a small ferrite rod. You can also experiment with the number of turns to get varied frequency outputs.

NOTE; you should correctly connect the phasing of the smaller coupling winding. If you don't, your circuit won't oscillate. Thus, it calls for a trial-and-error implementation throughout the project. 

Difference between LC and RC Oscillator

The main differences between RC oscillators and LC oscillators are as follows; 

Application Areas of LC Oscillator

The wide range of applications of LC oscillator include in;

• TVs,
• Radio programs and TV broadcasting,
• Mobile phones,
• Defense and civil communication,
• Surge controls in APFC panels and power capacitors, 
• Filter circuits with LC combinations, 
• Radios for carrier line communication and HV transmission systems, 
• RF generators, tuners, frequency mixers, RF modulators, sine wave generators, and 
• High-frequency heating. 

Conclusion

To summarize, oscillators generate continuous periodic waveforms when you apply a specific frequency. LC oscillator, particularly, is a harmonic oscillator or sinusoidal oscillator which generates high-frequency sine waves. The waves are later applicable in radio frequency applications. In such cases,  FETs or Bipolar transistors act as the transistor amplifier. And, you use them to build an amplifier stage.

The article further elaborates the types of LC oscillators such as Clapp and Colpitts oscillator and their circuits. 

Undeniably, there is still more to LC oscillator technology than what we have highlighted today. Therefore, if you wish to air out your concerns and views, contact us. We’ll be happy to help.