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Today ’ s Announcements. HW returned today. 2. Another HW assigned yesterday, because I messed up. Due Friday. Today ’ s take-home lessons (i.e. what you should be able to answer at end of lecture). FRET – Fluorescence Resonance Energy Transfer (Invented in 1967)
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Today’s Announcements • HW returned today. • 2. Another HW assigned yesterday, because I messed up. Due Friday.
Today’s take-home lessons(i.e. what you should be able to answer at end of lecture) FRET – Fluorescence Resonance Energy Transfer (Invented in 1967) why its useful, R-6 dependence; R0 (2-8 nm), very convenient.
FRET: measuring conformational changes of (single) biomolecules FRET FRET useful for 20-80Å Distance dependent interactions between green and red light bulbs can be used to deduce the shape of the scissors during the function.
FRET is so useful because Ro (2-8 nm) is often ideal Bigger Ro (>8 nm) can use FIONA-type techniques (where you use two-different colored-labels)
Donor Emission Donor Emission http://mekentosj.com/science/fret/
Acceptor Emission Acceptor Emission http://mekentosj.com/science/fret/
E.T. leads to decrease in Donor Emission & Increase in Acceptor Emission http://mekentosj.com/science/fret/
E Energy Ro 50 Å Transfer Acceptor Donor R (Å) Dipole-dipole Distant-dependent Energy transfer Time Time Fluorescence Resonance Energy Transfer (FRET) Spectroscopic Ruler for measuring nm-scale distances, binding Look at relative amounts ofgreen& red
Energy Transfer Acceptor Donor Derivation of 1/R6 Energy Transfer. = function (kET, knd) E.T. = kET/(kET + knd) E.T. = 1/(1+ knd/kET) E.T. = 1/(1+ 1/kETtD) Kn.d. How is kET dependent on R? kET knon-distance = knd = kf + kheat= 1/tD= 1/ lifetime
Classically: How is kET dependent on R? How does the energy go with distance? Think of a source emitting and look at R1, then 2R1, 3R1. U ≈1/R2 (Traveling: photons) U ≈ E2 ; E ≈ 1/R How does electric field go like? This is in the “Far-field”: (d >> l) In the Near-field (d << l) (must remember your E&M) E ≈1/R3 peE = pe/R3 Dipole emitting: Energy = U = Dipole absorption: paE Probability that absorbing molecule (dipole) absorbs the light So light emission goes like paE x peE = papeE2, pepa/R6 ≈ E.T. Classically: E.T. goes like R-6 (Depends on Ro) E.T. = 1/(1+ (R6/Ro6)) E.T. = 1/(1+ 1/kETtD)
or ? Energy Transfer goes like… Take limit…
Terms in Ro in Angstroms • J is the normalized spectral overlap of the donor emission (fD) and acceptor absorption (eA) • qD is the quantum efficiency (or quantum yield) for donor emission in the absence of acceptor (qD = number of photons emitted divided by number of photons absorbed). • n is the index of refraction (1.33 for water; 1.29 for many organic molecules). • k2 is a geometric factor related to the relative orientation of the transition dipoles of the donor and acceptor and their relative orientation in space.
Terms in RoJ: Does donor emit where acceptor absorbs? in Angstroms where J is the normalized spectral overlap of the donor emission (fD) and acceptor absorption (eA) Spectral Overlap between Donor (CFP) & Acceptor (YFP) Emission Ro≈ 49-52Å.
With a measureable E.T. signal E.T. leads to decrease in Donor Emission & Increase in Acceptor Emission http://mekentosj.com/science/fret/
E.T. by changes in donor. Need to compare two samples, d-only, and D-A. E.T. by increase in acceptor fluorescence and compare it to residual donor emission. Need to compare one sample at two l and also measure their quantum yields. Where are the donor’s intensity, and excited state lifetime in the presence of acceptor, and ________ are the same but without the acceptor. Time Time How to measure Energy TransferDonor intensity decrease, donor lifetime decrease, acceptor increase.
Class evaluation • What was the most interesting thing you learned in class today? • 2. What are you confused about? • 3. Related to today’s subject, what would you like to know more about? • 4. Any helpful comments. Answer, and turn in at the end of class.