mohammed zuned desai michael james wong koji hirota areio hashemi group d

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Mohammed Zuned Desai Michael James Wong Koji Hirota Areio Hashemi Group D

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Page 1: Mohammed Zuned Desai Michael James Wong Koji Hirota Areio Hashemi Group D

Mohammed Zuned DesaiMichael James Wong

Koji HirotaAreio Hashemi

Group D

Page 2: Mohammed Zuned Desai Michael James Wong Koji Hirota Areio Hashemi Group D

Background Applications Description Objectives Methodology Fabrication Results Future Work Gantt Chart References

Page 3: Mohammed Zuned Desai Michael James Wong Koji Hirota Areio Hashemi Group D

What are Magnetic Tweezers (MT)?◦ Scientific instrument used for studying molecular

and cellular interactions◦ Ability to apply known forces on paramagnetic

particles using a magnetic field gradient◦ One of the most commonly used force

spectroscopy techniques Atomic Force Microscopy Optical Tweezers

Page 4: Mohammed Zuned Desai Michael James Wong Koji Hirota Areio Hashemi Group D

They do not have problems of sample heating and photodamage that effects optical tweezers

Magnetic forces are orthogonal to biological interactions

Offer the prospect of highly parallel single-molecule measurements ◦ Hard to achieve with other single-molecule

force spectroscopy techniques

Page 5: Mohammed Zuned Desai Michael James Wong Koji Hirota Areio Hashemi Group D

The magnet configurations are relatively easy to assemble

Ideally suited for the study of DNA topology and topoisomerases

Study Molecular interactions 65pN to rupture bond between lectin and RBC membrane-

bound glycolipids. 60-130pN to extract beta2-integrins (CD18) from neutrophil

membrane in 1-4sec 100pN to extract integral glycoprotein from cell lipid bilayer

(RBC membrane) 165pN to rupture P-selectin bond with leukocyte-membrane-

bound P-selectin glycoprotein ligand-1. 40-400pN to separate a pair of cell adhesion proteoglycan

molecules on marine sponge cell surfaces.

Page 6: Mohammed Zuned Desai Michael James Wong Koji Hirota Areio Hashemi Group D

How do magnetic tweezers work?

http://www.biotec.tu-dresden.de/cms/fileadmin/research/biophysics/practical_handouts/magnetictweezers.pdf

Aspects:• Two magnets• Magnetic Field• Magnetic Gradient• Superparamagnetic

beads• Surface Molecules

Page 7: Mohammed Zuned Desai Michael James Wong Koji Hirota Areio Hashemi Group D

suspension of microspheres

molecular layer

transparent substrate

N

S

CCD

objective

mirrorlayer modified

with ligands

layer modified with protein

force

• Experiment design: Working View

7

Design of Magnetic Design of Magnetic TweezersTweezers

Page 8: Mohammed Zuned Desai Michael James Wong Koji Hirota Areio Hashemi Group D

Negative Control:No inhibitor on the surface

time

F

time

F

beadssettle

magn. wash @ 1 pN

beadssettle

magn. wash @ 1 pN

data collection @ 12 pN

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Beads and surfaces coated with BovineCarbonic anhydrase and sulfonamide inhibitor

8

Dissociation of CA-sulfonamide Dissociation of CA-sulfonamide complexes:complexes:

Page 9: Mohammed Zuned Desai Michael James Wong Koji Hirota Areio Hashemi Group D

Calibrating design: Side View

Square capillary with

suspension of microspheres

N

S

CCD

force

9

Page 10: Mohammed Zuned Desai Michael James Wong Koji Hirota Areio Hashemi Group D

force

Force calculations using Stoke’s drag equation:◦ Calibrate:

Distance between the core of the electromagnet and paramagnetic beads

Current flowing through the coil of the magnet

Example: ◦ Time it takes bead to move vertically 0.5mm =

3.46s◦ Velocity of bead (v) = 0.1445 mm/s◦ Fluid’s viscosity (u)= 0.998 mPa s◦ Radius of bead (r) = 1.5 um◦ Drag Force = 4.07379 pN

Gravitational Force ~ 0.3 pN

rFd 6

Fd Fg

10

FM

gdM FFF

Page 11: Mohammed Zuned Desai Michael James Wong Koji Hirota Areio Hashemi Group D

Design and fabricate magnetic tweezers that is capable of achieving forces up to 100pN◦ Current design can achieve 2pN◦ Consist of a single magnet

Introduce illumination for bright-field transmission microscopy

Page 12: Mohammed Zuned Desai Michael James Wong Koji Hirota Areio Hashemi Group D

Using Finite Element Method Magnetics (FEMM) to predict the geometries of the magnet and that will produce the largest possible field gradients

Machine and assemble the design that will produce the largest field gradients

Calibrate the magnet so it is ready for data acquisition

Page 13: Mohammed Zuned Desai Michael James Wong Koji Hirota Areio Hashemi Group D

Open source finite element analysis software package for solving electromagnetic problems.

