Jonathan Thomson's web journal

How to use the TSL2561 May 22, 2012

Filed under: Electronics,Spectrometer — jethomson @ 2:07 am

The TSL2561 is a light-to-digital converter from TAOS. It senses light intensity and transforms its measurement into a digital output that is transferred over I2C or SMB. If you are familiar with the TSL230R light sensors, you shouldn’t have much trouble working with TSL2561s, but there are a few important differences. The TSL230R outputs its data as a pulse train, so a microcontroller with frequency counting code is required to read the sensor’s output. The TSL2561 outputs its data directly over I2C or SMB, so the sensor’s output is simply read from the bus. The TSL230R is controlled by bringing purpose specific pins high or low. The TSL2561 is controlled by writing data to it over the bus. The TSL230R is available in a breadboardable package and runs at 5V. The TSL2561 needs an adapter board for breadboarding and it’s power supply must not exceed 3.3V. The TSL2561 also has a second diode specifically for sensing infrared.

Since the TSL2561 is so similar to the TSL230R in theory, I’ll only be writing one condensed article for the TSL2561. Please refer to the series of article of the TSL230R for a more in-depth explanation of how to acquire and process data from these sensors.


Serial Control
TSL2561_DAQ.ino (view online) enables serial control of the TSL2561 via a simple serial protocol between the host computer and Arduino. It allows the user to set the number of output samples, adjust the TSL2561’s sensitivity and integration time, and switch power to a light source. The Arduino IDE has a built in serial monitor, which you can use for testing serial commands. However, Tod E. Kurt’s arduino-serial is smaller and has more functionality.

The command:
./arduino-serial -b 9600 -p /dev/ttyUSB0 -d 3000 -s s016 -d 100 -s i101 -d 100 -s l111 -d 100 -s t005 -d 10000 -r -d 500 -r -d 500 -r -d 500 -r -d 500 -r -d 500 -r -d 100 -s l000

Outputs one read for each -r:
read: 697

read: 697

read: 696

read: 697

read: 696

read: EOT

This command waits three seconds for the bootloader to load the program (-d 3000) then it tells the program to set the sensitivity to 16x (s016), the integration time to 101 ms (i101), turn the light on (l111), and transmit five samples (t005). The command then waits 10 seconds for the buffer to fill (-d 10000), reads five samples (-r -d 500 repeated five times), and finally turns the light off. The blank lines in the output are from the line feed (i.e. \n) printed after each number. The uc code uses Serial.print('\n') instead of Serial.println() and the string “EOT” so that it can communicate with code written for GNU Octave and MATLAB.


Data Acquisition Scripts
The archive contains the m-files (view online: get_data, save_data, serial_open) necessary for controlling the TSL2561 within GNU Octave and MATLAB and reading the counts output from the ATmega uc.


Spectral Responsivity

The spectral responsivity for the Channel 0 diode when the gain is 16x, the integration time is 101 ms, Vdd = 3V, and Ta = 25°C is saved in Re2561.mat in the essential_data_sets folder within the archive


Converting Counts to Irradiance
With Re(λ) and a model of the spectral content of the light source irradiating the photodiode array we can calculate the spectral irradiance and total irradiance of the light source more accurately than in the simplistic case of assuming all the light source’s photons are 640 nm in wavelength.

For example, if we model a red LED with a peak wavelength at 640 nm and a full width at half maximum (FWHM) of 34 nm with MATLAB like so:

   % mathematically model lamp's spectrum as a gaussian curve with a peak 
   % wavelength at 640 nm and full width at half maximum of 34 nm
   e = exp(1);
   func_lamp = @(mu, FWHM) e.^(-2.7726*((lambda_Re-mu)/FWHM).^2);
   X = func_lamp(640, 2*17);  % [uW/(nm*cm^2)]

Then the output counts, cX, that would result if X irradiated the photodiode array can be calculated thusly:


However, cX is not the actual output counts of the TSL2561 because X is only a model of the shape of the light’s spectrum and lacks radiometric calibration. Since we can measure counts, finding the proper radiometric calibration multiplier for X is as simple as dividing counts/cX.


Therefore, a good approximation of the radiometrically calibrated spectral irradiance of the light source should be:


and the total irradiance is:



Newark gave me a TSL2561T light to digital converter from TAOS to evaluate as part of their product road testing program.

Thanks go out to ladyada for providing a library and basic example for working with the TSL2561.


Using a Wii Nunchuk as an Earthquake Sensor May 16, 2012

Filed under: Electronics,QCN — jethomson @ 9:57 pm



This article explores the suitability of a Wii nunchuk based USB accelerometer as an earthquake sensor for the Quake-Catcher Network (QCN) project. It examines the nunchuk over several metrics: precision and range, frequency response, total cost and availability.

