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Announcements - Tape sensor

Matheus improves the design

posted Feb 10, 2014, 8:36 PM by Tiberius Brastaviceanu   [ updated Feb 24, 2014, 2:09 PM ]


Presentation

YouTube Video



Documentation


Experimental data

Gap Optimization - Matheus



Rodrigo's R&D report on the low-cost tape transducer

posted Aug 28, 2013, 1:41 PM by Tiberius Brastaviceanu   [ updated Aug 28, 2013, 1:41 PM ]

Rodrigo's report on the low-cost tape transducer


New low-cost tape sensor 3D printed

posted Aug 9, 2013, 12:08 PM by Tiberius Brastaviceanu   [ updated Aug 30, 2013, 12:43 PM ]


First attempt 

Today Daniel printed the first thing using our new B9Creator. The low-cost tape sensor had the honor to go in first. We are now tuning the printer for better resolution. 


3 prototypes just out of the printer

3D model of this tape sensor on 3D printed device open model

One prototype after cleaning. 

Preparation and calibration of the 3D printer

Further notes

This first design had some problems. See Rodrigo's below.
 

Comparison between the Low-Cost Tape sensor and the Flex sensor

posted Jul 16, 2013, 4:35 PM by Tiberius Brastaviceanu   [ updated Aug 6, 2013, 11:51 AM ]




We are doing this comparison directly on a hockey stick, in order to make this data directly available to the Hockey Stick project.

Open doc to edit

Low cost Tape Sensor measures our piezo actuator

posted Jun 15, 2013, 8:10 PM by Sensorica Group   [ updated Jun 15, 2013, 8:11 PM by Tiberius Brastaviceanu ]



 low cost tape sensor
 piezo driver and stack
 piezo stack


The low cost Tape Transducer was fixed along the piezo stack, which was activated using our new driver. The graph below shows the signal from the tape transducer driven by the piezo. We started with a sin wave and ended with a triangular wave. The entire measurement took 20 seconds. 


We tried higher frequencies, but above 3 Hz the kapton tape used to fabricate the tape transducer, which takes time to relax from its stretched state, doesn't follow anymore. 

We didn't measure the total displacement of the piezo, but it was driven at max voltage, which, if everything was OK, would give 50um motion amplitude. The only thing we can say with certainty is that the amplitude of the motion recorded with the help of the tape transducer was max 50 microns. 

Why is this so exciting? Because we could test something we built with another thing we also built!!!! 

In terms of our business strategy, you can now see how these different devices we build combine together into more complex systems. This is in fact the first expression of the touch-sensitive and self-"aware" robots for micromanipulation, combining an actuator and a displacement sensor. 

Low cost tape sensor demonstrated and presented

posted Jun 11, 2013, 1:00 PM by Tiberius Brastaviceanu   [ updated Jun 17, 2013, 11:44 AM ]




The low-cost tape sensor





Beam deflection sensor built and tested

posted Apr 27, 2013, 11:54 PM by Sensorica Group   [ updated Apr 27, 2013, 11:56 PM by Tiberius Brastaviceanu ]

On 26th of April we finished the assembly of the first beam deflection optical sensor. Tibi worked on the photonics and the optomechanical assembly. Jonathan supplied the electronics. Ivan and Daniel also helped with the understanding of how it actually works. 
 

The night before the demo, Tibi, Ivan and Daniel tested the prototype.

YouTube Video


This prototype uses the Optical Design - Tape sensor one in (glass) 3 out (PMMA).

Optical Design - Tape sensor one in ‎(glass)‎ 3 out ‎(PMMA)‎


As you can see in the video above, we used an aluminum tube as the main structure of the beam. The fibers were placed into a grove made on a wooden rod, which was about the same diameter as the inner diameter of the aluminum tube. Glue was pored into the grove to keep the fibers in place. For lever we used an 2mm OD, 10cm long acrylic rod, which we coated with silver on a tip. The tip was polished with 1 micron paper before coating. For joint we used a transparent polymer tube. The gap was set at around 150 microns. The tip of the smaller glass fiber was rounded using a modified fiber splicer, in order to reduce the exit cone of the light from the fiber. A high power red LED was used to power the device. The wood rod with the fiber assembly was introduced within the aluminum tube.
Open main document for optomechanical assembly and electronics.



