Presentation on theme: "Announcements, Agenda Week 3 Reading for today: Ch. 1, 2 in Hibbs, Zucker 2006 Start up your computers – you will need them for some in-class exercises."— Presentation transcript:
Announcements, Agenda Week 3 Reading for today: Ch. 1, 2 in Hibbs, Zucker 2006 Start up your computers – you will need them for some in-class exercises. Open today’s Power point slides and Internet Explorer I.Lecture: Intro to Confocal, optics II.Paper discussion: Zucker 2006 III.TBA: Collect Z- series of Artemia samples IV.Assignment due Jan. 29
TBA times with Dr. Hertzler: Spring 2007 TimeTuesdayWednesdayThursdayFriday 8 9SEMCell BiologyTEMCell Biology 10Group 1OfficeGroup 2 11 Amy, Lauren, Rachel Hours Andrea, Emily, Molly Group 3Lab meeting 2students Becky, Ellen, Katie Group 4 3UCC Amanda, Brittaney, Joe 4Faculty Meeting Seminar
Outline: Understanding Microscopy A.Introduction to Confocal Microscopy 1.Confocal versus conventional (widefield) fluorescence 2.Optical sectioning 3.Imaging modes and applications 4.Advantages, limitations of confocal B.Essential Optics 1.Wave/particle nature of Light 2.Diffraction 3.Numerical aperture 4.Lateral resolution 5.Axial resolution Useful resource: Molecular Expression Microscopy Primer:
Confocal Light Path Confocal means “having the same focus.” Basis of optical sectioning: coherent light emitted by the laser system (excitation source) passes through a pinhole aperture that is situated in a conjugate plane (confocal) with a scanning point on the specimen and a second pinhole aperture positioned in front of the detector (a photomultiplier tube).
Applications Immunolabelling Organelle ID Protein trafficking Locating genes on chromosomes Analysis of molecular mobility Multiple labeling Live cell imaging Transmission imaging Measurement of subcellular functions and ion concentrations
4. Advantages, limitations of confocal microscopy Optical sectioning ability –Can image cells/tissues internally 3D reconstruction –Improved spatial relationships of structures Excellent resolution –Close to theoretical limit of LM: 0.2 μm Improved multiple labeling –Since specific wavelengths of light used by lasers Very high sensitivity –Capable of collecting single fluorescent molecule Easy manipulation and merging of images –Since they are digital Computer controlled –Complex settings can be programmed and recalled. Expensive to buy and maintain. –$250,000 + Difficult to operate. –Fixed material easy, live difficult. Fluorescent tag usually required. –May be bulky or toxic Objects smaller than 0.2 not resolved –Need to use EM. Damaging high intensity laser –Need to minimize exposure, especially in live cells. Digital images are easily mishandled. –Honesty in imaging very important.
B. Basic Optics 1. The nature of light Light behaves as both a particle and a wave. Can bounce (reflect) and bend (diffract or refract) Has wave properties –Amplitude –Wavelength: visible is between nm White light carries all visible wavelengths –Frequency –Direction of travel –Direction of vibration
Relation between Wavelength, Frequency, Energy Blue light 488 nm short wavelength high frequency high energy (2 times the red) Red light 650 nm long wavelength low frequency low energy Photon as a wave packet of energy
Light-Matter Interactions Absorption Reflection Refraction: bending of light as it passes, at an angle, from one material to another Diffraction: bending of light as it passes an edge Fluorescence: spontaneous emission of light after excitation Polarization Dispersion
2. Diffraction: Bending of light as it passes an edge λ < dλ > d See: Microscopy primer, One long continuous wave, unlike light from a lamp or the sun.
Diffraction Pattern from Slit Results from Interference
Java Tutorial: Diffraction Patterns raction/basicdiffraction/index.htmlhttp://micro.magnet.fsu.edu/primer/java/diff raction/basicdiffraction/index.html How does the width of the central maximum vary with the wavelength?
