Capacitance of diodes
From data sheet, the Cj0 of D1N4002 and D1N4004 are both 15pF.
Figure 1: datasheet of diodes
For Pispice, Cj0 of D1N4002 is 51.17pF.
According to lab results, Cj0 of D1N4002 is 61.8pF.
Cj0 of D1N4004 is 58 pF.
Resonance frequency
The resonance frequency is 102.516KHz.
When the amplitude of the source voltage is 50mV and the resistor is 100KΩ, the lab results are shown in the following table.
Frequency(Hz) | VR(mV) |
10 | 5 |
50 | 5 |
100 | 5 |
500 | 5 |
1000 | 5.4 |
5000 | 7.2 |
8000 | 10.8 |
10000 | 12.6 |
30000 | 20.6 |
50000 | 23.4 |
80000 | 30.4 |
97160 | 49.2 |
100000 | 21.2 |
300000 | 19 |
1000000 | 17.9 |
This figure is similar to the Pspice simulation
Figure 3 shows the resonance frequency of D1N4002 using Pspice
Figure 3: Resonance frequency for D1N4002 using Pspice
For D1N4004, C(measurement)= 58pF, L=39mH.
The resonance frequency is 105.821KHz.
When the amplitude of the source voltage is 50mV and the resistor is 100KΩ, the lab results are shown in the following table.
The resonance frequency is 99.13KHz.
Frequency(Hz) | VR(mV) |
10 | 5 |
50 | 5 |
100 | 5 |
500 | 5 |
1000 | 5.2 |
5000 | 7 |
8000 | 10.4 |
10000 | 12.4 |
30000 | 18.2 |
50000 | 21 |
80000 | 26.2 |
99130 | 42.6 |
100000 | 42.2 |
1000000 | 15.6 |
Figure 4: Resonance frequency for D1N4004
Resonance frequency shift
According to theory, resonance frequency should not change as the value of the resistor change.
But, in reality, resonance frequency increases with the value of the resistor increasing.
For D1N4002, when VPP of the source voltage is 100mV, the lab results are shown in the following table.
Resonance frequency(KHz) | VR(mV) | |
10000 | 89.6 | 25.6 |
55000 | 94.63 | 48 |
100000 | 95.92 | 49.6 |
Table 3: Resonance frequency change with resistor changing
This result compromises with the Pspice simulation.
Resistor(Ω) | Resonance frequency(KHz) | VR(mV) |
55000 | 109.548 | 49.824 |
100000 | 112.074 | 49.896 |
1000000 | 122.775 | 49.991 |
Table 4: Resonance frequency change with resistor changing using Pspice
Chaotic phenomenon
Chaotic circuit is a dynamic system caused by nonlinear component.
If the voltage of the source is fit, hovers around a limit ellipse can be observed.
The orbits of hovers never intersect.
Figure 6: D1N4002 totally chaotic at the frequency of resonance frequency |
The following radio shows the circuit starts becoming chaotic.








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