Here you'll see what we were able to measure with our own device, as well as how to build your own, low-priced iRIf device.

Result of the binding of rabbit/anti-rabbit measured in our own device. A: The first picture of the measurement. B: The last picture of the measurement. C: The quotient picture of first and last picture. D: Schematic illustration of the spots on the slide

For testing our device we bound proteins derived from rabbits onto an iRIf slide in distinct spots (Fig 1 D). The proteins used were polyclonal anti-HCV (hepatitis C virus) antibodies, which we then aimed to detect with anti-rabbit antibodies. The reason for using the rabbit/anti-rabbit couple in this series of experiments was to reproduce a successful measurement with this binding couple which we previously performed in our regular measuring device. The binding layer on the iRIf slide consisted of an APTES/PDITC surface. The spots on the slide were made by pipetting 3 µl (500 µg/ml) rabbit-anti-HCV protein and 3 µl (1 mg/ml) BSA in an alternating pattern onto the slide. After incubation, the slide was blocked for 30 min in BSA solution. A Canon 50D camera was used to record the measurement and was set to take one picture every 5 seconds. The exposure time was set so that the pixels in the image were approx. 80% of maximum light saturation before the solution was flown onto the chip. The antibody solution was pipetted into the flow-chamber without the use of any microfluidics device. Instead a syringe was loaded with 500 µl [5 µg/ml] anti-rabbit antibody solution (diluted in PBS) and slowly released into the binding chamber of the device by gently dispensing the solution from the syringe. As can be seen in the figure C, the quotient picture clearly showed binding of anti-rabbit to the rabbit protein spots. The BSA control-spots showed none or negligible unspecific binding.

An illustration showing the exact setup of our device from a top perspective

As can be seen in the illustration below, the basic setup is fairly simple. Light from an LED enters a lense where the light rays are made parallel. To achieve this, the distance from LED to the lense has to be exactly one focal length. The light then hits the iRIf slide, where it gets reflected (reflecting at the same angle it hit the slide) and enters a second lense, whose purpose is to project a sharp image of the slide onto the CCD chip of the camera.