Good for processing:◦ 2D planar and Axisymmetric problems ◦ Magnet◦ Electrostatic ◦ Heat and Current Flow

It is a simple, accurate, and low computational cost freeware product, popular in science and engineering.

Reliability comparable to commercial software Referenced in several Journals Used by several reputable societies

IEEE Magnetics UK and Japan Magnetics

Page 14: Mohammed Zuned Desai Michael James Wong Koji Hirota Areio Hashemi Group D

A) Characteristics of Magnets Core size Tip shape

B) Double Magnet Runs Test FEMM reliability Core, Shape, and Angle

C) Core Material Mu metal

D) Coil Manipulation Increasing the number of coils Changing their location

Looking at how these characteristics affect the magnetic gradient

¼ inch

1.5 inch

1/8 inch

Page 15: Mohammed Zuned Desai Michael James Wong Koji Hirota Areio Hashemi Group D

Small vs Big Core

Iron

0.25 in

0.5 in

1.5 in

0.37 in

0.75 in

1.25 inIron

Coil Core

Small core gave better uniform magnetic gradient

Page 16: Mohammed Zuned Desai Michael James Wong Koji Hirota Areio Hashemi Group D

Magnetic field and Magnetic gradient

Page 17: Mohammed Zuned Desai Michael James Wong Koji Hirota Areio Hashemi Group D

Tip Shape

Angle161.80

760

45.20

Arc Angle300

450

600

900

Concave300

450

600

900

θ

LengthSmall: 0.01mmMedium: 0.08mmLarge: 0.15

Flat showed best results Second best was tip with angle of 161.80

Page 18: Mohammed Zuned Desai Michael James Wong Koji Hirota Areio Hashemi Group D

Whatever characteristics of single magnet we don’t want to blindly assume are the same for double magnets◦ Ex: Flat small has better magnetic gradient but

this does not mean that Flat small gives better gradient with double magnets so we run double magnets

Reliability of FEMM through comparison of single and double results

Page 19: Mohammed Zuned Desai Michael James Wong Koji Hirota Areio Hashemi Group D

A) Small double vs Big double

B) Small double with Shapes (tip, arc, concave)

1800 shows best results

C) Changing angle (600, 900,1800)

θ

θ = 150

θ = 450

θ = 600

2mm

Page 20: Mohammed Zuned Desai Michael James Wong Koji Hirota Areio Hashemi Group D

Mu Metal vs Iron Different tip shapes Double vs Single

Angle Tips

The Small Mu Metal flat magnet showed the best results in single and double magnet runs

MuMetal

0.25 in

0.5 in

1.5 in

Page 21: Mohammed Zuned Desai Michael James Wong Koji Hirota Areio Hashemi Group D

Testing to see how coil manipulation effects the magnetic field

Increasing the number of coils Location of the coil

A) C)B)

Page 22: Mohammed Zuned Desai Michael James Wong Koji Hirota Areio Hashemi Group D

700

Page 23: Mohammed Zuned Desai Michael James Wong Koji Hirota Areio Hashemi Group D
Page 24: Mohammed Zuned Desai Michael James Wong Koji Hirota Areio Hashemi Group D

Overall Design

Light source

DC power supply

CCD camera

Stage

Reflect mirror

Objective lens

Stage adjuster

Magnet

Page 25: Mohammed Zuned Desai Michael James Wong Koji Hirota Areio Hashemi Group D

Stage Stage Manipulator

Page 26: Mohammed Zuned Desai Michael James Wong Koji Hirota Areio Hashemi Group D

MagnetMirror

Page 27: Mohammed Zuned Desai Michael James Wong Koji Hirota Areio Hashemi Group D

Objective: Verify that flat tip shows the best results Prove that the tip gives the largest magnetic field gradient

values at very short distances.

