Molecular motor
Molecular motors are natural (biological) or artificial
Examples
Some examples of biologically important molecular motors:[2]
- Cytoskeletal motors
- Myosins are responsible for muscle contraction, intracellular cargo transport, and producing cellular tension.
- anterograde transport.
- retrograde transport.
- Polymerisation motors
- Rotary motors:
- chloroplasts as well as in pumping of protons across the vacuolar membrane.[3]
- The bacterial flagellum responsible for the swimming and tumbling of E. coli and other bacteria acts as a rigid propeller that is powered by a rotary motor. This motor is driven by the flow of protons across a membrane, possibly using a similar mechanism to that found in the Fo motor in ATP synthase.
- Nucleic acid motors:
- RNA polymerase transcribes RNA from a DNA template.[5]
- DNA polymerase turns single-stranded DNA into double-stranded DNA.[6]
- Helicases separate double strands of nucleic acids prior to transcription or replication. ATP is used.
- Topoisomerases reduce supercoiling of DNA in the cell. ATP is used.
- is used.
- SMC proteins responsible for chromosome condensation in eukaryotic cells.[7]
- Viral DNA packaging motors inject viral genomic B-DNA to A-DNAand back again. A-DNA is 23% shorter than B-DNA, and the DNA shrink/expand cycle is coupled to a protein-DNA grip/release cycle to generate the forward motion that propels DNA into the capsid.
- Enzymatic motors: The enzymes below have been shown to diffuse faster in the presence of their catalytic substrates, known as enhanced diffusion. They also have been shown to move directionally in a gradient of their substrates, known as chemotaxis. Their mechanisms of diffusion and chemotaxis are still debated. Possible mechanisms include solutal buoyancy, phoresis or conformational changes leading to change in effective diffusivity[10][11][12] and kinetic asymmetry.[13]
- Catalase
- Urease
- Aldolase
- Hexokinase
- Phosphoglucose isomerase
- Phosphofructokinase
- Glucose Oxidase
A recent study has also shown that certain enzymes, such as Hexokinase and Glucose Oxidase, are aggregating or fragmenting during catalysis. This changes their hydrodynamic size that can affect enhanced diffusion measurements.[14]
- Synthetic molecular motors have been created by chemists that yield rotation, possibly generating torque.[15]
Organelle and vesicle transport
There are two major families of molecular motors that transport organelles throughout the cell. These families include the dynein family and the kinesin family. Both have very different structures from one another and different ways of achieving a similar goal of moving organelles around the cell. These distances, though only few micrometers, are all preplanned out using microtubules.[16]
- Kinesin – These molecular motors always move towards the positive end of the cell
- Uses ATP hydrolysis during the process converting ATP to ADP
- This process consists of ...
- The "foot" of the motor binds using ATP, the "foot" proceeds a step, and then ADP comes off. This repeats itself until the destination has been reached
- This process consists of ...
- The kinesin family consists of a multitude of different motor types
- Kinesin-1 (Conventional)
- Kinesin-2 (Heterotrimeric)
- Kinesin-5(Bipolar)
- Kinesin-13
- Uses ATP hydrolysis during the process converting ATP to ADP
- Dynein – These molecular motors always move towards the negative end of the cell
- Uses ATP hydrolysis during the process converting ATP to ADP
- Unlike kinesin, the dynein is structured in a different way which requires it to have different movement methods.
- One of these methods includes the power stroke, which allows the motor protein to "crawl" along the microtubule to its location.
- The structure of dynein consists of
- A Stem Containing
- A region that binds to dynactin
- Intermediate/light chains that will attach to the dynactin bonding region
- A Head
- A Stalk
- With a domain that will bind to the microtubule
- A Stem Containing
- These molecular motors tend to take the path of the microtubules. This is most likely due to the facts that the microtubules spring forth out of the centrosome and surround the entire volume of the cell. This in turn creates a "Rail system" of the whole cell and paths leading to its organelles.
Theoretical considerations
Part of a series on |
Microbial and microbot movement |
---|
Microswimmers |
Molecular motors |
Because the motor events are stochastic, molecular motors are often modeled with the Fokker–Planck equation or with Monte Carlo methods. These theoretical models are especially useful when treating the molecular motor as a Brownian motor.
Experimental observation
In experimental biophysics, the activity of molecular motors is observed with many different experimental approaches, among them:
- Fluorescent methods: fluorescence resonance energy transfer ().
- Magnetic tweezers can also be useful for analysis of motors that operate on long pieces of DNA.
- Neutron spin echo spectroscopy can be used to observe motion on nanosecond timescales.
- Optical tweezers (not to be confused with molecular tweezers in context) are well-suited for studying molecular motors because of their low spring constants.
- Scattering techniques: single particle tracking based on dark field microscopy or interferometric scattering microscopy(iSCAT)
- Single-molecule electrophysiology can be used to measure the dynamics of individual ion channels.
Many more techniques are also used. As new technologies and methods are developed, it is expected that knowledge of naturally occurring molecular motors will be helpful in constructing synthetic nanoscale motors.
Non-biological
Recently,
Other non-reacting molecules can also behave as motors. This has been demonstrated by using dye molecules that move directionally in gradients of polymer solution through favorable hydrophobic interactions.[19] Another recent study has shown that dye molecules, hard and soft colloidal particles are able to move through gradient of polymer solution through excluded volume effects.[20]
See also
- Brownian motor
- Brownian ratchet
- Cytoskeleton
- Molecular machines
- Molecular mechanics
- Molecular propeller
- Motor proteins
- Nanomotor
- Protein dynamics
- Synthetic molecular motors
References
- S2CID 28061339.
- ^ Nelson P, Radosavljevic M, Bromberg S (2004). Biological physics. Freeman.
- PMID 11158567.
- PMID 25078022.
- PMID 12384568.
- S2CID 26171993.
- S2CID 28364947.
- S2CID 4424168.
- PMID 25486612.
- S2CID 52845451.
- S2CID 229411011.
- PMID 31263753.
- S2CID 249625518.
- S2CID 237507756.
- PMID 17133632.
- ISBN 978-1-4641-8339-3.
- PMID 38396042.
- PMID 26636667.
- PMID 29064685.
- S2CID 195879481.
External links
- MBInfo - Molecular Motor Activity
- MBInfo - Cytoskeleton-dependent MBInfo - Intracellular Transport
- Cymobase - A database for cytoskeletal and motor protein sequence information
- Jonathan Howard (2001), Mechanics of motor proteins and the cytoskeleton. ISBN 9780878933334