Enhanced Ion Tweeter Our Team Members Rob Alejnikov Mark Blattner Colin Joye Our Advisor Dr. Robert...
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Transcript of Enhanced Ion Tweeter Our Team Members Rob Alejnikov Mark Blattner Colin Joye Our Advisor Dr. Robert...
Enhanced Ion TweeterOur Team Members Rob Alejnikov Mark Blattner Colin Joye
Our Advisor Dr. Robert Caverly
Project ObjectivesWhat did we do?
Created an audio transducer that offers the same frequency content in all directions.
Concentrated on high frequencies since they tend to beam the most.
How we did it: The Ion flame What is it? Voltage --> flame size --> sound Existing devices use vacuum tubes, creating
excessive heat
Goal Raise power efficiency Decrease unit cost
Presentation Objectives
Intro, Audio Subsystem – RobHigh Voltage Generation – MarkResults and Conclusions – Colin
The Audio SubsystemNeed
Ion tweeter cannot implement low frequencies --> Filter Output of source device (CD, cassette) up to 1 V; power
rail modulation requires ~ 30 V --> Gain
Design Criteria Flat frequency response for high audio frequencies Sufficient gain on signal passed to high voltage circuit
The Audio Subsystem
3-stage implementation
Buffer for high input impedance
Low Pass High Pass
Performance measures Cutoff at 4 kHz and 40
kHz Total gain factor up to
60
High Voltage Circuit Operation
Generates high voltage necessary for Corona DischargeMajor Components
Power MOSFET MOSFET Gate Driver Coil
Uses Resonant Properties of Coil to produce High VoltagesSelf-Oscillating nature of circuit provides resilience to environmental changes
Coil ImplementationsKeys to producing High Voltage
Resonant Frequency between 3MHz and 8MHz to avoid audible hiss and limitations of technology
High Quality Factor (Q) causes near open circuit
Low DC resistance
Coil Implementations
10 Coils Built and TestedBuilt with Varying Specs
Dimension, wire gauge, and number of turns
Coil Chosen 16 Gauge Wire 45 Turns 5 MHz Resonance D=3” H=2.5”
Field Effect Transistor (FET)
FET rapidly switches a small current in the coil.Optimal FET
High Voltage handling >500 volts
High Transconductance Greater current in coil
Low Gate Capacitance <500 pico-Farads Reduces stress on Gate
Driver
Interface MethodsNumerous Approaches Tried and Tested
Pulse Width Modulation (PWM) via Gate Driver Power Rail Modulation via Audio Transformer Ground Rail Modulation via Audio Transformer Faraday Shield Modulation
Interface Methods
Decided on Power Rail Modulation PWM unable to obtain clean waveforms and
oscillations Faraday Shield requires very High Voltages
Noise versus Coil Frequency
Flame Flicker Noise present up to 3MHz, as noted by Siegfried Klein in 1956.This noise is virtually inaudible 7MHz and up.At 30MHz, the flame has a different appearance and no noise.
Testing
Power Efficiency TestTube-based:
114W at 1cm flame height.
FET-based: 67W at 1cm flame
height.
40% Power savings
Unit CostUnit Cost (45% savings):
FET: $48.46 (to us), $65.44 (industry)
Tube: $120.53
Total man-hours: 750 man-hours
Estimated industry cost: $45,270
Recommendations
For Increased Linearity: Pulse Width modulation of the FET.
Requires high speed, high precision circuitry.
Requires virtually zero extra power. Occupies almost no space.
Faraday Shield Modulation. Affects the voltage gradient directly. Requires high voltage audio.
Increase operation frequencyIncrease flame power