k.l. sebastian ipc department, iisc kls chennai, september 14, 2005 molecular devices

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K.L. Sebastian IPC Department, IISc http://ipc.iisc.ernet.in/~kls Chennai, September 14, 2005 Molecular Devices

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Page 1: K.L. Sebastian IPC Department, IISc kls Chennai, September 14, 2005 Molecular Devices

K.L. Sebastian

IPC Department, IISc

http://ipc.iisc.ernet.in/~kls

Chennai, September 14, 2005

Molecular Devices

Page 2: K.L. Sebastian IPC Department, IISc kls Chennai, September 14, 2005 Molecular Devices

• Motivation – examples from biology

• Molecular Rollers and Rocker

• Molecular Wheel

• Molecular Rattle

. Fluxionality for Rotational Motion

• Nature does it very well! (Biological Molecular Motors)

• Synthetic Molecular Motors

• Light driven molecular motor

Outline

Page 3: K.L. Sebastian IPC Department, IISc kls Chennai, September 14, 2005 Molecular Devices

Height ~ 8 nm Width ~ 10 n

Is that a flower?

It is a motor

Page 4: K.L. Sebastian IPC Department, IISc kls Chennai, September 14, 2005 Molecular Devices

Can one design molecules that would

prefer to roll on a surface?

Seems rather difficult, perhaps we can try to

use fluxionality!

What do you mean?

ROLLERMOLECULAR

Page 5: K.L. Sebastian IPC Department, IISc kls Chennai, September 14, 2005 Molecular Devices

To explain, let us start with Pentaprismane

Consider Hypostrophene-it is fluxional -perhaps we

can use this property!

!!

Page 6: K.L. Sebastian IPC Department, IISc kls Chennai, September 14, 2005 Molecular Devices

Pentaprismane (C10H10)

D5h

Hypostrophene

C2v

Symmetry is broken! It can be broken in FIVE different ways!

hypostrophene

pentaprismane

H

Page 7: K.L. Sebastian IPC Department, IISc kls Chennai, September 14, 2005 Molecular Devices

Five degenerate minima! It should be possible to jump from

one to the other

It does! Known as Degenerate Cope Rearrangement

Page 8: K.L. Sebastian IPC Department, IISc kls Chennai, September 14, 2005 Molecular Devices

Rate constant

Degenerate Cope Rearrangement for Hypostrophene

GS TS

Activation energy

Q and Q* are the partition functions of GS and TS

Rate constant ~ 1.8 X 10-5 sec-1

Activation energy

25.31

B3LYP/6-31G** (kcal/mol)

Page 9: K.L. Sebastian IPC Department, IISc kls Chennai, September 14, 2005 Molecular Devices

Think of Hypostrophene

adsorbed on Al(100)

Page 10: K.L. Sebastian IPC Department, IISc kls Chennai, September 14, 2005 Molecular Devices

Rolling-TS Eact ~ 18 kcal/mol

Translation-TS:Eact ~ 65.5 kcal/mol

Rolling Motion

Page 11: K.L. Sebastian IPC Department, IISc kls Chennai, September 14, 2005 Molecular Devices

Same thing can happen with syn-

TOD!

Molecular Roller

Page 12: K.L. Sebastian IPC Department, IISc kls Chennai, September 14, 2005 Molecular Devices

GS TS

Activation energy

24.25

B3LYP/6-31G**(kcal/mol)

Syn-TOD

C2v

Cubane

Td

Page 13: K.L. Sebastian IPC Department, IISc kls Chennai, September 14, 2005 Molecular Devices

Activation energy

13.6 kcal/mol

(B3LYP/6-31G** C,H and 3-21G for Al)

TS

Page 14: K.L. Sebastian IPC Department, IISc kls Chennai, September 14, 2005 Molecular Devices

We conclude that:

Hypostrophene and tricyclooctadiene when chemisorbed on Al(100) surface should behave as ‘Molecular roller’

Bidisa Das, K.L Sebastian, Chemical Physics Letters, 330, 433 (2000).

