Progress and New Results from the H-1NF Scanning Interferometer Scott Collis, George Warr, John...

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Progress and New Results from the H-1NF Scanning Interferometer Scott Collis, George Warr, John Howard
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Page 1: Progress and New Results from the H-1NF Scanning Interferometer Scott Collis, George Warr, John Howard.

Progress and New Results from the H-1NF Scanning

InterferometerScott Collis, George Warr,

John Howard

Page 2: Progress and New Results from the H-1NF Scanning Interferometer Scott Collis, George Warr, John Howard.

A Time Multiplexed Interferometer

• The System is basically described as two Michelson Interferometers with a time varying viewing path viewing

• The phase shift induced by the plasma is given by

• The signal is time multiplexed, which means we only need one detector per probe beam

dlnλr2Δφ ec

Page 3: Progress and New Results from the H-1NF Scanning Interferometer Scott Collis, George Warr, John Howard.
Page 4: Progress and New Results from the H-1NF Scanning Interferometer Scott Collis, George Warr, John Howard.

Beams are swept by a grating wheel

• Wheel speed can be varied from 0-6000rpm

• At 6000 rpm with a 6 partitioned wheel one scan of the plasma takes 1.8ms

• The wheel also Doppler shifts the beam:

dmRf /

Page 5: Progress and New Results from the H-1NF Scanning Interferometer Scott Collis, George Warr, John Howard.

Motor and Grating

Page 6: Progress and New Results from the H-1NF Scanning Interferometer Scott Collis, George Warr, John Howard.

Continuous Grating allows viewing of small structures

• The grating constant changes linearly across a sector

• Possibility of seeing small structures, of order 1cm (beam size) such as islands and transport barriers

• Data can aliased when frequency of plasma oscillations approaches the scan frequency of the interferometer

Page 7: Progress and New Results from the H-1NF Scanning Interferometer Scott Collis, George Warr, John Howard.

Fosc > Fscan

Page 8: Progress and New Results from the H-1NF Scanning Interferometer Scott Collis, George Warr, John Howard.

Aliased Data

Page 9: Progress and New Results from the H-1NF Scanning Interferometer Scott Collis, George Warr, John Howard.

Calibration

•We need a transform from temporal position in scan

to spatial position in the H-1NF tank

Page 10: Progress and New Results from the H-1NF Scanning Interferometer Scott Collis, George Warr, John Howard.

A 2.5cm absorber was placed at three positions on the bottom

mirror

Page 11: Progress and New Results from the H-1NF Scanning Interferometer Scott Collis, George Warr, John Howard.

At 40cm above the centre

Page 12: Progress and New Results from the H-1NF Scanning Interferometer Scott Collis, George Warr, John Howard.

In the centre of the mirror

Page 13: Progress and New Results from the H-1NF Scanning Interferometer Scott Collis, George Warr, John Howard.

And at 40cm below the centre

Page 14: Progress and New Results from the H-1NF Scanning Interferometer Scott Collis, George Warr, John Howard.

Top Diagonal Results

Beam width: 1.3cm

Page 15: Progress and New Results from the H-1NF Scanning Interferometer Scott Collis, George Warr, John Howard.

Bottom Diagonal Results

Beam width: 3.2cm

Page 16: Progress and New Results from the H-1NF Scanning Interferometer Scott Collis, George Warr, John Howard.

Calculated Beam Positions

Page 17: Progress and New Results from the H-1NF Scanning Interferometer Scott Collis, George Warr, John Howard.

High Density ICRH Shot

•Fundamental ICRH resonance of Hydrogen

•B=0.5T

•Peaked density profile

•Highest B2ne product observed in H-1NF

Page 18: Progress and New Results from the H-1NF Scanning Interferometer Scott Collis, George Warr, John Howard.

Possibilities

• With the wheel running at high speed it is possible to get temporally and spatially resolved information on the plasma decay

• From this it will be possible to solve the two dimensional diffusion equation

• With the new ICRH mode it is possible to study the physics of fully ionized plasmas in H-1NF

Page 19: Progress and New Results from the H-1NF Scanning Interferometer Scott Collis, George Warr, John Howard.

But first….

• To tomographically reconstruct density maps of the H-1NF plasma we need a greater coverage of the plasma

• We will be expanding the fan of the diagonal views and installing a central view

Page 20: Progress and New Results from the H-1NF Scanning Interferometer Scott Collis, George Warr, John Howard.

Using the interferometer to understand particle transport

• Using a gas puffer it is possible to modulate the source term in the continuity equation

• By modulating the gas flow and using the high temporal and spatial resolution of the interferometer it is possible to gain an insight into how particle transport occurs in H-1NF

• Information can be combined with other instruments to gain not only ne but Te Ti and ion velocity

Page 21: Progress and New Results from the H-1NF Scanning Interferometer Scott Collis, George Warr, John Howard.

Conclusion

• The H-1NF Scanning interferometer can make spatially and temporally resolved measurements of the plasma with resolutions of up to 1cm and 1.8ms

• As the system is upgraded the data it produces will provide physical insight into the behavior of flexible Heliac plasmas