Friday, 3 February 2012

Second Lab

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.

We do not know why there is a huge difference among the Cj0 of Pspice, datasheet and measurement.

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 5:D1N4002 partly chaotic


Figure 6: D1N4002 totally chaotic at the frequency of resonance frequency 


Figure7: Partly chaotic D1N4004 


D1N4004 completely chaotic at the frequency of chaotic frequency


 The following radio shows the circuit starts becoming chaotic.



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