User:Brian P. Josey/Notebook/2009/09/01: Difference between revisions

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==Entry title==
==Notes of Papers==
* Larry asked me to look at a paper, "Force production by single kinesin motors" by Schnitzer et. al. He wanted me to find how the authors derive three of the equations, 2,4 and 5. I'm looking at these now.
* Larry asked me to look at a paper, "Force production by single kinesin motors" by Schnitzer et. al. He wanted me to find how the authors derive three of the equations, 2,4 and 5.
*Unfortunately I was unable to resolve this issues for him. I will return to the paper at a later date to see if I can understand it more.
 
However we did discuss the paper that I read last week, "Mechanical Design of Translocating Motor Proteins" by W. Hwang. The paper is a review of how basic motor proteins move in the cell. The authors suggest that we currently know enough about these proteins to create what is essentially a mechanical parts list that are necessary for the proteins to move. They then go on to explain the basic mechanics of how the proteins propagate. While they discuss a wide variety of different proteins, my notes will be limited to the discussion of kinesin due to its relevance to my own work.
 
There are a few key characteristics of the proteins that can be measured. They are:
*Unloaded Velocity- The unloaded velocity is essentially the maximum speed that the protein goes when it does not encounter any obstacles or has a load. This occurs when the load is not present and there are no obsticles in the way of protein. Because there is no load, there is a minimum amount of drag, although there still is some drag from the movement relative to the surrounding medium. For Kinesin-1 the typical unloaded velocity is ~700nm/s.
*Stall Force- The stall force is how much force is need to stop the motor from moving. For Kinesin-1 this typically falls in to the range of 5-7 pN.
*Step Size- The step size is simply how far the protein can go in a single step, which for kinesin is 8 nm, a value that correspond to the size of a tubulin dimer.
*Processivity- Processivity can be thought of as how far the motor can go along its path when unloaded. Kinesin is noted to have a higher processivity compared to other motors. The authors note that a protein that keeps its motor heads out of phase with each other in their steps is prone to have a higher processivity. Also, if proteins work as a group by forming pairs and binding to the same cargo this also increases the processivity. They do not state how this would work, but I figure that it is because one can take over for both if the other disassociates from the track, giving it time to reattach.
*Efficiency- How efficient the motor is is simply the maximum amount of work that can be done divided by the change in free energy. For kinesin, with a stall force of ~6pN and a steop size of 8.2 nm the efficiency is 48-60%
 
From here the authors continue on with a list of mechanical parts that are necessary for the protein to do its function, namely to move along a track while transporting a cargo.
 
Pulled away, I'll finish this later (hopefully this evening)


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Notes of Papers

  • Larry asked me to look at a paper, "Force production by single kinesin motors" by Schnitzer et. al. He wanted me to find how the authors derive three of the equations, 2,4 and 5.
  • Unfortunately I was unable to resolve this issues for him. I will return to the paper at a later date to see if I can understand it more.

However we did discuss the paper that I read last week, "Mechanical Design of Translocating Motor Proteins" by W. Hwang. The paper is a review of how basic motor proteins move in the cell. The authors suggest that we currently know enough about these proteins to create what is essentially a mechanical parts list that are necessary for the proteins to move. They then go on to explain the basic mechanics of how the proteins propagate. While they discuss a wide variety of different proteins, my notes will be limited to the discussion of kinesin due to its relevance to my own work.

There are a few key characteristics of the proteins that can be measured. They are:

  • Unloaded Velocity- The unloaded velocity is essentially the maximum speed that the protein goes when it does not encounter any obstacles or has a load. This occurs when the load is not present and there are no obsticles in the way of protein. Because there is no load, there is a minimum amount of drag, although there still is some drag from the movement relative to the surrounding medium. For Kinesin-1 the typical unloaded velocity is ~700nm/s.
  • Stall Force- The stall force is how much force is need to stop the motor from moving. For Kinesin-1 this typically falls in to the range of 5-7 pN.
  • Step Size- The step size is simply how far the protein can go in a single step, which for kinesin is 8 nm, a value that correspond to the size of a tubulin dimer.
  • Processivity- Processivity can be thought of as how far the motor can go along its path when unloaded. Kinesin is noted to have a higher processivity compared to other motors. The authors note that a protein that keeps its motor heads out of phase with each other in their steps is prone to have a higher processivity. Also, if proteins work as a group by forming pairs and binding to the same cargo this also increases the processivity. They do not state how this would work, but I figure that it is because one can take over for both if the other disassociates from the track, giving it time to reattach.
  • Efficiency- How efficient the motor is is simply the maximum amount of work that can be done divided by the change in free energy. For kinesin, with a stall force of ~6pN and a steop size of 8.2 nm the efficiency is 48-60%

From here the authors continue on with a list of mechanical parts that are necessary for the protein to do its function, namely to move along a track while transporting a cargo.

Pulled away, I'll finish this later (hopefully this evening)