The Quake-Catcher Network is a collaborative initiative for developing the world’s largest, low-cost strong-motion seismic network by utilizing sensors in and attached to internet-connected computers. With your help, the Quake-Catcher Network can provide better understanding of earthquakes, give early warning to schools, emergency response systems, and others. The Quake-Catcher Network also provides educational software designed to help teach about earthquakes and earthquake hazards.

Range and Precision
QCN supports a few different USB accelerometers. The most basic one is the JoyWarrior24F8 (JW24F8), which is a 3 axis accelerometer with 10 bits of precision and a measurement range of +-2g, +-4g, or +-8g. QCN uses the +-2g range. According to WiiBrew, the Wii nunchuk’s accelerometer also has 10 bits of precision over a range of +-2g. Therefore, the nunchuk meets the first criteria for evaluating its suitability as a QCN sensor.

Data Comparison
I don’t have access to a shake table so I’m unable to directly evaluate the frequency response of the nunchuk based USB accelerometer. However, QCN did provide me with a JoyWarrior24F8 USB accelerometer for comparison. Since the frequency response of the JoyWarrior24F8 was already deemed suitable by Prof. Cochran for QCN, I simply had to attach the JoyWarrior24F8 and the nunchuk to the same substrate, shake them by hand at various frequencies while recording data from both sensors simultaneously, and compare the Fourier transform of the nunchuk’s data to the transform of the JW24F8’s data.

Here are comparisons of an official (i.e. STMicroelectronics accelerometer) nunchuk to the JW24F8. The microcontroller code used was and the plots were made using the Octave scripts found in the code section below.


Accelerometer X-axis data comparison
Time domain plots:


Frequency domain plots:


Accelerometer Y-axis data comparison
Time domain plots:


Frequency domain plots:


Accelerometer Z-axis data comparison
Time domain plots:


Frequency domain plots


The STMicroelectronics based nunchuk appears to have a response that is very similar to the JW24F8’s response. It should be noted that I was shaking the accelerometers by hand so I don’t think I covered the entire range of frequencies of interest.

Unfortunately, there are fake (i.e. 6331 accelerometers) nunchuks that are unsuitable earthquake sensors because their accelerometer data has stuck bits. Even worse, it can be very difficult to impossible to tell if a nunchuk is official by external examination only.

The nunchuk uses I2C to transfer its data. Therefore, a microcontroller that supports USB and I2C is required to read the data from the nunchuk, filter it, and pass it to the host computer. Three different microcontrollers were evaluated: an ATmega32U2 board that supports hard USB and soft I2C, an ATmega328P with V-USB that supports soft USB and hard I2C, and an ATmega32U4 (teensy) that supports hard USB and hard I2C. The ATmega32U2 only works with 6331 based nunchuks and only at 100 kHz. The ATmega328P works with both STMicroelectronics and 6331 based nunchuks, but the two-wire interface (TWI) eventually locks up for an unknown reason. The ATmega32U4 works with both types of nunchuks tested and with no crashes observed over a two-week period. The STMicroelectronics nunchuk works at 100 and 200 kHz with hard I2C only. The 6331 based nunchuk works at 100, 200, and 400 kHz when hard I2C is used.

A Quake Catcher Kit from Saelig is $42.25 with about $12 for shipping to a U.S. residence, for a total of $54.25.

A Teensy with a 3.3V regulator and shipping costs about $22. A genuine, official nunchuk is approximately $20 shipped. A nunchuk extension cable from eBay is around $4.50. For a total price of $46.50. However, the cost of a proper mount for the nunchuk as well as the labor cost of assembly has not been included. Therefore, I believe that Quake Catcher Kit is most likely a better deal for your time and money.

_Microcontroller code_
The output resulting from microcontroller code that didn’t filter the accelerometer data was the most similar to the output of the JW24F8. Code that filters the accelerometer data with Chebyshev and moving-average filters is included for comparison purposes and because I’d already written it.

This code is for research purposes only; it uses an Atmel USB VID/PID pair for LUFA demos only. This code doesn’t work with QCN because the QCN software checks the joystick’s name to make sure it’s a JoyWarrior. This code can be easily made to work with QCN by modifying its USB descriptors, which I’ve done, but I won’t be releasing this code since it uses Code Mercenaries’s VID/PID. The code also checks the connected controller’s identification bytes to make sure its a genuine Wii nunchuk. It doesn’t work with fake nunchuks.

Wii Nunchuk quake sensor code for teensy (no filter)

Wii Nunchuk quake sensor code for teensy (moving average)

Wii Nunchuk quake sensor code for teensy (chebyshev)

_Host code_
Joystick Accelerometer Data Acquisition code for Linux

Octave plotting scripts