APh161 - Lecture 13: Molecular Motors Rob Phillips California Institute of Technology.

Slides:



Advertisements
Similar presentations
Lecture 6 Biomotors Self assembling rotary motors.
Advertisements

MotorMax ForceMax SpeedMax Power ROTARY ROTARY Flagellar motor (8 units, E. coli) 2400 pN nm 95 pN 300 Hz 35  m/s 2000 pN 150 Hz 1.9 x 10 6 pN nm.
Modeling Dynein: The Gear-Shifting Motor Manoranjan Singh, Roop Mallik, Steve Gross, and Clare Yu University of California, Irvine step.
How does kinesin walk? Chuang Wu Molecular Biophysics III Thursday 19 Jan
Biophysics Master Course, Fall 2002 Some of the physics cells have to deal with: Random walks, diffusion and Brownian motion.
How Does Intracellular Molecular- Motor-Driven Transport Work? Joseph Snider 2, Frank Lin 2, Neda Zahedi 3, Vladimir Rodionov 3, Clare Yu 2 and Steve Gross.
Chapter 16 The Cytoskeleton.
Moyes and Schulte Chapter 6 Copyright © 2005 Pearson Education, Inc., publishing as Benjamin Cummings Cellular Movement and Muscles.
CYTOSKELETON 1. SIGNIFICANCE OF CYTOSKELETON IN MEDICINE Example: Cytoskeletal structure: mitotic spindle (microtubules) * Cancer diseases therapy: taxanes.
Force and Velocity Measured for Single Molecules of RNA Polymerase Michelle D. Wang, Mark J. Schnitzer, Hong Yin, Robert Landick, Jeff Gelles, Steven M.
Lecture 10: Diffusive Dynamics Rob Phillips California Institute of Technology Verkman et al.
(and intermediate filaments)
APh161 - Lecture 2: The Rate of Things Rob Phillips California Institute of Technology.
Bio 178 Lecture 9 Cell Structure Copyright: E.G. Platzer.
Cell Motility Lecture 17. Cell Motility Includes: –Changes in Cell Location –Limited Movements of Parts of Cells Occurs at the Subcellular, Cellular,
APh161 - Lecture 11: The Cytoskeleton is Always Under Construction Rob Phillips California Institute of Technology Mullins et al.
Lecture 1 Rob Phillips California Institute of Technology (Block et al.) (Wuite et al.)
Molecular Motors Lecture 33`BSCI 420/421Nov 18, 2002 “To survive the 21 st century, our thinking must be creative and humane as well as analytical.” -
Microtubule motors Text and image sources are included using the notes function of this file.
APh161 - Lecture 2: The Rate of Things Rob Phillips California Institute of Technology (Pollard and Earnshaw)
Copyright (c) by W. H. Freeman and Company Chapter 18 Cell Motility and Shape I: Microfilaments.
Inside the Cell 7.1 What’s Inside the Cell? Prokaryotic Cells Eukaryotic Cells –The Nucleus –Ribosomes –Rough Endoplasmic Reticulum –Golgi Apparatus –Smooth.
APh161 - Lecture 15: Molecular Motors Rob Phillips California Institute of Technology.
Announcements HW: Due Tuesday Oct 27 th. Start looking at an article to do your write-up on. Best article is from Nature, Science, Cell. (though can.
Chapter 4 Cytoskeleton. You Must Know The structure and function of the cytoskeleton. Organelles found only in plant cells or only in animal cells. (Page.
Summary of single-molecule experiments Motor proteins:  Are uni-directional, and move along straight filaments  Exert 1-6 pN force  Typically go ~ 1.
Anatoly B. Kolomeisky UNDERSTANDING MECHANOCHEMICAL COUPLING IN KINESINS USING FIRST-PASSAGE PROCESSES.
Molecular motors Biological molecular machines that are the essential agents of movement in living organisms wiki.
Pages Molecular Motors. General Characteristics of Molecular Motors Motor proteins – bind to a polarized cytoskeletal filament and use the energy.
List different movements/motion that occur inside an organism Session I – How things move inside a cell 2/7/14.
Chemical-Mechano Free-Energy Transduction: From Muscles to Kinesin Motors and Brownian Ratchets IPAM workshop IV: Molecular Machines. May 23-28, 2004 Yi-der.
The Molecular Motor Myosin
CHAPTER 9 The Cytoskeleton and Cell Motility. Introduction The cytoskeleton is a network of filamentous structures: microtubulues, microfilaments, and.
Day 35 Announcements Please remove tests, etc. from your folders. Friday, April 6: Microtubules and microfilaments, pp (quiz material),
Kinesin hydrolyses one ATP per 8-nm step Mark J. Schnitzer*† & Steven M. Block†‡ Departments of * Physics and † Molecular Biology, and ‡ Princeton Materials.
Molecular Motors Jean V Bellissard Georgia Institute of Technology School of Physics Fall 2015.
Motor Proteins. One-state model with unequal forward and backward rates.
Ron Rock University of Chicago The Role of the Proximal Tail in the Large Steps of Myosin VI.
Cell Motility Lecture 24 BSCI 420/421Nov 21, 2002 “ A university is a group of faculty and student entrepreneurs, united by a common opposition to parking.
The Eukaryotic Cytoskeleton Oct 9 and 11 Organizing compartments, and a whole lot more!
LECTURE 6 THE CELL – CH. 3 PART 1. A Cell has 3 Major Parts Plasma membrane – Selectively permeable – Intercellular communication Nucleus - the largest.
The Cytoskeleton الهيكل الخلوي
QUATERNARY STRUCTURES AND COMPLEX
By Jennifer Raymond April 14, 2004
APh161 - Lecture 13: Molecular Motors
F1-ATPase: A Rotary Motor Made of a Single Molecule
Continued…….. Cell Organelles
Motor Force Homeostasis in Skeletal Muscle Contraction
Volume 115, Issue 4, Pages (November 2003)
Torque Generation by the Fo motor of the Sodium ATPase
Lecture 24 Tubulin and Microtubule dynamics.
Continued…….. Cell Organelles
Volume 96, Issue 3, Pages (February 2009)
On the Origin of Kinesin Limping
Sean X. Sun, Hongyun Wang, George Oster  Biophysical Journal 
General Animal Biology
Volume 101, Issue 2, Pages (July 2011)
Megan T. Valentine, Steven M. Block  Biophysical Journal 
Stefan Lakämper, Edgar Meyhöfer  Biophysical Journal 
Qiaochu Li, Stephen J. King, Ajay Gopinathan, Jing Xu 
Geometric Asymmetry Induces Upper Limit of Mitotic Spindle Size
Volume 79, Issue 2, Pages (August 2000)
Mechanism of Force Generation of a Viral DNA Packaging Motor
Volume 90, Issue 8, Pages (April 2006)
A Chemically Reversible Brownian Motor: Application to Kinesin and Ncd
Continuous Allosteric Regulation of a Viral Packaging Motor by a Sensor that Detects the Density and Conformation of Packaged DNA  Zachary T. Berndsen,
Continued…….. Cell Organelles
Volume 111, Issue 6, Pages (September 2016)
Mechanical Coupling between Myosin Molecules Causes Differences between Ensemble and Single-Molecule Measurements  Sam Walcott, David M. Warshaw, Edward P.
Volume 99, Issue 9, Pages (November 2010)
Presentation transcript:

