1. Bioimaging ChemEng 590B: Lecture 15 4/11/13

2. Rat mammary carcinoma cells 10 min, images every 20 seconds Michele Balsamo, Gertler lab MIT 1. Imaging Cells in Culture

3. Quantifying Cell Migration: Live Microscopy White light Incubator: physiological conditions camera Objectives (magnification) Not shown Fluorescent light

4. Magnification of signal This is actually not how a modern LM is built

5. The origin of the resolution problem Light propagates as a wave f f Superposition (addition) of incoming wave fronts

6. In Phase Out of Phase Constructive interference Increased amplitude (brightness) Destructive interference Decreased amplitude (brightness) Superposition of waves

7. A (good) lens is built to produce constructive interference in the main image point Huygens’ principle (wave theory)

8. Z Image of a Point Source of Light – The Point Spread Function (PSF) Objective Airy disk XY

9. The opening of the cone of rays captured by a lens defines the width of the main lobe of the PSF This “opening” is the numerical aperature

10. NA = n x sin(angle) n = refractive index of medium between lens & specimen Image from www.microscopyu.com Definition of the Numerical Aperture (NA) NA is defined for every objective. NA increases with increasing magnification

11. d Resolution: a measure of how close two point images can come such that they are perceived as separate Lord Rayleigh’s criterion: Physiologically motivated !!! The practical limit for \theta is about 70°. In an air objective or condenser, this gives a maximum NA of 0.95. In a high-resolution oil immersion lens, the maximum NA is typically 1.45, when using immersion oil with a refractive index of 1.52. Due to these limitations, the resolution limit of a light microscope using visible light is about 200 nm.

12. Nyquist sampling undersampled critically sampled ‘Nyquist’ sampled over sampled

13. Link between resolution and pixel size: Magnification Defined by camera Defined by objective Interline transfer CCD EM-CCDsCMOS 6.4 um 12.4 um 6.5 um p x < 8.9 um Not an easy decision: decreasing pixel size means increasing $$!

14. Pros and Cons of Standard LMs Pros Live imaging! Fairly quick: images every one second, if necessary (depends on camera speed) Cons Resolution limited at 200nm Increasing resolution, camera speed, light sources, depth of imaging == $$$. Some examples: Peyton lab: $170K Fancier, 3D microscopy: $1M + Can’t pick out individual proteins…..

15. Susan Anderson, University of Washington Charras, et al. JCB 2006 Ezrin Actin 2. Imaging of Intracellular Proteins

16. How immunofluorescence works

17. Pros and Cons of Fluorescent LM Pros Can visualize how what proteins a cell is expressing as a function of your material. Can visualize how the cells is organizing that protein, how much of the protein it’s expressing at a given time, and where in the cell it is. Cons Resolution limited at 200nm Increasing resolution, camera speed, light sources, depth of imaging == $$$. Some examples: Peyton lab: $170K Fancier, 3D microscopy: $1M + Sample prep can be time consuming. Cells are fixed, not live.…..

18. EGFP-Mena /mcherry-actin 3. Live Imaging of Individual Proteins Gertler Lab, MIT Tag protein with GFP How: recombinant DNA technology

19. Actin dynamics are regulated by density of matrix proteins 19 Speckle Microscopy: Individual actin monomers are stained at sub-maximum concentration Can see individual monomers move within a filament to watch dynamics

20. Pros and Cons of Live-fluorescent LM Pros Can visualize how what proteins a cell is expressing as a function of your material. Can visualize how the cells is organizing that protein, how much of the protein it’s expressing at a given time, and where in the cell it is. Live microscopy! Cons Increasing resolution, camera speed, light sources, depth of imaging == $$$. Some examples: Peyton lab: $170K Fancier, 3D microscopy: $1M + Sample prep can be time consuming. Takes months to create a single recombinant protein. Still resolution limited at 200nm…

21. MenaMena11a 3. Beat the Resolution Limits with Scanning Electron Microscopy Michele Balsamo & Leslie Mebane, Gertler Lab, MIT These filamentous structures are less than 100nm wide!

22. How SEM works Pro: sub-visible light wavelength imaging Con: fixed samples only, everything is under super vacuum. Con: sample preparation can be destructive, no water!!! Con: sample must be conductive!

23. Other issues that we don’t have time to discuss. What about very deep into tissues? LMs are depth limited to about 300um. Options: 2-photon imaging What about in an animal? A human??? Options: Intravital imaging, Photoacoustic tomography, MRI

24. Multiphoton Imaging

25. Intravital Imaging Cancer biophysics, Hubrect Institute

26. Photoacoustic Tomography

27. MRI

28. PET

29. Bone density scan