To study the perception of "sound" induced by irradiation with pulse-modulated, ultrahigh-frequency electromagnetic energy and to answer the following questions: 1) Is perceived loudness a function of peak power, average power, or both? 2) What is the required energy density for the perceptual threshold? 3) Is there a minimal or optimal pulse width? Are there modulation characteristics that yield the perception of pitch?
Exposure | Parameters |
---|---|
Exposure 1:
1.245 GHz
Modulation type:
pulsed
Exposure duration:
intermittent, 5 s off/2 s on
|
|
Exposure 2:
1.245 GHz
Modulation type:
pulsed
Exposure duration:
intermittent 5 s off / 2 s on
|
|
Frequency | 1.245 GHz |
---|---|
Type | |
Polarization | |
Exposure duration | intermittent, 5 s off/2 s on |
Additional info | vertical polarisation |
Modulation type | pulsed |
---|---|
Repetition frequency | 50 Hz |
Additional info |
pulse widths of 70, 60, 50, 30, 20, 10 µs, and 40 µs (special case) |
Exposure source |
|
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Setup | The subject sat on a wooden stool with his back to the antenna and his head fixed in space by placing his chin on an acrylic rest mounted on a wooden pole. |
Additional info | Each trial started with a brief dim light; after a variable period of up to 5 s, a reference RF sound was presented for 2 s, followed by a silent period of about 5 s, and finally the RF sound of variable loudness was presented for 2 s. Occasionally, no variable RF sound was presented at the expected time in order to test for false positives. |
Measurand | Value | Type | Method | Mass | Remarks |
---|---|---|---|---|---|
power density | 90 mW/cm² | peak value | measured | - | 70 µs |
power density | 105 mW/cm² | peak value | measured | - | 60 µs |
power density | 125 mW/cm² | peak value | measured | - | 50 µs |
power density | 210 mW/cm² | peak value | measured | - | 30 µs |
power density | 315 mW/cm² | peak value | measured | - | 20 µs |
power density | 630 mW/cm² | peak value | measured | - | 10 µs |
power density | 0.32 mW/cm² | mean | measured | - | kept constant for all pulse widths |
Frequency | 1.245 GHz |
---|---|
Type | |
Polarization | |
Exposure duration | intermittent 5 s off / 2 s on |
Additional info | vertical polarisation |
Modulation type | pulsed |
---|---|
Repetition frequency | 50 Hz |
Additional info |
pulse widths of 10, 20, 30, 50, 60, and 70 µs |
Exposure source |
|
---|
Measurand | Value | Type | Method | Mass | Remarks |
---|---|---|---|---|---|
power density | 370 mW/cm² | peak value | measured | - | - |
power density | 0.19 mW/cm² | mean | measured | - | 10 µs |
power density | 0.37 mW/cm² | mean | measured | - | 20 µs |
power density | 0.55 mW/cm² | mean | measured | - | 30 µs |
power density | 0.93 mW/cm² | mean | measured | - | 50 µs |
power density | 1.11 mW/cm² | mean | measured | - | 60 µs |
power density | 1.29 mW/cm² | mean | measured | - | 70 µs |
The perceived loudness of the radiofrequency sound and within the limitation of the radiofrequency parameters investigated here, is a function of peak power rather than average power. Calculations from the data presented indicate that in this particular study, the peak power required for perception is somewhat less than 80 mW/cm². A band of optimal pulse widths seems to exist for the effect and there are also radiofrequency modulation parameters that cause subjects to report hearing "sounds" with definite pitch and timbre characteristics.
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