Basics of Inverted Microscope
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Single Pass Cooling Systems
A Sustainable Alternative to Single Pass Cooling Systems Amorette Getty, PhD Co-Director, LabRATS What is Single Pass Cooling? ● Used for distillation/reflux condensers, ice maker condensers, autoclaves, cage washers… ● Use a continuous flow of water from faucet to sewer o 0.25-2 gallons per minute, o up to 1,000,000 gallons of water/year if left on continuously Single Pass Cooling: Support ● “U.S. Environmental Protection Agency has ranked the elimination of single-pass cooling systems #4 on its list of top ten water management techniques” -Steve Buratto, Chair of Chemistry and Biochemistry department NOT Just a Sustainability Issue! California Nanosystems Institute (CNSI) flood in a second-floor laboratory in July, 2014. Water ran at ~1-2 gallons per minute for 6-10 hours, overflowing into a ground floor electron microscopy lab CNSI Flood Losses ● $ 2.2 Million in custom built research equipment ● Research shutdown for 4 months ● over 200 hours of staff time ● Insurance no longer covering this type of incident again Campus Responses to the Incident • CNSI ban on single pass cooling systems • TGIF grant financial incentive for optional change of single replacement systems • Chemistry and Material Research Laboratory (MRL) • Additional Grants being sought • Conversation at Campus and UC-level to regulate and replace these types of systems. Seeking Allies… ● “The replacement of single-pass cooling systems with closed-loop and water free systems would save water and represent a major advance in the sustainability efforts of the campus.” -Steve Buratto, Chair of Chemistry and Biochemistry department Barriers to Replacement ● “...major obstacle to replacing the single-pass cooling systems with closed-loop and water- free systems is cost. -
Two-Photon Excitation, Fluorescence Microscopy, and Quantitative Measurement of Two-Photon Absorption Cross Sections
Portland State University PDXScholar Dissertations and Theses Dissertations and Theses Fall 12-1-2017 Two-Photon Excitation, Fluorescence Microscopy, and Quantitative Measurement of Two-Photon Absorption Cross Sections Fredrick Michael DeArmond Portland State University Let us know how access to this document benefits ouy . Follow this and additional works at: https://pdxscholar.library.pdx.edu/open_access_etds Part of the Physics Commons Recommended Citation DeArmond, Fredrick Michael, "Two-Photon Excitation, Fluorescence Microscopy, and Quantitative Measurement of Two-Photon Absorption Cross Sections" (2017). Dissertations and Theses. Paper 4036. 10.15760/etd.5920 This Dissertation is brought to you for free and open access. It has been accepted for inclusion in Dissertations and Theses by an authorized administrator of PDXScholar. For more information, please contact [email protected]. Two-Photon Excitation, Fluorescence Microscopy, and Quantitative Measurement of Two-Photon Absorption Cross Sections by Fredrick Michael DeArmond A dissertation submitted in partial fulfillment of the requirements for the degree of Doctor of Philosophy in Applied Physics Dissertation Committee: Erik J. Sánchez, Chair Erik Bodegom Ralf Widenhorn Robert Strongin Portland State University 2017 ABSTRACT As optical microscopy techniques continue to improve, most notably the development of super-resolution optical microscopy which garnered the Nobel Prize in Chemistry in 2014, renewed emphasis has been placed on the development and use of fluorescence microscopy techniques. Of particular note is a renewed interest in multiphoton excitation due to a number of inherent properties of the technique including simplified optical filtering, increased sample penetration, and inherently confocal operation. With this renewed interest in multiphoton fluorescence microscopy, comes increased interest in and demand for robust non-linear fluorescent markers, and characterization of the associated tool set. -
Statement by the Association of Hoving Image Archivists (AXIA) To
Statement by the Association of Hoving Image Archivists (AXIA) to the National FTeservation Board, in reference to the Uational Pilm Preservation Act of 1992, submitted by Dr. Jan-Christopher Eorak , h-esident The Association of Moving Image Archivists was founded in November 1991 in New York by representatives of over eighty American and Canadian film and television archives. Previously grouped loosely together in an ad hoc organization, Pilm Archives Advisory Committee/Television Archives Advisory Committee (FAAC/TAAC), it was felt that the field had matured sufficiently to create a national organization to pursue the interests of its constituents. According to the recently drafted by-laws of the Association, AHIA is a non-profit corporation, chartered under the laws of California, to provide a means for cooperation among individuals concerned with the collection, preservation, exhibition and use of moving image materials, whether chemical or electronic. The objectives of the Association are: a.) To provide a regular means of exchanging information, ideas, and assistance in moving image preservation. b.) To take responsible positions on archival matters affecting moving images. c.) To encourage public awareness of and interest in the preservation, and use of film and video as an important educational, historical, and cultural resource. d.) To promote moving image archival activities, especially preservation, through such means as meetings, workshops, publications, and direct assistance. e. To promote professional standards and practices for moving image archival materials. f. To stimulate and facilitate research on archival matters affecting moving images. Given these objectives, the Association applauds the efforts of the National Film Preservation Board, Library of Congress, to hold public hearings on the current state of film prese~ationin 2 the United States, as a necessary step in implementing the National Film Preservation Act of 1992. -
