TB4: Microscopy Flashcards
What is an image?
A matrix of numbers
Brightfield microscopy uses
Commonly used in a wide variety of laboratory applications as the standard microscope; produces an image on a bright background.
Darkfield microscopy uses
Increases contrast without staining by producing a bright image on a darker background; especially useful for viewing live specimens.
Phase contrast microscopy uses
Uses refraction and interference caused by structures in the specimen to create high-contrast, high-resolution images without staining, making it useful for viewing live specimens, and structures such as endospores and organelles.
Fluorescence microscopy uses
Uses fluorescent stains to produce an image; can be used to identify pathogens, to find species, to distinguish living from dead cells, or to find locations of molecules within a cell; also used for immunofluorescence.
Confocal microscopy uses
Uses a laser to scan multiple z-planes successively, producing numerous 2D, high resolution images at various depths that can be constructed into 3D images by a computer, making this useful for examining thick specimens such as biofilms.
Widefield vs Confocal
- widefield lights up the entire sample whilst confocal has a pinhole
- confocal has scan mirrors
- widefield is quicker but can’t do optical sectioning
Experimental Considerations for Microscopy
- living samples need environmental controls
- always do confocal before super-resolution
- widefield microscope when studying dynamics
- thin or thick sample
- laser lines and filter sets
Rayleigh Criterion (equation)
θ = 1.22 x λ(m)/diameter(m)
Abbe Equation
r = λ/2NA (numerical aperature)
Focal Point
When a beam is transmitted through a lens, all the rays entering parallel will converge to a single spot called the focal point which resides on the focal plane.
Snell’s law
sin(incident angle)/sin(refractive angle)=n (refractive index)
Chromatic aberration
Caused by different wavelengths passing through a lens as each of these will have a different refractive index, and thus have differing focal points.
Spherical aberration
Occur even when there’s only one wavelength passing through, stemming from the fact that spheres of lenses aren’t perfect and so won’t focus the light to a perfect point. This isn’t as bad as chromatic aberrations.
Objective lens
Located closest to the object, this relays the real image of the object to the eyepiece. It’s needed to produce the base magnification.
Eyepiece lens
Located closest to the eye/sensor, projects and magnifies the real image and yields a virtual image of the object.
Brightfield illumination
Backlit illumination where incident light floods the object with light from behind. It uses two lenses (collector and condenser) to provide bright and even illumination on the object plane and image plane. This ensures the user doesn’t image the filament from the light bulb.
Airy Rings
Lenses don’t form perfect images of points of light due to waves having 3D dimensions. They instead distort the images in 3D to form airy rings. The out of focus light from this reduces contrast and resolution.
Rayleigh Resolution Limit
‘The separation where the central maximum of the Airy pattern of one point is directly overlapping with the first minimum of the Airy pattern of another’. Gives a rough idea of the resolution limit. It’s dependent on the wavelength and angle of the light.
Full-Width-Half-Maximum
If you know the wavelength and aperture of a lens, you can use FWHM to determine the resolution limit. The thinner the peak, the better the SNR you can achieve.
Abbe’s Resolution
A simplified view on resolution: high frequencies correspond to small structures which diffract light further than larger structures.
Point Spread Function
The spread of the Airy rings in a diffraction pattern.
Deconvolution
Reassignment of out-of-focus information to increase contrast and resolution.
FISH (fluorescence in situ hybridization)
Fluorescent probes bind to only particular parts of a nucleic acid sequence with a high degree of sequence complementarity.