MOLECULAR ROLLERS

Page 15: K.L. Sebastian IPC Department, IISc kls Chennai, September 14, 2005 Molecular Devices

MOLECULAR ROCKER

Page 16: K.L. Sebastian IPC Department, IISc kls Chennai, September 14, 2005 Molecular Devices

GS GS

Cope Rearrangement of Semibullvalene

Activation energy

5.5

B3LYP/6-31G**(kcal/mol)

TS

Page 17: K.L. Sebastian IPC Department, IISc kls Chennai, September 14, 2005 Molecular Devices

Semibullvalene on Al(100)

Page 18: K.L. Sebastian IPC Department, IISc kls Chennai, September 14, 2005 Molecular Devices

Metal surface: cluster of 14 or 32 Al atoms in two layers Hydrogen atoms at the edges.

B3LYP/Al:3-21G, C,H:6-31G**Ea = 21.8 kcal/mol

MOLECULAR ROCKER

Page 19: K.L. Sebastian IPC Department, IISc kls Chennai, September 14, 2005 Molecular Devices

Fe(CO)3

Fe(C

O) 3

Fe(C

O)3

Fe(CO)3 moving around

hypostrophene

Fluxionality for Rotational Motion

Page 20: K.L. Sebastian IPC Department, IISc kls Chennai, September 14, 2005 Molecular Devices

Hypostrophene

33.6

kcal/mol

4.3 kcal/mol

203i cm-1

Page 21: K.L. Sebastian IPC Department, IISc kls Chennai, September 14, 2005 Molecular Devices

Molecular wheel

Page 22: K.L. Sebastian IPC Department, IISc kls Chennai, September 14, 2005 Molecular Devices

C5H5Ge(CH3)3 is known to be fluxional!

Eact ~ 16.0 kcal/mol

MOLECULAR WHEEL

Page 23: K.L. Sebastian IPC Department, IISc kls Chennai, September 14, 2005 Molecular Devices

The activation barriers and rate constants

3.7X1085.74Sn (C,H: 6-31G**

& Sn: 3-21G)

1.6X10312.21Ge (C,H: 6-31G** & Ge: 6-31G**)

3.2X10214.04Si (C,H: 6-31G** & Si: 6-31G**)

rate constant at 298.15 K

(sec-1)

Eact

(kcal/mol)M atom bonded to Cp and basis-sets used

Page 24: K.L. Sebastian IPC Department, IISc kls Chennai, September 14, 2005 Molecular Devices

Cyclopentadienyl adsorbed on Ge surface,

should move like a

wheel!

Eact ~ 11.9 kcal/mol

Adsorbed to the same site!

Hopping onto adjacent Ge

atoms

Page 25: K.L. Sebastian IPC Department, IISc kls Chennai, September 14, 2005 Molecular Devices

2.5X1085.97

1.9X10411.90

8.5X10213.45

Rate constant(sec-1)

298.15 KEact

(kcal/mol)

Sn (C,H: 6-31G** & Sn:

3-21G)

Ge (C,H: 6-31G** & Ge:

6-31G**)

Si (C,H: 6-31G** & Si:

6-31G**)

M atom bonded to Cp and basis-sets used

Page 26: K.L. Sebastian IPC Department, IISc kls Chennai, September 14, 2005 Molecular Devices

Molecular Wheel

Sn

Ea = 5.97 kcal/mol

B. Das and K.L. Sebastian: CPL 357, 25 ( 2002)

That is not bad!Why don’t you call it a molecular “seal”?

Page 27: K.L. Sebastian IPC Department, IISc kls Chennai, September 14, 2005 Molecular Devices

We conclude that :

Bidisa Das, K.L Sebastian, Chemical Physics Letters, 357, 25 (2002).

The cyclopentadienyl co-adsorbed with hydrogen on Si/Ge/Sn (111) surfaces would form a system where the five membered ring can undergo spinning motion with low activation energies.