Second Harmonic Imaging Microscopy
170 Microsc Microanal 9(Suppl 2), 2003 DOI: 10.1017/S143192760344066X Copyright 2003 Microscopy Society of America Second Harmonic Imaging Microscopy Leslie M. Loew,* Andrew C. Millard,* Paul J. Campagnola,* William A. Mohler,* and Aaron Lewis‡ * Center for Biomedical Imaging Technology, University of Connecticut Health Center, Farmington, CT 06030-1507 USA ‡ Division of Applied Physics, Hebrew University of Jerusalem, Jerusalem 91904, Israel Second Harmonic Generation (SHG) has been developed in our laboratories as a high- resolution non-linear optical imaging microscopy (“SHIM”) for cellular membranes and intact tissues. SHG is a non-linear process that produces a frequency doubling of the intense laser field impinging on a material with a high second order susceptibility. It shares many of the advantageous features for microscopy of another more established non-linear optical technique: two-photon excited fluorescence (TPEF). Both are capable of optical sectioning to produce 3D images of thick specimens and both result in less photodamage to living tissue than confocal microscopy. SHG is complementary to TPEF in that it uses a different contrast mechanism and is most easily detected in the transmitted light optical path. It also does not arise via photon emission from molecular excited states, as do both 1- and 2-photon excited fluorescence. SHG of intrinsic highly ordered biological structures such as collagen has been known for some time but only recently has the full potential of high resolution 3D SHIM been demonstrated on live cells and tissues. For example, Figure 1 shows SHIM from microtubules in a living organism, C. elegans. The images were obtained from a transgenic nematode that expresses a ß-tubulin-green fluorescent protein fusion and Figure 1 also shows the TPEF image from this molecule for comparison. -
502-13 Magnifiers and Telescopes
13-1 I and Instrumentation Design Optical OPTI-502 © Copyright 2019 John E. Greivenkamp E. John 2019 © Copyright Section 13 Magnifiers and Telescopes 13-2 I and Instrumentation Design Optical OPTI-502 Visual Magnification Greivenkamp E. John 2019 © Copyright All optical systems that are used with the eye are characterized by a visual magnification or a visual magnifying power. While the details of the definitions of this quantity differ from instrument to instrument and for different applications, the underlying principle remains the same: How much bigger does an object appear to be when viewed through the instrument? The size change is measured as the change in angular subtense of the image produced by the instrument compared to the angular subtense of the object. The angular subtense of the object is measured when the object is placed at the optimum viewing condition. 13-3 I and Instrumentation Design Optical OPTI-502 Magnifiers Greivenkamp E. John 2019 © Copyright As an object is brought closer to the eye, the size of the image on the retina increases and the object appears larger. The largest image magnification possible with the unaided eye occurs when the object is placed at the near point of the eye, by convention 250 mm or 10 in from the eye. A magnifier is a single lens that provides an enlarged erect virtual image of a nearby object for visual observation. The object must be placed inside the front focal point of the magnifier. f h uM h F z z s The magnifying power MP is defined as (stop at the eye): Angular size of the image (with lens) MP Angular size of the object at the near point uM MP d NP 250 mm uU 13-4 I and Instrumentation Design Optical OPTI-502 Magnifiers – Magnifying Power Greivenkamp E. -
Lab 11: the Compound Microscope
OPTI 202L - Geometrical and Instrumental Optics Lab 9-1 LAB 9: THE COMPOUND MICROSCOPE The microscope is a widely used optical instrument. In its simplest form, it consists of two lenses Fig. 9.1. An objective forms a real inverted image of an object, which is a finite distance in front of the lens. This image in turn becomes the object for the ocular, or eyepiece. The eyepiece forms the final image which is virtual, and magnified. The overall magnification is the product of the individual magnifications of the objective and the eyepiece. Figure 9.1. Images in a compound microscope. To illustrate the concept, use a 38 mm focal length lens (KPX079) as the objective, and a 50 mm focal length lens (KBX052) as the eyepiece. Set them up on the optical rail and adjust them until you see an inverted and magnified image of an illuminated object. Note the intermediate real image by inserting a piece of paper between the lenses. Q1 ● Can you demonstrate the final image by holding a piece of paper behind the eyepiece? Why or why not? The eyepiece functions as a magnifying glass, or simple magnifier. In effect, your eye looks into the eyepiece, and in turn the eyepiece looks into the optical system--be it a compound microscope, a spotting scope, telescope, or binocular. In all cases, the eyepiece doesn't view an actual object, but rather some intermediate image formed by the "front" part of the optical system. With telescopes, this intermediate image may be real or virtual. With the compound microscope, this intermediate image is real, formed by the objective lens. -
