To generate signals in a range of frequencies between a few tens of kilohertz to 30 or 40 MHz, the Hartley oscillator shown in figure 1 fits perfectly.

 


 

 

    In this circuit is the resonant pair LC that determine the frequency of operation. For high frequencies we can use either an adjustable core coil or a variable capacitor. The values ​​of C1 are chosen according to the range of frequencies to be generated, as well as the coil, which must be wound on a ferrite rod for frequencies below 20 MHz and without a core above 20 MHz.

   The table below gives the number of turns in a rod 1 cm in diameter x 10 cm in length as well as the value of C1. The value of C is also given

 

   For the values ​​of resistors indicated in the diagram the power can be between 3 and 12 V. The formula next to the diagram allows to calculate more accurately the frequency of operation.

   In figure 2 we have a suggestion of printed circuit board for the assembly of this oscillator.

 

 


 

 

 

   We observed that for frequencies above 1 MHz the capacitors must be ceramic.

 

 

Material list

 

Q1 - BC548 or equivalent - NPN general purpose transistor

C1 - 1 nF at 100 nF - capacitor - see table

C - capacitor - see table

L - coil according to frequency - see table

R1 - 10 k ohm x 1/8 W - resistor

R2 - 5.6 k ohm x 1/8 W - resistor

Several:

Printed circuit board, wires, ferrite core for coil, solder, etc.

 

 

 

 
Frequency  
C1  
L  
C
 
10 kHz to 100 kHz  
22 a 100 nF  
200 - 500 turns  
10 a 100 nF
 
100 kHz to 1 MHz  
4,7 nF a 22 nF  
100 - 200 turns  
100 pF a 10 nF
 
1 MHz to 10 MHz  
2,2 nF a 4,7 nF  
20 - 100 turns  
10 pF a 1 nF
 
10 MHz to 30 Mhz  
470 pF a 1 nF  
8 - 20 turns  
4,7 pF a 10 pF