Molecular motor

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Molecular motors are natural (biological) or artificial molecular machines that are the essential agents of movement in living organisms. In general terms, a motor is a device that consumes energy in one form and converts it into motion or mechanical work; for example, many protein-based molecular motors harness the chemical free energy released by the hydrolysis of ATP in order to perform mechanical work.[1] In terms of energetic efficiency, this type of motor can be superior to currently available man-made motors. One important difference between molecular motors and macroscopic motors is that molecular motors operate in the thermal bath, an environment in which the fluctuations due to thermal noise are significant.

Examples[edit]

Some examples of biologically important molecular motors:[2]

  • Cytoskeletal motors
  • Polymerisation motors
    • Actin polymerization generates forces and can be used for propulsion. ATP is used.
    • Microtubule polymerization using GTP.
    • Dynamin is responsible for the separation of clathrin buds from the plasma membrane. GTP is used.
  • Rotary motors:
    • FoF1-ATP synthase family of proteins convert the chemical energy in ATP to the electrochemical potential energy of a proton gradient across a membrane or the other way around. The catalysis of the chemical reaction and the movement of protons are coupled to each other via the mechanical rotation of parts of the complex. This is involved in ATP synthesis in the mitochondria and 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.
Molecular dynamics simulation of a synthetic molecular motor composed of three molecules in a nanopore (outer diameter 6.7 nm) at 250 K.[4]
  • 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.
    • RSC and SWI/SNF complexes remodel chromatin in eukaryotic cells. ATP is used.
    • SMC proteins responsible for chromosome condensation in eukaryotic cells.[7]
    • Viral DNA packaging motors inject viral genomic DNA into capsids as part of their replication cycle, packing it very tightly.[8] Several models have been put forward to explain how the protein generates the force required to drive the DNA into the capsid; for a review, see [1]. An alternative proposal is that, in contrast with all other biological motors, the force is not generated directly by the protein, but by the DNA itself.[9] In this model, ATP hydrolysis is used to drive protein conformational changes that alternatively dehydrate and rehydrate the DNA, cyclically driving it from B-DNA to A-DNA and 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 local and global thermal effects, phoresis or conformational changes.[10][11][12]
    • Catalase
    • Urease
    • Aldolase
    • Hexokinase
    • Phosphoglucose isomerase
    • Phosphofructokinase
    • Glucose Oxidase
  • Synthetic molecular motors have been created by chemists that yield rotation, possibly generating torque.[citation needed]

Organelle and vesicle transport[edit]

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.[13]

  • 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
    • The kinesin family consists of a multitude of different motor types
  • 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
          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 tern creates a "Rail system" of the whole cell and paths leading to its organelles.

Theoretical considerations[edit]

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[edit]

In experimental biophysics, the activity of molecular motors is observed with many different experimental approaches, among them:

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[edit]

Recently, chemists and those involved in nanotechnology have begun to explore the possibility of creating molecular motors de novo. These synthetic molecular motors currently suffer many limitations that confine their use to the research laboratory. However, many of these limitations may be overcome as our understanding of chemistry and physics at the nanoscale increases. One step toward understanding nanoscale dynamics was made with the study of catalyst diffusion in the Grubb's catalyst system.[14] Other systems like the nanocars, while not technically motors, are also illustrative of recent efforts towards synthetic nanoscale motors.

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.[15] 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.[16]

See also[edit]

References[edit]