Improving Plastics Management: Trends, Policy Responses, and the Role of International Co-Operation and Trade
Improving Plastics Management: Trends, policy responses, and the role of international co-operation and trade POLICY PERSPECTIVES OECD ENVIRONMENT POLICY PAPER NO. 12 OECD . 3 This Policy Paper comprises the Background Report prepared by the OECD for the G7 Environment, Energy and Oceans Ministers. It provides an overview of current plastics production and use, the environmental impacts that this is generating and identifies the reasons for currently low plastics recycling rates, as well as what can be done about it. Disclaimers This paper is published under the responsibility of the Secretary-General of the OECD. The opinions expressed and the arguments employed herein do not necessarily reflect the official views of OECD member countries. This document and any map included herein are without prejudice to the status of or sovereignty over any territory, to the delimitation of international frontiers and boundaries and to the name of any territory, city or area. For Israel, change is measured between 1997-99 and 2009-11. The statistical data for Israel are supplied by and under the responsibility of the relevant Israeli authorities. The use of such data by the OECD is without prejudice to the status of the Golan Heights, East Jerusalem and Israeli settlements in the West Bank under the terms of international law. Copyright You can copy, download or print OECD content for your own use, and you can include excerpts from OECD publications, databases and multimedia products in your own documents, presentations, blogs, websites and teaching materials, provided that suitable acknowledgment of OECD as source and copyright owner is given. -
Handheld Microscope Users Guide
Handheld Microscope Users Guide www.ScopeCurriculum.com ii Handheld Microscope Users Guide Hand-Held Microscope User’s Guide Table of Contents INTRODUCTION ..................................................................................................................................1 What is a Scope-On-A-Rope? .....................................................................................................1 Which model do you have?.........................................................................................................2 Analog vs. Digital .........................................................................................................................3 Where can I buy a SOAR? ...........................................................................................................3 NEW SCOPE-ON-A-ROPE..................................................................................................................4 Parts and Assembly of SOAR .....................................................................................................4 Connections .................................................................................................................................5 Turning It On.................................................................................................................................5 Comparing and Installing Lenses...............................................................................................6 How to Use and Capture Images with the 30X Lens.................................................................7 -
Subwavelength Resolution Fourier Ptychography with Hemispherical Digital Condensers
Subwavelength resolution Fourier ptychography with hemispherical digital condensers AN PAN,1,2 YAN ZHANG,1,2 KAI WEN,1,3 MAOSEN LI,4 MEILING ZHOU,1,2 JUNWEI MIN,1 MING LEI,1 AND BAOLI YAO1,* 1State Key Laboratory of Transient Optics and Photonics, Xi’an Institute of Optics and Precision Mechanics, Chinese Academy of Sciences, Xi’an 710119, China 2University of Chinese Academy of Sciences, Beijing 100049, China 3College of Physics and Information Technology, Shaanxi Normal University, Xi’an 710071, China 4Xidian University, Xi’an 710071, China *[email protected] Abstract: Fourier ptychography (FP) is a promising computational imaging technique that overcomes the physical space-bandwidth product (SBP) limit of a conventional microscope by applying angular diversity illuminations. However, to date, the effective imaging numerical aperture (NA) achievable with a commercial LED board is still limited to the range of 0.3−0.7 with a 4×/0.1NA objective due to the constraint of planar geometry with weak illumination brightness and attenuated signal-to-noise ratio (SNR). Thus the highest achievable half-pitch resolution is usually constrained between 500−1000 nm, which cannot fulfill some needs of high-resolution biomedical imaging applications. Although it is possible to improve the resolution by using a higher magnification objective with larger NA instead of enlarging the illumination NA, the SBP is suppressed to some extent, making the FP technique less appealing, since the reduction of field-of-view (FOV) is much larger than the improvement of resolution in this FP platform. Herein, in this paper, we initially present a subwavelength resolution Fourier ptychography (SRFP) platform with a hemispherical digital condenser to provide high-angle programmable plane-wave illuminations of 0.95NA, attaining a 4×/0.1NA objective with the final effective imaging performance of 1.05NA at a half-pitch resolution of 244 nm with a wavelength of 465 nm across a wide FOV of 14.60 mm2, corresponding to an SBP of 245 megapixels. -
