Posts by Danny de Gans

Wave Maker Hits The Water For The First Time

The first tests with the flap type wave maker are looking good. Today the electronic control loop was tuned and the setup was placed in water for the first time. The flap is actuated by a voice coil and its position is measured by an LVDT. The position controller accepts an analog setpoint signal which is generated by a function generator with arbitrary wave form possibility. This makes it very easy to create special waves.

Affordable and Low Field MRI

MRI scanners are very expensive machines that cost about 1M€/T, and a typical MRI scanner has a static magnetic field of 3 to 7T. Because of this many people in the world have no access to it. LUMC and TU Delft have worked together to develop an affordable MRI scanner. The project was made open source so it’s even possible to build your own, and quite a few copies have been built around the world.

The main way the costs were lowered is by using permanent magnets for the main field and use cheap computing power to compensate for that. The magnet was designed at the LUMC and the mathematics and gradient coils at TU Delft EWI.

DEMO has designed and built a RF Power Amplifier, Gradient Amplifier, Low Noise Amplifier, Software Defined Radio and a Halbach Magnet.

Proton Beam Intensity Profile Measurement

This instrument is designed to measure the penetration depth of a proton beam in a water tank. Many protons will deposit their energy at the Bragg peak which can be located with this instrument. It can move a detector through the water and simultaneously measure a reference chamber outside the tank for the incoming proton beam and the sensor in the water tank.

The instrument synchronously measures the detector currents between 3.4pA and +/-800nA at a rate of 1kS/s in a single range with 98fA precision. After digital filtering the current noise floor is reduced even further. Charge is integrated at 1MS/s with a resolution of 6.25fC. The initial offset correction can be set with the same 98fA precision to minimize the integrated charge drift. The required bias voltage for the ion chambers can be set in a range of +/-400V at 1V steps or precisely at 0V when a synthetic diamond diode detector is connected. The user can manually move the sensor with the keypad or perform an automated measurement sequence from a computer.

First proton beam intensity measurement with the setup
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