  1. ^ Bustamante C, Chemla YR, Forde NR, Izhaky D (2004). "Mechanical processes in biochemistry". Annual Review of Biochemistry. 73: 705–48. doi:10.1146/annurev.biochem.72.121801.161542. PMID 15189157. S2CID 28061339.
  2. ^ Nelson P, Radosavljevic M, Bromberg S (2004). Biological physics. Freeman.
  3. ^ Tsunoda SP, Aggeler R, Yoshida M, Capaldi RA (January 2001). "Rotation of the c subunit oligomer in fully functional F1Fo ATP synthase". Proceedings of the National Academy of Sciences of the United States of America. 98 (3): 898–902. Bibcode:2001PNAS...98..898T. doi:10.1073/pnas.031564198. PMC 14681. PMID 11158567.
  4. ^ Palma CA, Björk J, Rao F, Kühne D, Klappenberger F, Barth JV (August 2014). "Topological dynamics in supramolecular rotors". Nano Letters. 14 (8): 4461–8. Bibcode:2014NanoL..14.4461P. doi:10.1021/nl5014162. PMID 25078022.
  5. ^ Dworkin J, Losick R (October 2002). "Does RNA polymerase help drive chromosome segregation in bacteria?". Proceedings of the National Academy of Sciences of the United States of America. 99 (22): 14089–94. Bibcode:2002PNAS...9914089D. doi:10.1073/pnas.182539899. PMC 137841. PMID 12384568.
  6. ^ Hubscher U, Maga G, Spadari S (2002). "Eukaryotic DNA polymerases". Annual Review of Biochemistry. 71: 133–63. doi:10.1146/annurev.biochem.71.090501.150041. PMID 12045093. S2CID 26171993.
  7. ^ Peterson CL (November 1994). "The SMC family: novel motor proteins for chromosome condensation?". Cell. 79 (3): 389–92. doi:10.1016/0092-8674(94)90247-X. PMID 7954805. S2CID 28364947.
  8. ^ Smith DE, Tans SJ, Smith SB, Grimes S, Anderson DL, Bustamante C (October 2001). "The bacteriophage straight phi29 portal motor can package DNA against a large internal force". Nature. 413 (6857): 748–52. Bibcode:2001Natur.413..748S. doi:10.1038/35099581. PMID 11607035. S2CID 4424168.
  9. ^ Harvey SC (January 2015). "The scrunchworm hypothesis: transitions between A-DNA and B-DNA provide the driving force for genome packaging in double-stranded DNA bacteriophages". Journal of Structural Biology. 189 (1): 1–8. doi:10.1016/j.jsb.2014.11.012. PMC 4357361. PMID 25486612.
  10. ^ Zhao X, Gentile K, Mohajerani F, Sen A (October 2018). "Powering Motion with Enzymes". Accounts of Chemical Research. 51 (10): 2373–2381. doi:10.1021/acs.accounts.8b00286. PMID 30256612.
  11. ^ Ghosh S, Somasundar A, Sen A (2021-03-10). "Enzymes as Active Matter". Annual Review of Condensed Matter Physics. 12 (1): 177–200. doi:10.1146/annurev-conmatphys-061020-053036. S2CID 229411011.
  12. ^ Zhang Y, Hess H (June 2019). "Enhanced Diffusion of Catalytically Active Enzymes". ACS Central Science. 5 (6): 939–948. doi:10.1021/acscentsci.9b00228. PMC 6598160. PMID 31263753.
  13. ^ Lodish H, Berk A, Kaiser CA, Krieger M, Bretscher A, Ploegh H, Amon A, Martin KC (2014). Molecular Cell Biology (8th ed.). New York, NY: w.h.freeman, Macmillan Learning. ISBN 978-1-4641-8339-3.
  14. ^ Dey KK, Pong FY, Breffke J, Pavlick R, Hatzakis E, Pacheco C, Sen A (January 2016). "Dynamic Coupling at the Ångström Scale". Angewandte Chemie. 55 (3): 1113–7. doi:10.1002/ange.201509237. PMID 26636667.
  15. ^ Guha R, Mohajerani F, Collins M, Ghosh S, Sen A, Velegol D (November 2017). "Chemotaxis of Molecular Dyes in Polymer Gradients in Solution". Journal of the American Chemical Society. 139 (44): 15588–15591. doi:10.1021/jacs.7b08783. PMID 29064685.
  16. ^ Collins M, Mohajerani F, Ghosh S, Guha R, Lee TH, Butler PJ, et al. (August 2019). "Nonuniform Crowding Enhances Transport". ACS Nano. 13 (8): 8946–8956. doi:10.1021/acsnano.9b02811. PMID 31291087.

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