Diffraction Through a Circular Aperture creates an Airy Disk The radius of the Airy disk is the distance r from the center to the first dark ring, given by the resolution equation. Increasing resolution of lens
Resolution and Airy disk patterns
Java Tutorial: Airy Pattern Basics mation/airydiskbasics/index.htmlhttp://micro.magnet.fsu.edu/primer/java/imagefor mation/airydiskbasics/index.html –How does resolution vary with wavelength and numerical aperture? mation/airyna/index.htmlhttp://micro.magnet.fsu.edu/primer/java/imagefor mation/airyna/index.html –What is the effect of higher NA? mation/rayleighdisks/index.htmlhttp://micro.magnet.fsu.edu/primer/java/imagefor mation/rayleighdisks/index.html –What is the Rayleigh criterion?
3. Numerical aperture (NA) NA = n sin where n = refractive index and = the collecting angle. n air = 1.00 and n oil = W.D.
Maximum theoretical NA Maximum collecting angle is 90 o sin 90 o = For dry objective, max. NA = (1.00)(1.00) = 1.0 –In practice, it is –All dry objectives have NA < 1.00 For oil objective, max NA = (1.515)(1.00) = 1.5. –In practice, it is 1.4. –All oil objectives have NA > 1.00
4. Lateral Resolution (XY or r lateral ) The smallest distance two objects can be imaged as two. Depends on wavelength and NA.
Optimal Resolution for LM Visible light ranges from nm Best NA lens is 1.4 Calculate best theoretical resolution using 520 nm emission of fluorescein: (Footnote: for confocal, the resolution equation is slightly better: r lateral = 0.4λ/NA so best resolution is closer to 0.15 μm).
XY under- and over-sampling Optimal zoom settings (for full xy resolution) for 512 X 512 pixel box are given for various lenses on p –You don’t need to operate at these settings unless you want to push the resolution limit. Rules of thumb for 1024 X 1024 box: –60X 1.4 NA: 4X max zoom –40X 0.75 NA: 5X max zoom –20X 0.7 NA: 6X max zoom Zooming higher than this creates empty magnification.
No Zoom 2X Zoom Zooming for maximum XY resolution
Java Tutorial: 3D Airy disk is the Point Spread Function ageformation/depthoffield/index.html This Z step will not resolve the objects in Z axis. This Z step will resolve the objects in Z axis.
5. Axial Resolution (Z or r axial ) Minimum distance between the 3D diffraction patterns of two points along the Z axis that can still be seen as two. Depends on wavelength and NA obj as follows: Rule of thumb: step size = ½ Z resolution. See also and on04.shtml on04.shtml
Ideal step sizes Ideal step size (higher Z resolution, e.g. NA=1.4) Ideal step size (lower Z resolution, e.g. NA=0.7)
Z axis under- and over-sampling Undersampled Too few sections for full Z resolution But: full Z resolution may not be needed. Oversampled: Overlapping sections add no additional information since full Z resolution is realized; just makes a bigger file.
XY and Z resolutions (μm) 10X 0.4 NA 20X 0.7 NA 40X 0.75 NA 60X 1.4 NA r lateral fluorescein 488/ r lateral rhodamine 543/ r axial step fluorescein 488/ r axial step rhodamine 543/
The bottom line on optimal step size The Nyquist Sampling Theorem states that the pixel size should be 2.3X smaller than the resolution limit of the microscope (p. 126). –So 1.4 NA objective with r lateral = 0.2 μm requires xy pixel size of 0.08 μm, optimal zoom of 3.7X at 512 X 512. –Step size should be 3X xy pixel size = 0.24 μm for 1.4 NA objective with r axial = 0.6 μm
Week 3 TBA Assignment (each person): –Collect Z-series of one of your Artemia samples, using the 20X lens and a step size of 1 or 2 um. –Display the sections in tile mode. –Save (as a normal TIFFs) extended focus images in black and white, showing (a) every section of the Z- series, (b) the top 1/3, (c) the middle 1/3, and d) the bottom 1/3. Always include a scale bar on your images. Save in the BIO553 file on the imaging computer. –Turn in a description of your images using the form available on Blackboard.