The fiber assembly was first tested using a gimbal, see video below.

YouTube Video


We assumed that once assembled into a aluminum beam, the sensor will behave very similarly to the bench test using the gimbal, in which the mirror rotates around a point on its surface, facing the laser emitting fiber. In reality, the prototype was assembled with the fibers off axis, i.e. not in the center of the beam. They were placed into a grove made on the surface of the wooden rod. When the beam is bent, the fibers are stretched or compressed, if they find themselves within the bending plane. When stretched, the mirror get's away from the fibers. When compressed, the mirror get's closer to the fibers. This induces an intensity variation that is greater than what is produced by the small tilt of the mirror. The signal is dominated by this compression/stretching mode. We were not able to extract 2D spatial information from the device, but we can easily detect bending in the plane containing the optical fibers.

Photo album

Tape sensor prototype and demo



Characterization and optimization tests

posted Apr 11, 2013, 1:13 PM by Tiberius Brastaviceanu   [ updated Apr 11, 2013, 2:01 PM ]

Enrique used the setup made by Tibi to characterize and optimize the tape transducer and recorded the first comprehensive data. 
The main goal of this experiment was to find the optimal size of the gap (distance between the mirror and the fibers).
The one in 3 out prototype with round glass fiber tip was used. The setup consisted of a green laser coupled to the 125/62.5 MM glass fiber (the in fiber) using a lens. The fiber was hold in place using the reusable ST connector. The
one in 3 out prototype (fiber assembly) was prepared by Tibi before the experiment: PMMA fibers were polished and the glass fiber tip was cleaned with alcohol. The tip of the fiber on the side of laser was freshly cleaved. 

Setup used during this experiment
Setup built by Tibi and Enrique for calibration and characterization.

Acquiring data
Program made by Tibi and used by Enrique for characterization and optimization.


Preliminary data obtained

Chart 4


We are looking for a linear relation between angle (mirror tilt) and gap size. The preliminary data shows that being too far from, or too close to the mirror is not good. There is a sweet spot somewhere in the middle. Open the spreadsheet used for characterization and optimization of the tape transducer. Next week we'll continue exploring this same prototype and evaluate its sensitivity. Tibi needs to modify the LabView program in order to allow faster acquisition and better statistics


Live demos of the Tape sensor

posted Feb 6, 2013, 12:16 PM by Sensorica Group   [ updated Mar 19, 2013, 12:01 PM by Tiberius Brastaviceanu ]

Today we made some progress on the Tape sensor. We made and tested two prototypes: the 4 fibers all 1mm PMMA fiber, and the 4 fiber one glass 125/62.5 MM delivery and 3 PMMA 1mm collectors 


Test of the 4 fibers all PMMA - 0.1 degrees resolution

First, we built and tested the all 1mm PMMA transducer: one fiber in and 3 fibers out. The resolution test was done  at around 800 microns gap. The device was feed by a red LED. We measured signal steps induced by 0.1 angle degree variations. The acquisition rate was slow in this experiment, only 1kHz. Moreover, 100 points are digitally averaged to reduce noise. The video below shows the results. The signal plotted was intensity of one fiber minus intensity of another fiber. The test was performed on a single axis.


a stereo microscope was used for visualization and optical alignment
experimental setup using mirror on gimbal

The operation of the transducer was simulated using a flat mirror on a gimbal, which is positioned on a XY manual stage.

fiber assembly in front of the mirror
experimental setup using mirror on gimbal
 

Test of the 4 fibers, one glass 3 PMMA - 0.02 degrees resolution

Two versions were made, one with the glass fiber having a flat tip, like in the first picture below, and the other one using a glass fiber with round tip, made by melting, see second picture below.