Depth of Focus (DOF)
Erect Image Depth of Focus (DOF) unit: mm Also known as ‘depth of field’, this is the distance (measured in the An image in which the orientations of left, right, top, bottom and direction of the optical axis) between the two planes which define the moving directions are the same as those of a workpiece on the limits of acceptable image sharpness when the microscope is focused workstage. PG on an object. As the numerical aperture (NA) increases, the depth of 46 focus becomes shallower, as shown by the expression below: λ DOF = λ = 0.55µm is often used as the reference wavelength 2·(NA)2 Field number (FN), real field of view, and monitor display magnification unit: mm Example: For an M Plan Apo 100X lens (NA = 0.7) The depth of focus of this objective is The observation range of the sample surface is determined by the diameter of the eyepiece’s field stop. The value of this diameter in 0.55µm = 0.6µm 2 x 0.72 millimeters is called the field number (FN). In contrast, the real field of view is the range on the workpiece surface when actually magnified and observed with the objective lens. Bright-field Illumination and Dark-field Illumination The real field of view can be calculated with the following formula: In brightfield illumination a full cone of light is focused by the objective on the specimen surface. This is the normal mode of viewing with an (1) The range of the workpiece that can be observed with the optical microscope. With darkfield illumination, the inner area of the microscope (diameter) light cone is blocked so that the surface is only illuminated by light FN of eyepiece Real field of view = from an oblique angle. -
22 Bull. Hist. Chem. 8 (1990)
22 Bull. Hist. Chem. 8 (1990) 15 nntn Cn r fr l 4 0 tllOt f th r h npntd nrpt ltd n th brr f th trl St f nnlvn n thr prt nd ntn ntl 1 At 1791 1 frn 7 p 17 AS nntn t h 3 At 179 brr Cpn f hldlph 8Gztt f th Untd Stt Wdnd 3 l 1793 h ntr nnnnt rprdd n W Ml "njn h Cht"Ch 1953 37-77 h pn pr dtd 1 l 179 nd nd b Gr Whntn th frt ptnt d n th Untd Stt S M ntr h rt US tnt" Ar rt Invnt hn 199 6(2 1- 19 ttrfld ttr fnjn h Arn hl- phl St l rntn 1951 pp 7 9 20h drl Gztt 1793 (20 Sptbr Qtd n Ml rfrn 1 1 W Ml rfrn 1 pp 7-75 William D. Williams is Professor of Chemistry at Harding r brt tr University, Searcy, Al? 72143. He collects and studies early American chemistry texts. Wyndham D. Miles. 24 Walker their British cultural heritage. To do this, they turned to the Avenue, Gaithersburg, MD 20877, is winner of the 1971 schools (3). This might explain why the Virginia assembly Dexter Award and is currently in the process of completing the took time in May, 1780 - during a period when their highest second volume of his biographical dictionary. "American priority was the threat of British invasion following the fall of Chemists and Chemical Engineers". Charleston - to charter the establishment of Transylvania Seminary, which would serve as a spearhead of learning in the wilderness (1). -
Introduction to Light Microscopy
Introduction to light microscopy A CAMDU training course Claire Mitchell, Imaging specialist, L1.01, 08-10-2018 Contents 1.Introduction to light microscopy 2.Different types of microscope 3.Fluorescence techniques 4.Acquiring quantitative microscopy data 1. Introduction to light microscopy 1.1 Light and its properties 1.2 A simple microscope 1.3 The resolution limit 1.1 Light and its properties 1.1.1 What is light? An electromagnetic wave A massless particle AND γ commons.wikimedia.org/wiki/File:EM-Wave.gif www.particlezoo.net 1.1.2 Properties of waves Light waves are transverse waves – they oscillate orthogonally to the direction of propagation Important properties of light: wavelength, frequency, speed, amplitude, phase, polarisation upload.wikimedia.org 1.1.3 The electromagnetic spectrum 퐸푝ℎ표푡표푛 = ℎν 푐 = λν 퐸푝ℎ표푡표푛 = photon energy ℎ = Planck’s constant ν = frequency 푐 = speed of light λ = wavelength pion.cz/en/article/electromagnetic-spectrum 1.1.4 Refraction Light bends when it encounters a change in refractive index e.g. air to glass www.thetastesf.com files.askiitians.com hyperphysics.phy-astr.gsu.edu/hbase/Sound/imgsou/refr.gif 1.1.5 Diffraction Light waves spread out when they encounter an aperture. electron6.phys.utk.edu/light/1/Diffraction.htm The smaller the aperture, the larger the spread of light. 1.1.6 Interference When waves overlap, they add together in a process called interference. peak + peak = 2 x peak constructive trough + trough = 2 x trough peak + trough = 0 destructive www.acs.psu.edu/drussell/demos/superposition/superposition.html 1.2 A simple microscope 1.2.1 Using lenses for refraction 1 1 1 푣 = + 푚 = physicsclassroom.com 푓 푢 푣 푢 cdn.education.com/files/ Light bends as it encounters each air/glass interface of a lens.