The
Biological Physics Training Laboratory
Contacts
Projects
Biophysical
forces and Laser tweezing Electrophysiology
Biological
Pattern Formation
Biological
Fluid Dynamics
Biology,
Mathematics and Physics Initiative
For further information contact
Applied Mathematics (520-621-2016)
|
The University of Arizona
Biological Physics Teaching Laboratory
Biophysical
Forces
Optical Tweezing and Kinesin Motility
Kinesin is a molecular motor that
converts the energy derived from adenosine triphosphate (ATP) hydrolysis into
mechanical work and moves along polymeric tubes of the protein tubulin. These
tubes, called microtubules, are found in virtually all eucaryotic cells and provide
lines of transport and communication between different levels in the cell. Thus
kinesin functions as an intracellular transport vehicle, binding to organelles
or supply vesicles and carrying them down microtubules to all parts of the cell.
While the details of how chemical energy stored in ATP is released as mechanical
energy in kinesin stepping remain unknown, it is clear that kinesin hydrolyses
one ATP molecule for each 8 nm step forward. In this module, students investigate
kinesin velocity, measured in steps taken per second, as a function of ATP concentration.
| | An image captured by differential
interference contrast (DIC) microscopy, shows a small glass bead (diameter ~1
um) which is being carried by Kinesin molecular motor(s) along polymeric tubes
of the protein tubulin (the thin strands). | Although
the kinesin motor is far too small to be observed with standard microscopy techniques,
the activity of kinesin motors is still possible to observe thanks to the fact
that the kinesin tail binds well to materials like glass. Individual, or collections
of motors, can be made to carry a small glass bead (diameter ~1 um) which can
be easily observed using differential interference contrast (DIC) microscopy (right).
Knowledge of the techniques of laser tweezing, microtubule polymerization and
the preparation of a kinesin motility assay are required before measurements commence.
Data are captured onto VHS tape via CCD camera from DIC microscopy observations.
The frame-by-frame position of transported beads is analyzed with computer software.
Brownian motion, Stokes flow, and Activated processes
Thermal fluctuations are ubiquitous
at the cellular level and below, yet it is rare for students in the biological
sciences to see quantitative treatments of their effects. Likewise, physicists
and mathematicians interested in the biological world often study stochastic phenomena
in the abstract, with no true sense of their significance. The goal of this core
experimental module is to use the techniques of video microscopy and optical trapping
to quantify several phenomena associated with Brownian motion.
 |
| A small latex bead (diameter ~1 um) is shown at high magnification.Brownian
motion affects the bead position over time. | A
first goal is to learn the principles of optical trapping "laser tweezers", used
also in other experiments, and calibrate traps of varying intensity through Stokes
drag on latex beads of varying sizes (left). The fluctuations of those beads
in the trap will be compared with theoretical calculations using the basic principles
of statistical mechanics. Observations of Brownian motion in the absence of a
trap will be used to determine Avogadro's number from the universal gas constant,
along the lines of the original Einstein work on Perrin's results. Fluids of different
viscosities and particles of different sizes will be used to check
the
| | This collection of optical components (mirrors,
lenses, and beamsplitters) is used to split an infrared laser beam into to components
of with orthogonal polarization, to control the position of the two beams, and
to recombine them before they are focused by the microscope objective at the sample
plane. The result is two steerable optical traps which can capture and manipulate
microscopic objects. | Stokes-Einstein
relation (fluctuation-dissipation theorem). Finally, a double trap has been constructed
(right) to examine Kramers' theory, which attempts to characterize a chemical
reaction by the rate at which a Brownian particle can move over the energy barrier
of a one-dimensional double-well potential. Experimentally, such a potential is
readily obtained by using two optical traps positioned closely together.
By video-recording the images a glass
particle (~500 nm in diameter) jumping from one optical trap into the other, and
subsequent Particle tracking (below left) using a dedicated image-processing computer,
the transition rate can be determined, and Kramers' results can be experimentally
verified.
| | A collection of data points that are samples
of the position of a microsphere over time that hops back and forth between two
nearby optical traps of approximately equal depth. | |