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ver sensor with “sample inside” al (Manalis lab) Weighing biomolecules…in f 446:1066 (2007) echanism of ver as mass 2p)(k/m e ) 1/2 ing for position of Dm along length of canti /2p) [k/(m e + aDm)] 1/2 Df r /f r ~ -aDm/2m e if at end f evenly distributed

Cantilever sensor with “sample inside”

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Cantilever sensor with “sample inside” Burg et al ( Manalis lab) Weighing biomolecules …in fluid. Nature 446:1066 (2007) Basic mechanism of c antilever as mass s ensor: f r = (1/2 p) (k/m e ) 1/2 Correcting for position of D m along length of cantilever: - PowerPoint PPT Presentation

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Page 1: Cantilever  sensor with “sample inside”

Cantilever sensor with “sample inside”Burg et al (Manalis lab) Weighing biomolecules…in fluid. Nature 446:1066 (2007)

Basic mechanism ofcantilever as mass sensor:

fr = (1/2 )p (k/me)1/2

Correcting for position of Dm along length of cantilever: f’r = (1/2p) [k/(me + aDm)]1/2 Dfr/fr ~ -aDm/2me

a = 1 if at end¼ if evenly distributed

Page 2: Cantilever  sensor with “sample inside”

What is m for cantilever? (Does it make sensein terms of vol x sp grav?)

What is fr?

What is k? What are units for k?

Page 3: Cantilever  sensor with “sample inside”

How accurately can you measure Dfr (and hence Dm)?

Depends on “sharpness” of resonance, measured byQuality factor Q = fr/width at half-max

Q is also measure of damping of resonance= 2p x energy stored/energy dissipated per cycle

Caveat – this Q is not the same as Qflow [vol/s]!

Page 4: Cantilever  sensor with “sample inside”

What limits precision in measurements of fr?Let dfr = st. dev. of repeated measurements of fr

What happens if you don’t drive the cantilever?

Do these motions add to motion of driven cantilever?

Would you be surprised if kBT/average driving energyof cantilever EC appeared in formula for dfr?

Is Brownian motion related to viscous damping?(both due to random hits …)

Since Q is related to dissipation, would you be surprisedif Q appeared in formula for dfr?

Page 5: Cantilever  sensor with “sample inside”

dfr/fr ~ (kBT/EC)1/2 (1/Q)1/2

Ekinci et al, J Appl Phys 95:2682 (2004)

So Brownian motion (which limits Q) provides fundamental limit to mass detection

and is more important the bigger kBT compared to EC

100-fold decrease in Q can -> ~ 10-fold loss ofsensitivity to measure small Dm

Page 6: Cantilever  sensor with “sample inside”

Q in vacuum ~ 15,000Q in water ~ 150

So putting aqueous sample inside cantilever insteadof cantilever in water sample may permit ~ 10-fold greater sensitivity to detect small masses

How important is it for cantilever to be in vacuum ratherthan air (given that sample is inside)? How doesQ vary with viscosity?

Page 7: Cantilever  sensor with “sample inside”

Does water inside the cantilever lead to damping?

Why doesn’t Fig 2bshow a shift in freq.on filling with water?Doesn’t water changethe mass?

Page 8: Cantilever  sensor with “sample inside”

Perfect paper to calculate m (from cantilever dim.); expected fr; expected sensitivity from Dm for given # of molecules bound; flow channel vol.; flow rate as function of P; PeH, PeS, ds, Da; receptor density, sensor area, equil. fraction of receptors with tgt. at different co, KD; teq

and compare all to observed values!

Example: ds = av. distance diffused in time it takes to flow L At flow rate 10pl/s, flow chamber 3x8x400mm (HxWxL) vol = 10pl, so time to flow L = 1s. For 10nm molecule, D=kBT/6phr = 2x10-11m2/s, <x>=(6Dt)1/2 = 10mm, so proteins have time to bind. Is depletion zone important?

Page 9: Cantilever  sensor with “sample inside”

Charging up device w/capture antibody – whatis coating method?Est. # capturing mol. boundAnalyte binding: in steady state, b/bm= (c0/KD)/(1+c0/KD)Estimate KD = co at half- max binding. Is this higher than expected?Estimate koff (= 1/2tequil at c0 = KD). Is it longer than expected? ? rebinding Est. lowest detectable conc.

Page 10: Cantilever  sensor with “sample inside”

In steady state,b/bm= (c0/KD)/(1+c0/KD)

If they can reliably detect2nM analyte, estimate howhow many molecules are bound at this conc.

If closely packed, # receptors = (1/100nm2) x area= 2x[3x400 + 8x400]mm2/100nm2 = 108

b/bm = 1/10 => # bound molecules = 107

Is Dfr consistent with Dm predicted from this # molecules?

Page 11: Cantilever  sensor with “sample inside”

Does sample need to bind to inside wall of cantileverto be sensed?

What is this figuresupposed to show? What should be thetime scale of the x axis?Could you check ifthis is what you expect for given P?

Page 12: Cantilever  sensor with “sample inside”

mcant ~ 5x10-8gfr ~ 200kHzDfr ~ 0.05HzDm ~ 10fgDfr/fr ~ Dm/2mAre the masses reasonable (vol x sp grav)? Are the Dfr’s expected for these masses?

Why might they be able to detect smaller Dfr‘s here thanin protein binding?

Page 13: Cantilever  sensor with “sample inside”

Could they get 5x106-fold sensitivity increase(detect single molecules) if they dida sandwich assay by flowing in 100nm goldparticles coated with 20 antibody?

A tethered gold np could act as a “mass amplifier”

Would the drag force on a tethered gold np belarge enough to break one antigen-antibody bond?Estimate Fdrag = 6phrv ~ 5pN at 1/3 atm pressure, probably close to limit where bond destabilized

Page 14: Cantilever  sensor with “sample inside”

Why mightbacteriahave a broaderdistribution offrequency shiftsthan the goldbeads?

How big are bacteria compared to channel dimensions?What might you worry about?

Page 15: Cantilever  sensor with “sample inside”

Remarkable reproducibility after regenerating surfacewith acetic acid/H2O2! So (presumably mod. expensive)chips could be reused.

Without subtracting change dueto 1mg/ml BSA in sample

Can devices be re-used for multiple assays?

Page 16: Cantilever  sensor with “sample inside”

Area

(100mm)2

1mm2

1cm2

Exercise – convert total mass to # mol. if MW = 105

Page 17: Cantilever  sensor with “sample inside”

Summary

Very nice idea of putting flow cell inside cantilever!

Do they need fancy vacuum? How does Q vary with h?

Sensitivity for mass detection ~5x106 protein molecules ~2nM at standard KD in “label-free” mode; not so diff. from ELISA!

Nice idea of counting particles (that change mass> 10 fg) as they flow through

Could it be used in sandwich format with “mass amplifiernp” to detect single protein molecules?

Page 18: Cantilever  sensor with “sample inside”

Next week – ELISA with magnetic read-out using giantmagneto-resistance (GMR) sensors Nat. Med. 15:1327 (09)

Issues to pay attention to:How small a fraction of capture antibodies binding

analyte can they detect? What is dynamic range?Why does it work in real-time mode (without washing)?How much better is it with washing?How complex is the sensor?