j a3 = -r 7 2 r3 r θ F = m a3 j Centripetal force: m7 2 r; radial; towards centre.

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&(175,)8*$7,1 &LUFXODU PRWLRQ 7 = angular velocity (rad sec -1). (x,y) = r (cos, sin); = 7t j r3 = (x,y) =(r cos(7t), r sin(7t)) a3 = (d x/dt, d y/dt ) = -r 7 (cos(7t) - sin(7t)) j a3 = -r 7 r3 r θ F = m a3 j Centripetal force: m7 r; radial; towards centre. (In the spinning particle's frame of reference, the fictitious force is centrifugal.)

6HGLPHQWDWLRQ Archimedes' Principle (see.ppt slide)

3DUWLDO VSHFLILF YROXPH What is the volume of a molecule in solution? 1 cup sugar + 1 cup water << cups v dv dm volume increment of solution per unit mass solute v 1 ρ solute volume displaced by solute: v = m dv = m v dm Measurement of v: pycnometry (solution density) (or calculation based on a.a. composition) For proteins, v.73 cm 3 /g For nucleic acids, v.5 cm 3 /g

For a molecule in solution: dv volume = m = m v dm buoyancy = mass eff. weight = eff. = m v m (1- m (1- ρ g v ρ ) drag = f v = m (1- v ρ) ω r m (1- v ρ) ω r v = f v m (1- v ρ ) s = = ω r f v ρ) ω r

6HGLPHQWDWLRQ FRHIILFLHQW s v = = ω r m (1- v ρ ) f dimensions of s are time Svedberg unit: 1S 1-13 sec. For a hard spherical particle: f = 6 % r (Stokes equation) r = radius = viscosity of solution For proteins, f 1 to 1.5 the Stokes value (larger for fibrous proteins)

&HQWULIXJDWLRQ PHWKRGV see cent.ppt slides

&ODVVHV RI FHQWULIXJH low speed: to 5, g (Beckman J6) high speed: to 4, g (Beckman J1) vacuum ultracentrifuge: to 4, g (Beckman L8-55) Most lab. centrifuges are preparative instruments designed for recovery of samples after the run. An analytical ultracentrifuge incorporates an optical system designed to allow the progress of the sedimentation to be monitored continuously during the run. This facilitates determinations of sedimentation coefficients and molecular weights.

)L[HGDQJOH URWRUV

6ZLQJLQJEXFNHW URWRUV

'HQVLW\ JUDGLHQW FHQWULIXJDWLRQ RI FHOOV DQG RUJDQHOOHV s high (1 6 S to 1 7 S) ' low (1 to 1.) Media: appropriate density high water solubility low viscosity sterile biocompatible membrane-impermeant iso-osmolar: high MW Ficoll, albumin, metrizamide, etc. - not sucrose or salts

HOCH OH N H O C I O I C O CH 3 C N CH I NH OH CH OH OH CH H 3 C CH C O N I NH I C O OH O C I CH OH N H OH CH OH Iodixanol MW = 155 Smith et al., The use of iodixanol as a density gradient material for separating human sperm from semen, Arch. Androl. 38: 3-3, 1997. Iodixanol, a new nonionic density gradient material with relatively low osmolality and high density, was evaluated... for the separation of human sperm from semen... Using a three-layer iodixanol gradient (approximately 1.17/1.15/1.5 g/ml), sperm were centrifuged at 1, g for 3 min and collected from the 1.5/1.15 interface.... Sperm survived iodixanol density gradient centrifugation well, showing only modest declines in motility and velocity during a subsequent 4h incubation period....

5DWH ]RQDO EDQG VHSDUDWLRQ RI PDFURPROHFXOHV RQ SUHIRUPHG JUDGLHQWV VXFURVH RU JO\FHURO The gradient minimizes mixing due to mechanical disturbances or convection currents. Bands are collected in fractions; detected by UV-vis., fluorescence, radioactivity, enzyme assay, etc. Applications: Analytical: determination of s value Preparative: separation of proteins, nucleic acids

Schoettle et al., Mechanisms of inhibition of amido phosphoribosyltransferase from mouse L11 leukemia cells, Biochemistry 36: 6377-6383, 1997. Interconversion between the large and small forms of amido PRTase induced by AMP and piritrexim: Amido PRTase (.5 mg protein) was sedimented through sucrose gradients containing (a) 5. mm AMP, (b).5 mm AMP and 5 µm piritrexim, and (c) 1 µm piritrexim.

