Organelles are positioned within the cell by motor proteins moving along microtubules.
Microtubules have distinct ends: plus ends and minus ends.
Examples of organelles include the ER and Golgi apparatus.
Kinesins and dynein are motor proteins involved in organelle movement.
Axoplasm is an extract system that supports motor-based motility, similar to what occurs in a living giant axon.
Experiments involve in vitro studies using giant squid axons.
Shinya Inoue's lab at MBL in Woods Hole utilized video-enhanced DIC (Differential Interference Contrast) microscopy to study these processes.
Illustrations show the propagation of an action potential along an axon.
Sodium (Na+) channels open and close during depolarization and repolarization of the membrane.
Adding AMP-PNP to axoplasm freezes vesicles on microtubules, halting movement.
This indicates that microtubules are the filaments along which organelles move in both directions.
The gliding assay involves organelle, bead, and microtubule translocations promoted by soluble factors from the squid giant axon.
Figure 1: Illustrates experimental conditions:
(a) Purified microtubules (MTs).
(b) Axoplasm (S2) extract.
(c) Control: MTs + ATP release (no AMP-PNP).
(d) MTs + AMP-PNP followed by ATP release.
(e) MT pellets - AMP-PNP.
(f) MT Pellets + AMP-PNP Axoplasm Extracts.
The process involves taking eluted material, diluting it to lower ATP concentration, and rebinding it to MTs +/- AMP-PNP.
Elution is performed again using salt + ATP.
Chromatography columns are used in the purification process.
Gel filtration separates proteins by size.
SDS-PAGE is used to analyze the composition of each fraction.
The translocator activity corresponds to the ~110 kDa band.
The hydroxyapatite column is an ion exchange column that separates proteins based on their charge.
Images of purified kinesins and their motor domains are shown.
Kinesin walks along microtubules in a hand-over-hand fashion.
Step 1: HEAD 1 (ADP) binds to the microtubule (MT).
Step 2: HEAD 1 releases ADP.
Step 3: HEAD 1 binds ATP, causing the neck linker to zip up and swing HEAD 2 into position.
Step 4: HEAD 1 hydrolyzes ATP and releases Pi (now HEAD 1 is bound to ADP).
This process repeats with HEAD 2.
Coupling conformational changes in the “neck linker” domain to its ATPase cycle allows kinesin to directionally walk along microtubules.
Laser tweezers are used to study kinesin motility.
Optical traps work by focusing a laser beam to create a potential well that can trap particles with a different refractive index than the surrounding solution.
Light is refracted by the bead, and due to the law of conservation of momentum, forces pull the bead into the center of the laser.
Hooke’s Law: Force = kx, where k is the spring constant and x is the distance.
Changes in laser light are measured to detect extremely small changes in x (sub-nanometer).
Forces that can be measured with an optical trap range from 0.1 pN to 100 pN.
Kymographs are used to visualize kinesin motility.
Motors move directionally along microtubules, and microtubule polarity is important.
Gaussian analysis of a diffraction-limited spot allows defining the “centroid”.
By fitting a 2D-Gaussian to the signal, the centroid can be defined with ~1-3nm accuracy if the signal is high enough above background.
Purified kinesin can be made to glow for single-molecule imaging.
FIONA (Fluorescence Imaging with One Nanometer Accuracy) is a technique used.
8 nm steps can be imaged at 50 msec.
Retrograde transport of cargo in axons is mediated by dynein.
Bidirectional transport of organelles and beads on MTs in axoplasm is observed.
Dynein activity is required for retrograde transport of beads on MTs in axoplasm.
A comparison between dynein and kinesin is made.
In many organisms, dynein motility requires its association with the dynactin complex via adaptors.
Quantification of dynein heavy chain stoichiometry reveals double dynein complexes (Urnavicius et al., Nature 2018).
In vitro, the mean velocity is 1.2 mm/s.
Optical trapping is used to study dynein-dynactin interactions.
Each blip upwards represents a distance of ~8 nm.
Step size analysis is performed for kinesin and dynein.
The structure of tubulin is shown, with α-tubulin and β-tubulin subunits.
The size of the tubulin dimer indicated. 8 nm.
Atomic Force Microscopy (AFM) is used to study molecular structures.
Hooke’s Law: F = kx, where k is the spring constant of the cantilever arm and x is the distance the arm moved.
AFM tips can be “functionalized” with antibodies, streptavidin, biotin, etc.
AFM can be used to pull on single molecules.
AFM can be used to scan surfaces coated with molecules to visualize them, including motors like Myosin II on actin filaments.