Page 28: K.L. Sebastian IPC Department, IISc kls Chennai, September 14, 2005 Molecular Devices

Molecular Rattle

A

B

B B

A

A

Page 29: K.L. Sebastian IPC Department, IISc kls Chennai, September 14, 2005 Molecular Devices

H

H

HHH

H

Does not happen! Ionization potential of

H too large!

Perhaps, in an excited state, this

might happen

H+

-

H+

-

Page 30: K.L. Sebastian IPC Department, IISc kls Chennai, September 14, 2005 Molecular Devices

Replace H with Li! Li+

-

Ring too small

Li+

-

Page 31: K.L. Sebastian IPC Department, IISc kls Chennai, September 14, 2005 Molecular Devices

These are the molecules that we studied but activation energies for the ‘umbrella inversion’

kind of motion was found to be high.

Eact~42.4 kcal/mol

Eact

a:315 kcal/mol

b:36.6kcal/mol

c:33.6kcal/mol

M. Oda, Pure & Appl. Chem. 58, 7 (1986), T.Z. Ktaz, P. A. Garratt, J. Am. Chem. Soc. 85, 2852 (1963).

Page 32: K.L. Sebastian IPC Department, IISc kls Chennai, September 14, 2005 Molecular Devices

C9H9-

Page 33: K.L. Sebastian IPC Department, IISc kls Chennai, September 14, 2005 Molecular Devices

Ea = 11.7 kcal/mol

B. Das and K.L. Sebastian: CPL, 365, 320 (2002)

Molecular Rattle

Proton going through benzene (C6H7

+)Mahapatra, Sathyamurthy, Current

Science, 1995

Page 34: K.L. Sebastian IPC Department, IISc kls Chennai, September 14, 2005 Molecular Devices

Cyclononatetraenyl-lithium

The activation barrier for the ‘umbrella

inversion’ in this case is ~11.5 kcal/mol

Normal mode analysis: 276 cm-1(GS), 274i cm-1(TS)

1D through ring motion calc.: 277 cm-1(GS), 267i cm-1 (TS)

Page 35: K.L. Sebastian IPC Department, IISc kls Chennai, September 14, 2005 Molecular Devices
Page 36: K.L. Sebastian IPC Department, IISc kls Chennai, September 14, 2005 Molecular Devices

Nature does it well!

Page 37: K.L. Sebastian IPC Department, IISc kls Chennai, September 14, 2005 Molecular Devices

Biological Molecular Motors

We know of several, efficient

molecular motors!

All of them occur in BIOLOGICAL

systems

Page 38: K.L. Sebastian IPC Department, IISc kls Chennai, September 14, 2005 Molecular Devices

Figure from: http://ccgb.umn.edu/~mwd/cell.html

Page 39: K.L. Sebastian IPC Department, IISc kls Chennai, September 14, 2005 Molecular Devices

Energy from photosynthesis

Figures and animation from: http://www.sp.uconn.edu/~terry/images/anim/ATPmito.html

Page 40: K.L. Sebastian IPC Department, IISc kls Chennai, September 14, 2005 Molecular Devices

ATP Synthase

Synthesizes ATP.Rotates while it

does this!

Most powerful known motor

ATP Synthase (Rotary)

Page 41: K.L. Sebastian IPC Department, IISc kls Chennai, September 14, 2005 Molecular Devices

Kinesin (Walker)

Proteins that WALK!

Works like a PORTER at the railway station

See animation at http://mc11.mcri.ac.uk/wrongtrousers.html

Page 42: K.L. Sebastian IPC Department, IISc kls Chennai, September 14, 2005 Molecular Devices

Myosin

Proteins that PUSH!