APh161 - Lecture 13: Molecular Motors Rob Phillips California Institute of Technology

Mitotic Spindle Organization Cilia and Flagella Assembly and Dynamics Formation of Golgi and ER Networks Vesicle Transport Molecular Motors

Rogues Gallery of Motor Action: Rotary Motors Show Berg movie Show Yasuda et al. movie

Rogues Gallery of Motor Action: Translocation

Rogues Gallery of Motor Action: Translational Motor 1

Rogues Gallery of Motor Action: Translational Motor 2 - Muscles See Hugh Huxley review on website

Rogues Gallery of Motor Action: Translational Motor 2 - Muscles Heuser lab – Washington University

Organellar Transport (Hirokawa, Science 1998)

Rogues Gallery of Motor Action: Translational Motor 2

Myosin V Speed: 350 nm/s ATPase: 5.0 1/s Kinesin Speed: 850 nm/s ATPase: /s Dynein Speed: nm/s ATPase: 2.0 1/s **ALL INVOLVED IN VESICLE TRANSPORT** Translational Motors

How We Know: Gliding Motility Assays Show Vale movie

Dynamics of Molecular Motors Science, Vol 300, Issue 5628, , 27 June Yildiz et al. Show Gelles, Selvin movie

Stepping Kinetics Spudich et al., PNAS 2000

Kinesin Data Fig. 3. Kinesin velocity as a function of [ATP] under external loads, F, fixed by a force clamp. The plots, from the top down, are for F = 0, 1.05, 3.59, 4.60, and 5.63 pN, respectively. Data from Block and colleagues (9): solid curves, N = 2 fits; dashed curves, N = 2 predictions (see text) (Fisher and Kolomeisky, PNAS)

Kinesin Data continued Fig. 4. Fits to the data of Block and colleagues (9) (and predictions) for velocity as a function of load for fixed concentrations of ATP. Note the inflection points at low [ATP] and convex profile at saturating [ATP]. (Fisher and Kolomeisky, PNAS)

Kinesin Randomness Data Fig. 5. Randomness data from Block and colleagues (9) and theoretical fits (A) as a function of external load, F, at fixed [ATP] (note that the two data points at F 5.7 pN and [ATP] = 2 mM appear separately in Block and coworkers: see figure 4 a and b of ref. 9, respectively) and (B) as a function of [ATP] at fixed loads of, from top down, F = 5.69 pN ( ), 5.35 and 4.60 pN (dashed-line predictions), 3.59 pN ( ), and 1.05 pN ( ).

What do we mean by the states?