Methods: Single-Molecule Techniques Biochemistry 4000 Dr. Ute Kothe.

Slides:



Advertisements
Similar presentations
D e t e c t o r s f o r H P L C.
Advertisements

Surface Plasmon Resonance Biosensors
1 Outline Basic Idea Simple Theory Design Points Calibration of Forces Selected Biological Applications.
Limits and Interfaces in Sciences / Kumboldt-Kolleg São Paulo-SP,
Fluorophores bound to the specimen surface and those in the surrounding medium exist in an equilibrium state. When these molecules are excited and detected.
Single Molecule Studies of DNA Mechanics with Optical Tweezers Mustafa Yorulmaz Koç University, Material Science and Engineering.
New TURF for TIRF Joel Schwartz Stowers Institute for Medical Research Imaging Center.
Optical Tweezers F scatt F grad 1. Velocity autocorrelation function from the Langevin model kinetic property property of equilibrium fluctuations For.
Methods: Fluorescence Biochemistry 4000 Dr. Ute Kothe.
Lecture 8: Measurement of Nanoscale forces II. What did we cover in the last lecture? The spring constant of an AFM cantilever is determined by its material.
Lecture 2 Single-Molecule Methods. Advantages of single-molecule experiments Observe heterogeneity: static (differences between molecules) dynamic (history.
Methods: Cryo-Electron Microscopy Biochemistry 4000 Dr. Ute Kothe.
OPTICAL FIBER WAVEGUIDE Optical Fiber Waveguides An Optical Fiber is a dielectric waveguide that operates at optical frequencies Normally cylindrical.
In practice, optical tweezers are very expensive, custom-built instruments. These instruments usually start with a commercial optical microscope.
P. Moghe, 125:583 1 Microscopy Techniques for Biomaterials and Cell Based Interfaces Professor Prabhas V. Moghe October 26, :583 Fall 2006.
Methods: Protein-Protein Interactions
Microscopy Techniques for Biomaterial Characterization: A Primer Prabhas V. Moghe Lecture 3 September 21, 1999 RU CBE 533 or BME 553; NJIT BME 698.
Physics 1502: Lecture 29 Today’s Agenda Announcements: –Midterm 2: Monday Nov. 16 … –Homework 08: due Friday Optics –Index of Refraction.
Optical Tweezers + DNA Stretching Lecture Notes stored at: Then select the “Lecture” button. David Carberry,
Study of Protein Association by Fluorescence-based Methods Kristin Michalski UWM RET Intern In association with Professor Vali Raicu.
FUTURE APPLICATION OF LASER. OPTICAL TWEEZER An optical tweezer uses a focused laser beam to provide an attractive or repulsive force depending on the.
Fluorescence Microscopy Chelsea Aitken Peter Aspinall.
1© Manhattan Press (H.K.) Ltd. Reflection Refraction Refraction 12.1 Reflection and refraction Total internal reflection Total internal reflection.
Time out—states and transitions Spectroscopy—transitions between energy states of a molecule excited by absorption or emission of a photon h =  E = E.
4-1 Chap. 7 (Optical Instruments), Chap. 8 (Optical Atomic Spectroscopy) General design of optical instruments Sources of radiation Selection of wavelength.
“Nanophotonics and Optical Control of Single Nanoparticles” Keonwoo Nam Moscow 2012 Supervisor: Professor A. A. Fedyanin Lomonosov Moscow State University,
An Introductory Information about Optical Tweezers Mustafa Yorulmaz Koç University, Material Science and Engineering.
Fluorescence Spectroscopy 1Dr. Nikhat Siddiqi. Principles Interaction of photons with molecules results in promotion of valence electrons from ground.
Cameras Course web page: vision.cis.udel.edu/cv March 22, 2003  Lecture 16.
TIRF Total Internal Reflection Fluorescence Microscopy specialized fluorescence microscopy technique specifically images a very thin optical section (50-250nm)
Total Internal reflection Fluorescence Microscopy: Instrumentation and Applications in Cell biology.
Single molecule pull-down Jain et al, Nature 473:484 (2011) Main points to cover fluorescence TIRF microscopy main advantage evanescent field depth single-fluor.
Refraction is the change of direction of a light wave caused by a change in speed as the wave crosses a boundary between materials.
RamanRaman. Scattering Tyndall scattering – if small particles are present During Rayleigh scattering (interaction of light with relatively small molecules)
Lecture 7: Fluorescence: Polarization and FRET Bioc 5085 March 31, 2014.
Properties of Light / EM waves Polarization Why is that? In many cases light is radiated/scattered by oscillating electric dipoles. + – Intensity lobe.
Surface Plasmon Resonance (SPR)
Epi-illumination is form of Kohler Illumination:
Single Molecule Spectroscopy (SMS) 2010/6/9 Miyasaka Lab. Iida Atsushi.
IPC Friedrich-Schiller-Universität Jena 1 ASP_MP_S2j Biophotonics Prof. Dr. Rainer Heintzmann Institut für Physikalische Chemie Friedrich-Schiller-Universität.
Single Molecule: Detection and Manipulation Ilan Tsafrir Tamar Arzi Physics of Complex Systems - Weizmann Institute of Science Interaction Between Membranes.
IPC Friedrich-Schiller-Universität Jena 1 ASP_MP_S2j Biophotonics Prof. Dr. Rainer Heintzmann Institut für Physikalische Chemie Friedrich-Schiller-Universität.
Today’s take-home lessons (i.e. what you should be able to answer at end of lecture) FRET – why it’s useful, R -6 dependence; R 0 (3-7 nm), very convenient.
Today’s Announcements 1.Next Tuesday: Diffusion (Why moving in a cell is like swimming in concrete.) 2. Homework assigned today Last graded Homework:
Förster Resonance Energy Transfer (FRET)
Ch 10 Pages ; Lecture 24 – Introduction to Spectroscopy.
Designing a Microscopy Experiment Kurt Thorn, PhD Director, Image from Susanne Rafelski, Marshall lab.
Dr R.Jayaprada CONFOCAL MICROSCOPY.
Date of download: 6/22/2016 Copyright © 2016 SPIE. All rights reserved. Index-matching effect. Matching the index of refraction of the bead with the solution.
Light & Optics. Electromagnetic Waves Electromagnetic waves include: light, radio, microwaves, x-rays, gamma rays, ultra-violet, and infrared radiation.
Evanescent wave induced Time-resolved Fluorescence
Date of download: 7/8/2016 Copyright © 2016 SPIE. All rights reserved. Through-the-objective TIRF creates the evanescent field on the aqueous side of the.
Introduction to Light Stolen from Florin Albeanu 2016/07/19.
Solutions of Schrodinger Equation
Interference of Light Waves
Optics Kathy Geise April 2007
Comparison of Unitary Displacements and Forces Between 2 Cardiac Myosin Isoforms by the Optical Trap Technique by Seiryo Sugiura, Naoshi Kobayakawa, Hideo.
Light scattering method Introduction: The illumination of dust particles is an illustration of light scattering, not of reflection. Reflection is the deviation.
Single Tapered Fibre “Optical Tweezers”
Selected Measurements
Today’s take-home lessons: FRET (i. e
New Turf for CFP/YFP FRET Imaging of Membrane Signaling Molecules
Interference of Light Waves
LIGHT MICROSCOPY variations
New Turf for CFP/YFP FRET Imaging of Membrane Signaling Molecules
REMOTE SENSING.
FLUORESCENCE MICROSCOPY
Volume 104, Issue 1, Pages (January 2013)
Marco Capitanio, Francesco S. Pavone  Biophysical Journal 
PLASMONICS AND ITS APPLICATIONS BY RENJITH MATHEW ROY. From classical fountations to its modern applications
Presentation transcript:

