Spring 2011:Optical Trapping Lab

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20.309: Biological Instrumentation and Measurement

ImageBar 774.jpg

Team FTS

Huayu & Cory

XY position detector calibration

check to see the direction of scan (X)
check to see the direction of scan (Y)
Xcal - volt Vs. position center slope = -3.457
Ycal - volt Vs. position center slope = m = -7.816

Roll Off

Power of laser 10mW, Calculated stiffness =9.28E-6 N/m = .00926 pN/nm

Stoke

StokeTeamFTS.png

Equipartition

for 10 mW : 2.09*10^-9 N/m

Team Humble

XY position detector calibration

Xcallibration.jpg

Trap stiffness by equipartition theorem

Method1 stiffness.jpg

These values are off by about 8 orders of magnitude. This graph is up temporarily until I figure out what is going wrong with my calculations.

Trap stiffness by PSD rolloff

Method2 stiffness.jpg

These values are about 2 orders of magnitude larger than those found in the OTKB document.

Trap stiffness by Stokes' theorem

Method3 stiffness.jpg

These values are about the correct order of magnitude, but the slope of the graph should be positive, not negative! Again, this graph is up temporarily until I can figure out what data processing mistakes are going on.

Team Watson (?)

XY position detector calibration

Sens x.jpg Sens y.jpg

Although the Y axis plot looks OK, I'm not sure of what happened to the X axis one

Trap stiffness by equipartition theorem

Eq x.jpg Eq y.jpg

The X-axis plot follows the expected trend of higher stiffness with higher power, but the Y axis has a very off-line measurement, although the orders of magnitude seem right.

Trap stiffness by PSD rolloff

PSD x.jpg PSD y.jpg

Both of these plots are right around the expected value, although they are around twice the values found for the Equipartition method (maybe there are some conversion errors).

Trap stiffness by Stokes' theorem

Stokes x.jpg Stokes y.jpg

Finally, this method seems to follow the expected trend, but its values are around an order of magnitude off from the previous methods. Again, this may be due to unit conversion issues (currently revising).

Team Watson (Emmanuel)

XY position detector calibration

QPD eq.jpg

  • QPD_XY[V/um] = 3.38e-4 * Power[mW] + 1.6e-3
  • QPD_YX[V/um] = 4.60e-4 * Power[mW] + 8.5e-3

Trap stiffness by equipartition theorem

Equipart eq.jpg

  • Equipart_stiff for X axis: kg/s^2 = 4.57e-16 * Power[mW] + 5.14e-16
  • Equipart_stiff for Y axis: kg/s^2 = 3.37e-16 * Power[mW] + 3.85e-16

Trap stiffness by PSD rolloff

PSD.jpg

  • PSD roll-off stiff for X axis: kg/s^2 = 1.8e-15 * Power[mW] - 51.6e-15
  • PSD roll-off stiff for Y axis: kg/s^2 = 1.9e-15 * Power[mW] - 60.6e-15

Trap stiffness by Stokes' theorem

Team with Brian, Siv, Gustavo

The following analysis is done with data collected by "Team Watson" unless noted otherwise.


Power Spectral Density roll-off

Here, we use the free bead, fixed stage data from "Team GustavSiv".

Note that the corner frequency is approaching the Nyquist frequency and is thus occluded for higher laser intensities
Trap stiffness by PSD roll-off method. The super-linear trend is almost definitely attributed to the error in estimating the corner frequency for high laser intensities.

QPD Responsivity

To perform the next methods, it is necessary to calibrate the QPD.

Stuck bead fit x 10mW.png

Time-series waveform. The star indicates the selected subset to fit.

The procedure depicted in the above graphs is repeated for each measurement, in each of the x and y axes.

Don't be alarmed by the negative slope. The magnitude is positive!

Equipartition Method

Equipartition methodGG.png The equipartion method gives results which are off by several orders of magnitude from the expected trap stiffness.

Navier-Stokes Drag Method

Better news here.

The stage is swept back and forth and the amount of displacement of a free (as in not adhered to the cover slip, but trapped by the laser) bead is plotted over stage velocity.

Navstok x 30mW.png

The best fit line to the data gives a measure of trap stiffness. If the trap were very stiff, then the particle would move very little while the fluid moves around it.

The procedure depicted above is repeated for several laser intensities and for each stage direction.

Navier stoke drag methodGG.png

The point at 70mW unfortunately breaks the expected linear trend.