Methods: Linear sucrose gradients from 1 to 5% (w/v) were prepared using a... gradient maker. The sucrose gradients also contained... mm K Hepes (ph 7.3), 1. mm MgCl, 1. mm DTT, and other components (AMP, piritrexim, or P-Rib-PP) as required. Samples for centrifugation contained in a volume of µl, partially purified murine amido PRTase (.5 mg of protein), three marker proteins [alcohol dehydrogenase (1 mg), lactate dehydrogenase (15 µg), and catalase (5 µg)] with other components as indicated. Sedimentation profiles for amido PRTase were developed by centrifugation at 4, rpm in a Beckman SW41Ti rotor for 4h at 4C using a Beckman L8-8M ultracentrifuge. Gradients were fractionated by puncturing the bottom of the tube; 3 µl fractions were collected and assayed immediately for amido PRTase.

$SSOLFDWLRQ 6HSDUDWLRQ RI SRO\VRPHV Polysome profile of pea stem tissue using a 15 to 6% sucrose gradient spun at 3, g for 45 min. Polysomes with various size classes were analyzed using gradient fractionator with absorbance at 6 nm. http://133.71.15.39/english/methods/gradient.htm Lab. of Molecular Cell Biology, Ehime University, Japan

'HWHUPLQDWLRQ RI V XVLQJ DQDO\WLFDO XOWUDFHQWULIXJH v dr s = v = s = ω r dt dr = ω sdt r dr dt ω r r dr t = ω s dt r1 r ln r ln r = ω st t ln r = ω st ln r t So, if we plot ln r t vs. t, slope = 7 s.

'HWHUPLQDWLRQ RI : IURP V s = m (1- v ρ ) f f = RT ND R = gas constant; T = temperature; D = diffusion coefficient; N = Avogadro s number. (G.M. Barrow, Physical Chemistry, 5th ed., 1988,.5) s = m (1- v ρ ) RT ND m N = M M = RTs D (1- v ρ ) 6YHGEHUJ HTXDWLRQ But, accurate measurement of D is not easy.

6HGLPHQWDWLRQ HTXLOLEULXP (G.M. Barrow, Physical Chemistry, 5th ed., 1988,.7) One of the best methods for determining protein molecular weights, under native conditions (Laue, T.M., Advances in sedimentation velocity analysis, Biophys. J. 7: 395-396, 1997). Relatively low speed (about, rpm). Sedimentation tends to pull the protein to the bottom of the tube, but speed is insufficient to pellet out the protein. Protein concentration gradient develops, but the concentration difference (i.e., the gradient of chemical potential) causes net diffusion of protein molecules back up the tube. Centrifugation and diffusion processes reach sedimentation equilibrium: rate of sedimentation = rate of counter-diffusion. Difference in energy due to concentration (chemical potential energy difference): C C 1 = e ( E E ) 1 kt or ln C C 1 = ( E E ) 1 kt (k = R/N = Boltzmann's constant)

At equilibrium: 1 1 E E = F( r) dr = m ( 1 vρω ) r dr 1 r r 1 = ω ( r r1 ) m ( 1 vρ) C ln = C 1 r ω ( r r1 ) m ( 1 vρ) kt M = m N and R= k N, so m /k =M/R. r C ln = C 1 ω ( r r1 ) M ( 1 vρ) RT plot ln c vs r slope = ( 1 vρ) ω RT M M = RT d(ln c) ( 1 vρ) ω d( r )

$SSOLFDWLRQ RI VHGLPHQWDWLRQ HTXLOLEULXP PHWKRG Pauls, J.E.D., et al., Self-association of human protein S, Biochemistry 39, 5468-5473,.

,VRS\FQLF EXR\DQW GHQVLW\ FHQWULIXJDWLRQ RI QXFOHLF DFLGV Cs + salts of nucleic acids are very dense ('1.8). CsCl (7M) spun to sedimentation equilibrium at very high speeds, forming a narrow [CsCl] gradient. Applications: Analytical: Separate 14 N-DNA from 15 N-DNA: Meselson-Stahl experiment, 1958; semi-conservative replication of DNA. (method was developed for this experiment) Preparative: Plasmid purification.