A Hartley oscillator is a type of LC oscillator circuit that generates a sinusoidal output signal at a specific frequency. It was invented by Ralph Hartley in 1915 and is commonly used in radio frequency (RF) applications and other electronic circuits where a stable and accurate oscillator frequency is required. The oscillator circuit is named after its inventor.
The basic operation of a Hartley oscillator involves the interaction of two reactive components, usually inductors and capacitors, to form a resonant tank circuit. The tank circuit is coupled to a transistor amplifier, and the feedback from the output of the amplifier to the tank circuit sustains the oscillations.
Here's a step-by-step explanation of the Hartley oscillator circuit's operation:
Tank Circuit: The essential frequency-determining components in a Hartley oscillator are two inductors (L1 and L2) and a capacitor (C). These components are connected to form a resonant tank circuit. The tank circuit can be arranged in several configurations, but the most common one involves connecting the two inductors in series and connecting the capacitor between the junction of the inductors and the ground.
Resonance: The tank circuit functions as a band-pass filter and allows only a specific frequency (the resonant frequency) to be transmitted while attenuating other frequencies. The resonant frequency (f) of the tank circuit is determined by the values of the inductors (L1 and L2) and the capacitor (C) and can be calculated using the formula:
f = 1 / (2π√(L1 * L2 * C))
The resonant frequency is also influenced by the mutual inductance between L1 and L2, which can affect the coupling coefficient in the calculation.
Transistor Amplifier: The tank circuit is connected to a transistor amplifier. The transistor used is typically a bipolar junction transistor (BJT) or a field-effect transistor (FET) configured in a common-emitter or common-source configuration, respectively.
Feedback: The output of the transistor amplifier is coupled back to the tank circuit. This feedback is achieved by tapping a portion of the amplified output voltage and feeding it back to the junction between L1 and L2 in the tank circuit.
Phase Shift: The feedback creates a phase shift of 180 degrees between the input and the output of the amplifier at the resonant frequency of the tank circuit. This condition ensures positive feedback, causing the circuit to oscillate.
Oscillation: When the circuit is turned on, it starts oscillating at the resonant frequency determined by the tank circuit components. The sinusoidal waveform is generated at the output of the amplifier, and this signal is then fed back to the tank circuit to maintain the oscillations.
Amplitude Control: To ensure that the oscillations sustain without clipping, appropriate biasing and gain control mechanisms are employed in the transistor amplifier.
Frequency-Determining Components:
The frequency of oscillation of a Hartley oscillator is primarily determined by the inductors (L1 and L2) and the capacitor (C) in the tank circuit. By adjusting the values of these components, you can set the desired frequency of oscillation. The resonant frequency can be calculated using the formula mentioned earlier:
f = 1 / (2π√(L1 * L2 * C))
By altering the inductance or capacitance values, you can change the resonant frequency of the Hartley oscillator circuit.
In summary, a Hartley oscillator uses a resonant tank circuit coupled to a transistor amplifier to generate stable oscillations at a specific frequency. The resonant frequency is primarily determined by the inductors and capacitor in the tank circuit. It is widely used in various electronic applications where a stable oscillator frequency is required.