Methods: Single-Molecule Techniques Biochemistry 4000 Dr. Ute Kothe

Why single-molecule detection? Hairpin Ribozyme Standard ensemble measurements provide only an average of the measured property. Single-molecule measurements reveal subpopulations with different properties.

Signal-to-Noise Ratio Raman Scatter from Water: Inelastic scattering of light at longer wavelength Overlaps with light emitted by fluorophore  Use dyes with high quantum yield  Measure 1 dye molecule in a small volume of solvent (1fl = l)

Total Internal Reflection Above a certain angle, the light is totally internally reflected at an interface with low refractive index. But the incident beam can still interact with the sample at the interface because the intensity penetrates a short distance into the sample = evanescent field in limited volume. Illumination through Prism

Confocal Detection Pinhole allows observation of light only from the focal point, thus reducing the observed volume.

Example: G protein activation Intracellular Single Molecule: YFP = yellow fluorescent protein Visualization of RAs activation, i.e. of GTP binding to Ras Using FRET between YFP And Bodipy-GTP

Example: k on, k off measurement Histogram of off & on time durations

Optical Tweezers A bead is hold in place by an optical trap (see below) Bead is linked to biomolecule Biomolecule is also linked to coverslip Movement of coverslip relative to optical trap generates force on biomolecule  Force or distance can be measured Optical trap Streptavidin-coated microsphere Example: Linear rate of transcription by RNA-Pol. measured in distance/nt per time under constant force: Note random pauses!

Principle of optical trap Intense beam of light (laser) is focussed into a very small region Intense electromagnetic field will “capture” a small dielectric sphere Intensity of light influence the force exerted on the bead if displaced from center

Example 1: measuring force A feedback circuit, based on microscopic observation of the bead position, increases the laser power to keep the bead fixed as the force increases (and vice versa).  While the distance is increased (x axis), the force exerted on the microsphere is measured (y axis). Stretching of a single chromatin fiber of whích one end is linked to the coverslip and the other end is linked to the microsphere

Example 2: fun Tying a knot in an actin fiber, using optical tweezers.