first version, flat tip glass fiber version


second version, round tip

In both cases a green laser was used. The picture below shows, from left to right,  the laser, a lens, and the fiber.

one 62.5 glass fiber in and three 1mm PMMA fibers out - laser and optics for coupling

In both cases, a flat mirror on a gimbal was used to simulate the operation of the device. The gimbal was placed on a XY stage.

one 62.5 glass fiber in and three 1mm PMMA fibers out and the gimbal

The the case of the flat tip version the results obtained were only sightly better than in the case of the 4 fibers all PMMA prototype. We also noticed that the light coming out of the glass fiber was not very gaussian, almost resembles a flat top, with a lot of speckles.
We moves right a way to the second version, with the round tip, since the results were not encouraging.

The advantage of the round tip is that it makes the exit cone of the glass fiber smaller, and increases the sensitivity of the device. This was confirmed by observing the light out of the round tip of the fiber using a white piece of paper. We used a fiber splicer modified by Jonathan to process the tip of the fiber.

on the computer screen, the 125 micron diameter glass fiber
between the two electrodes, waiting to get zapped
zapped fiber on the sceen

fiber getting zapped on the same screen, you can see the plasma
between the two electrodes. this plasma melts the glass
fiber being zapped on the screen

the kind of shapes we can get, a much smaller sphere was created
in the case of the fiber used in the tested device, see picture above
125 micron D 62.5 MM glass fiber with ball formed on tip


The video below shows the results obtained. Angle steps of 0.02 degrees were made while the signal was recorded. The signal plotted was intensity of one fiber minus intensity of another fiber. The test was performed on a single axis.  We can clearly see that we have a resolution of at least 0.02 degrees. This can be greatly improved by doing some signal conditioning on the electronic board.

YouTube Video




Making and testing the 1 in 3 out all PMMA design

posted Jan 25, 2013, 7:44 PM by Sensorica Group   [ updated Jan 25, 2013, 7:50 PM by Tiberius Brastaviceanu ]

Jonathan
improved the electronic circuit for the tape sensor, adding variable gains (third version, see more on this evolving circuit prototype). This is a huge improvement!

Tibi assembled the 1 in, 3 out all PMMA design, connected it to the electronics and tested it with a mirror to see if there is sign of signal crossing, which is an indication that we can map small deflections in 2D. The screenshot below shows signal crossings for small angle variations of the mirror, placed 1mm away from the tip of the fibers.

3 signals from the 1 in 3 out all PMMA design, showing signal crossings


A video was also made to demonstrate this prototype. Next step is to assemble everything into a single wire, including the mirror on a lever, and test it on a 1m long beam. In order to optimize the sensitivity we'll keep the gap variable.



The making of this prototype

7 fibers were put together like in this picture
All 1mm PMMA fiber bundle

Since we only use 3 outer fibers to collect light, the other 3 were pushed back a little, in order to glue the remaining 4. 
assembly of the 7 PMMA fibers, after gluing

The remaining 4 fibers were polished
assembly to polish the 4 PMMA fibers at once

And tested shining light through them.
The 4 PMMA fibers - this pic is for assessing the symetry of the assembly. Light was whined into the fibers from the other side.

In order to ease the connections with the LED and PS a plastic tube was put over the tip of all fibers. The end results looks like this. The red one is the hot fiber, i.e. the one that brings light into the sensing area. The other 3 black ones are collecting fibers.
PMMA fibers, left is the polished end, where the miccor is going to be, on the right are the individual fibers with plastic tube over them, coming from an electrical wire. The red is the hot one, the one that brings light into the sensitive area. The black ones are the ones that bring light back to the 3 detectors.

Everything was connected to the electronics and tested.
3-th version of the electronic circuit made by Jonathan, with variable gain
the entire system, testing the 1 in 3 out all PMMA device
1 in 3 out all PMMA device - fibers in front of mirror








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