Tested different tips Flat Cylinder Tip

Parameters◦ Voltage: 3v, 6v, 12v◦ Current: 0.1 Amps◦ Distance:

0-.5mm (0.1mm increments) .5-3.1mm (0.2mm increments)

Page 28: Mohammed Zuned Desai Michael James Wong Koji Hirota Areio Hashemi Group D

Magnetometer Probe

Tip

Magnet

AdjustmentsKnobs

DC power supply

ScotchTape

Page 29: Mohammed Zuned Desai Michael James Wong Koji Hirota Areio Hashemi Group D

G vs Length dG/dL vs Length

1Gauss = 1 x 10-4 Tesla (B)

Page 30: Mohammed Zuned Desai Michael James Wong Koji Hirota Areio Hashemi Group D

B vs Length dB/dL vs Length

Page 31: Mohammed Zuned Desai Michael James Wong Koji Hirota Areio Hashemi Group D

Finished experimenting on magnet characteristics to obtain greatest magnetic field gradient.

Fabricated majority of the device setup

Performed trial runs on single magnet with different tips to verify certain trends

Page 32: Mohammed Zuned Desai Michael James Wong Koji Hirota Areio Hashemi Group D

Ship final magnetic design with the material to the Robert M. Hadley Company.

Locate homogeneous field Experiment with horizontal distance with very small

increments Capability: 100th of a mm

Start working with beads◦ Velocity measurements◦ Force measurements

Page 33: Mohammed Zuned Desai Michael James Wong Koji Hirota Areio Hashemi Group D
Page 34: Mohammed Zuned Desai Michael James Wong Koji Hirota Areio Hashemi Group D

Dr. Valentine Vullev Dr. Sharad Gupta Dr. Hyle Park Dr. Jerome Schultz Gokul Upadhyayula Hong Xu

Page 35: Mohammed Zuned Desai Michael James Wong Koji Hirota Areio Hashemi Group D

1) Neuman, Keri C, and Nagy, Attila. “Single-molecule force spectroscopy: 1) Neuman, Keri C, and Nagy, Attila. “Single-molecule force spectroscopy: optical tweezers, magnetic tweezers and atomic force microscopy.” optical tweezers, magnetic tweezers and atomic force microscopy.” Nature Nature Publishing GroupPublishing Group Vol. 5, NO. 6. June 2008. Vol. 5, NO. 6. June 2008.

2) Danilowicz, Claudia, Greefield, Derek and Prentiss, Mara. “Dissociation of 2) Danilowicz, Claudia, Greefield, Derek and Prentiss, Mara. “Dissociation of Ligand-Receptor Complexes Using Magnetic Tweezers.” Ligand-Receptor Complexes Using Magnetic Tweezers.” Analytical ChemistryAnalytical Chemistry Vol. 77, No. 10. 15 May. 2005.Vol. 77, No. 10. 15 May. 2005.

3) Humphries; David E., Hong; Seok-Cheol, Cozzarelli; Linda A., Pollard; Martin 3) Humphries; David E., Hong; Seok-Cheol, Cozzarelli; Linda A., Pollard; Martin J., Cozzarelli; Nicholas R. “Hybrid magnet devices fro molecule manipulation J., Cozzarelli; Nicholas R. “Hybrid magnet devices fro molecule manipulation and small scale high gradient-field applications”. United States Patent and and small scale high gradient-field applications”. United States Patent and Trademark Office, An Agency of The United States Department of Commerce. Trademark Office, An Agency of The United States Department of Commerce. <http://patft.uspto.gov>. January 6, 2009. <http://patft.uspto.gov>. January 6, 2009.

4) Ibrahim, George; Lu, Jyann-Tyng; Peterson, Katie; Vu, Andrew; Gupta, Dr. 4) Ibrahim, George; Lu, Jyann-Tyng; Peterson, Katie; Vu, Andrew; Gupta, Dr. Sharad; Vullev, Dr. Valentine. “Magnetic Tweezers for Measuring Forces.” Sharad; Vullev, Dr. Valentine. “Magnetic Tweezers for Measuring Forces.” University of California Riverside. Bioengineering Senior Design June 2009.University of California Riverside. Bioengineering Senior Design June 2009.

5) Startracks Medical, “Serves Business, Education, Government and Medical 5) Startracks Medical, “Serves Business, Education, Government and Medical Facilities Worldside.” American Solution. Startracks.org, Inc. CopyrightFacilities Worldside.” American Solution. Startracks.org, Inc. Copyright 2003. <http://images.google.com/imgres?imgurl=http://www.startracksmedical.com/supplies/invertedmicroscope.jpg&imgrefurl=http://www.startracksmedical.com/supplies.html&usg=__butCY2zWJa7nAkwkjiPxX_mFy0=&h=450&w=450&sz=24&hl=en&start=2&um=1&tbnid=XH6gnQuJLS7bRM:&tbnh=127&tbnw=127&prev=/images%3Fq%3Dinverted%2Bmicroscope%26hl%3Den%26sa%3DN%26um%3D1>