Design of a 1-D Sonic Anemometer MDR Presentation Group Members: Vanessa Dubé, Michael Jao, Chethan Srinivasa, Robert Vice Advisors: Professor Jackson.

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Presentation transcript:

Design of a 1-D Sonic Anemometer MDR Presentation Group Members: Vanessa Dubé, Michael Jao, Chethan Srinivasa, Robert Vice Advisors: Professor Jackson (ECE Department), Professor Voss (Geoscience Department)

Background What is a Sonic Anemometer? –Device that measures wind speed What is unique about our anemometer? –Will measure small wind speeds –Will be utilized by the Geoscience Department for weather research

Background (Cont’d) Anemometer uses transducers to send and receive ultrasonic signals through air Used two transmitters and two receivers Absolute time will vary with wind speed Sine wave sent from function generator to both transmitters

Block Diagram Frequency Generator Comparator Circuitry LED Display PLD Speaker 1 Receiver 2Speaker 2 Receiver 1

Initial Calculations Found how absolute time was affected by a change of 1mm/s in velocity –Began with simple equations for velocity that relate distance, time, and temperature to speed of signal –Assumed room temperature, so that the velocity of sound in air was m/s – Looked at the change in absolute time that resulted from a change of 1mm/s in wind speed over a distance of 1.06 m

Initial Calculations (Cont’d) –Calculated t 1 and t 2 –Found change in absolute time Found the frequency of the counter we will need –Chose a counter frequency higher than 58.95MHz –Solved for the number of bits in the counter register

Zero Crossing Detector Chose to convert sine waves to digital signals using LM339 Comparator Digital signal is high only when amplitude of the sine wave is greater than zero Distance between zero crossings stays the same width Must use zero crossings because of amplitude variations caused by side winds Phase difference of two received waves is the difference in zero crossing locations

Comparator Used LM339 because operates at higher frequencies and has less delay time Comparator circuitry:

Comparator (Cont’d) Input and output waveforms of comparator circuitry

Comparator Theory This shows that we only need to find the change in time between the two waves. For Example:

Transducers Part numbers P9895-ND and P9894-ND One for transmit and one for receive Lowest frequency for cost effectiveness and familiarization Nominal frequency 40.0 kHz Temperature range °C Sensitivity is 0dB

Optimal measured frequency of 40.2 kHz Continuous sine input for optimal received signal Transducers (Cont’d)

Test Setup DC fan 4”x84” PVC drain pipe Quick-cap (end cap) 6’x2”x2” pine board with slots separated 5” CD case for mounts Wendy’s™ straws Twisted pair insulated wire

Wind Flow Testing Developed method to test wind speed generated by fan

Wind Flow Testing (Cont’d)

Read phase difference from oscilloscope Compared generated wind speed to wind speed observed by system Found observed wind speed to be relatively close to actual wind speed

Wind Flow Testing (Cont’d)

PLD/Counter PLD Controller (Left) - For direction and clock signal PLD Counter (Right) - Temporary until counter is received 4 MHz clock (will use 125MHz )

Complications BiCMOS Comparator has offset base current, which affects the zero-crossing detection An LM741 is not capable of functioning properly with a 40kHz signal, which forced us to use the LM339 comparator Side winds affect the amplitude of the wave, which greatly affects the zero-crossing detection Noise in the system had to be minimized

Expenses

Conclusion We were able to remedy several of the complications Anemometer is capable of measuring a wind speed, and was tested on the oscilloscope Although there is an initial offset, shown by the graphs, the proper trend is followed From here, we will be able to use digital logic and display the wind speed on 15 LED’s, as well as display the direction