DRAFT: This module has unpublished changes.

First step to testing the antennae was to find the approximate inductance of each antenna.  We did frequency sweeps using a function generator and an oscilloscope to find the resonant peaks of each antenna with given capacitances.  At the resonance frequency of the circuit, a peak in voltage is observed.  The frequency of the peak observed and the given capacitance were used in the following equation to determine inductance:

 

Antenna Test Circuit

This test circuit was used to test the resonance frequency of all coils hand wound and ordered.

 

 

 

Coil 1

 

Antenna Test Circuit

 

A large coil was designed and created based off of calculations from an inductor calculator. 

  

The coil was wrapped on a  wooden core.  This coil was tested using function generators and oscilloscopes at several lab benches to try to find the resonance peak in order to tune it to 125 kHz.  All of the bench tests were inconclusive. 

 

Second to Last Left Lab Bench in Senior Design Tests [ML1]

 

Last Right Lab Bench in Senior Design Tests [ML1]

 

First Right Lab Bench in EE 283 Tests [ML1]

 

 

First Left Lab Bench in EE 283 Tests [ML1]

 

 

Second Left Lab Bench in EE 283 Tests [ML1]

 

We either found multiple peaks or peaks that were completely inconsistent with changing capacitances.  Multiple peaks should not be present except in the case of the existence of harmonics in close range to each other.  It is also seen that doubling capacitance gave almost the same results in two cases. 

 

The data below was generated using the second lab bench on the left in EE283.

 

Finding Peak Voltages To Get Inductance

Capacitance (pF)

Inductance Range (mH) *

Peak Frequency Range (kHz)

Peak Voltage (mVrms)

310

6.5/8.9

112-113/96-97

716/714

300

5.1/6.9

129-130/111-113

708-709/713-714

150

7.8/10.1

162-162/147/129

703-704/709-710/713-714

160

12.4/9.5

113/129

711-712/713

170

11.5/9.1

113.6/128.2/147.1

711-712/712-713/708-709

551

5

96

713

691

5.9/4.1

79/95

715/708

661

4.2/6.1

95-96/79-80

710/714

511

7.7/5.4

80/96

709/715

401

5.1/6.9

111-113/96

711/714

 

 

Averaging Ranges

Capacitance (pF)

150-170

300-691

Inductance (H)

0.009-0.01

0.006-0.007

 

 

Calculating Necessary Capacitance

Frequency (kHz)

125

125

Capacitance (pF)*

180.13

162.11

Inductance (H)

0.009

0.01

 

Based off of the findings of the data, we tried the antenna with 170 pF in the transceiver circuit.  After troubleshooting some connections and removing troublesome parts, we managed to pick up a write signal off of the antenna. 

 

When plugged into the transceiver circuit initially, there was a good modulation but the frequency was very far off. 

 

 

Write Output: Carrier Close Up

 

According to this data, we needed to change our capacitance in the antenna. 

 

With this value, the capacitance needed for the antenna should have been

 

 


Write Output: Modulation Frequency Close Up


The modulation envelope is very clean and is at the correct frequency input into the transceiver.  This shows that the connection debugging and removal of parts around the modulation pin was successful.  However, a retest with the above calculated capacitance gave the same carrier problems. 

  

Using a spectral analyzer, the coil was tuned to 125 kHz.  The inductance was found to be 4.5 mH.  The resonance frequency of the coil changed when plugged into the transceiver circuit.  When it was retuned, the transceiver was ringing with large amounts of decays and frequencies overlapping each other.

 

 

Varying Close ups of Transceiver Circuit Ringing

 

It was concluded that using higher inductance values in the antenna coil causes a great deal of undesirable decays in the circuitry.  Lower value coils were then tested for use.  It was also decided to use round coils for cleaner signals. 

 

The inductance of a round coil is:


Coil 2

A small coil was wrapped around a 28 mm plastic core with 32 turns.  This coil was tested with great results on frequency sweeps using the function generator and an oscilloscope.  The inductance was found to be around 40 µH.  This coil was used in the tag circuit.

 

Coil 2 Testing Data 1 [ML2]

 

Approximate resonance frequency = 168.4 kHz

Approximate Inductance = 40.6 uH

Approximate Capacitance Needed for 125 kHz = 36.35 nF

 

 

Coil 2 Testing Data 2 [ML2]

 

Approximate resonance frequency = 133.35 kHz

Approximate Inductance = 39.2 uH

Approximate Capacitance Needed for 125 kHz = 41.35 nF

 

These values were averaged to L= 39.9 µH and C= 38.84 nF.  These values were used as starting values for tuning the coil with the transceiver circuit.

 

The coil was put into a tag circuit to be tuned.  The capacitance needed for 125 kHz was 40.6 nF for the 39.93 µH coil.

 

 

125 kHz Carrier Close-up

 

2 kHz Modulation Envelope Close-up

 

Tag Circuit with Coil 2

 

 

Coil 3

A coil was ordered online with a value of 2.8 mH.  The capacitance for a 125 kHz resonance with the labeled value is 578.98 pF.  This coil had the same problem as the first coil in testing with frequency sweeps and gave inconclusive results.  Due to these results, it was decided that coil selection for the circuitry would remain in the µH range.

 

Coil 3 Data [ML3]

 

There are no remarkable peaks or consistent variance in voltage.  This is with a capacitance less than 2 pF away from the value calculated from the factory tested value of inductance of the coil.

 

Coil 4

A small coil was wrapped around a 28 mm plastic core with 52 turns.  This coil was tested with great results on frequency sweeps using the function generator and an oscilloscope.  The inductance was found to be around 150 µH.

 

Coil 4 Data [ML4]

The inductance of the coil from this data was calculated to be 154 µH.  The needed capacitance would then be 10.47 nF.

 

Coil 5

A small coil was wrapped around a 16 mm plastic core with 52 turns.  This coil was tested with great results on frequency sweeps using the function generator and an oscilloscope.  The inductance was found to be around 50 µH.  This coil was used in the reader circuit.

 

Coil 5 Data [ML5]

During this test, the circuit resonance frequency was 138.9 kHz.  The calculated inductance was 50 µH.  The capacitance for 125 kHz resonance was approximately 32.42 nF.  This was used as a starting value when tuning the antenna in the transceiver circuit.

 

The coil was put into a tag circuit to be tuned.  The capacitance needed for 125 kHz was 31.04 nF for the 52.23 µH coil.

 

 

125 kHz Carrier Close-up

 

2 kHz Modulation Envelope Close-up

 

 

Reader Circuit with Coil 5

DRAFT: This module has unpublished changes.