Myosin

For an animation, see the CD of the book: Molecular Biology of the Cell by

B. Alberts et. Al.

See also:

http://www.rpi.edu/dept/bcbp/molbiochem/MBWeb/mb2/part1/myosin.htm

Page 43: K.L. Sebastian IPC Department, IISc kls Chennai, September 14, 2005 Molecular Devices

Synthetic Molecular Motors

NO WAY near the natural

ones!

Page 44: K.L. Sebastian IPC Department, IISc kls Chennai, September 14, 2005 Molecular Devices

Rotaxane

shuttlestationstopper

station

Page 45: K.L. Sebastian IPC Department, IISc kls Chennai, September 14, 2005 Molecular Devices

-e+e

Electron Removal

Page 46: K.L. Sebastian IPC Department, IISc kls Chennai, September 14, 2005 Molecular Devices

+ H+

- H+

Proton Addition

Page 47: K.L. Sebastian IPC Department, IISc kls Chennai, September 14, 2005 Molecular Devices

Either electron removal or

proton addition

Page 48: K.L. Sebastian IPC Department, IISc kls Chennai, September 14, 2005 Molecular Devices

Catenanes

2-catenane 3-catenane

Page 49: K.L. Sebastian IPC Department, IISc kls Chennai, September 14, 2005 Molecular Devices

Switching by Oxidation-Reduction Reations

-e

+e

Page 50: K.L. Sebastian IPC Department, IISc kls Chennai, September 14, 2005 Molecular Devices

Catenanes – how to have light driven motor?

Leigh et. al. Nature, 424, 174 (2003)

Excitation of the station leads to unbinding!

station

shuttle

Page 51: K.L. Sebastian IPC Department, IISc kls Chennai, September 14, 2005 Molecular Devices

Light induced excitation of the shuttle is better!

Page 52: K.L. Sebastian IPC Department, IISc kls Chennai, September 14, 2005 Molecular Devices

K.L. Sebastian: Current Science, 87, 232 (2004)

Page 53: K.L. Sebastian IPC Department, IISc kls Chennai, September 14, 2005 Molecular Devices

Light induced conformational change driving translation!

Cis-trans isomerization as in Azobenzene could be

useful

Can one have……?

Page 54: K.L. Sebastian IPC Department, IISc kls Chennai, September 14, 2005 Molecular Devices

Brownian motion would drive the ratchet! But it can rotate only in

one direction! So thermal, random motion can be used to

drive the ratchet in one direction!

Molecular Ratchets, Second Law and Detailed Balance

Page 55: K.L. Sebastian IPC Department, IISc kls Chennai, September 14, 2005 Molecular Devices

[4]helicene

triptycene

Axle

It can undergo ratchet-like internal rotation!

A molecular ratchet was Synthesized and studied by Kelly et. al. Angewandte Chemie 109, 1969 (1997).

Page 56: K.L. Sebastian IPC Department, IISc kls Chennai, September 14, 2005 Molecular Devices

To probe rotational motion use NMR

That is clever!

Second Law verified!

Page 57: K.L. Sebastian IPC Department, IISc kls Chennai, September 14, 2005 Molecular Devices

But wait! Let us think about this!

There he goes! As mad as a

coot!

The fact that you can see rotation means

that your initial state is a non-equilibrium

one!So even if you had seen net rotation, that would not violate the second

law!

Page 58: K.L. Sebastian IPC Department, IISc kls Chennai, September 14, 2005 Molecular Devices

But you do not see any net rotation! What does

that mean?

Because of Detailed Balance!

K.L. Sebastian, Physical Review E61, 937 (2000)

Page 59: K.L. Sebastian IPC Department, IISc kls Chennai, September 14, 2005 Molecular Devices

CONCLUSIONS

Molecular Roller, Wheel, Rocker, Rattle!

Fluxional behavior can be used to get

interesting mechanical motion

Ratchets, Light driven motor……

Page 60: K.L. Sebastian IPC Department, IISc kls Chennai, September 14, 2005 Molecular Devices

 

        

        

  

Acknowledgements

Dr. Bidisa Das

Prof. Ashoka Samuelson