Title: Molecular Devices
1Molecular Devices
Chennai, September 14, 2005
K.L. Sebastian IPC Department, IISc http//ipc.iis
c.ernet.in/kls
2Outline
- 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
3 Height 8 nm Width 10 n
4ROLLER
MOLECULAR
What do you mean?
5Consider Hypostrophene-it is fluxional -perhaps
we can use this property!
To explain, let us start with Pentaprismane
6Pentaprismane (C10H10) D5h
Hypostrophene C2v
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8Degenerate Cope Rearrangement for Hypostrophene
Rate constant 1.8 X 10-5 sec-1
Activation energy
Q and Q are the partition functions of GS and TS
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10 Rolling Motion
Rolling-TS Eact 18 kcal/mol
Translation-TS Eact 65.5 kcal/mol
11Molecular Roller
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13Activation energy 13.6 kcal/mol (B3LYP/6-31G
C,H and 3-21G for Al)
TS
14MOLECULAR ROLLERS
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).
15MOLECULAR ROCKER
16Cope Rearrangement of Semibullvalene
17Semibullvalene on Al(100)
18Metal surface cluster of 14 or 32 Al atoms in
two layers Hydrogen atoms at the edges.
B3LYP/Al3-21G, C,H6-31G Ea 21.8 kcal/mol
19Fluxionality for Rotational Motion
20Hypostrophene
21Molecular wheel
22 MOLECULAR WHEEL
Eact 16.0 kcal/mol
23The activation barriers and rate constants
24Hopping onto adjacent Ge atoms
Adsorbed to the same site!
Eact 11.9 kcal/mol
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26Ea 5.97 kcal/mol B. Das and K.L. Sebastian
CPL 357, 25 ( 2002)
27We conclude that
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.
Bidisa Das, K.L Sebastian, Chemical Physics
Letters, 357, 25 (2002).
28Molecular Rattle
A
B
B
A
B
A
29Perhaps, in an excited state, this might happen
30Ring too small
31Eact42.4 kcal/mol
Eact a315 kcal/mol b36.6kcal/mol c33.6kcal/mol
These are the molecules that we studied but
activation energies for the umbrella inversion
kind of motion was found to be high.
M. Oda, Pure Appl. Chem. 58, 7 (1986), T.Z.
Ktaz, P. A. Garratt, J. Am. Chem. Soc. 85, 2852
(1963).
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33Ea 11.7 kcal/mol B. Das and K.L. Sebastian
CPL, 365, 320 (2002)
34Cyclononatetraenyl-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)
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36Nature does it well!
37Biological Molecular Motors
All of them occur in BIOLOGICAL systems
38Figure from http//ccgb.umn.edu/mwd/cell.html
39Figures and animation from http//www.sp.uconn.ed
u/terry/images/anim/ATPmito.html
40ATP Synthase (Rotary)
ATP Synthase
Synthesizes ATP. Rotates while it does this!
41Kinesin (Walker)
Works like a PORTER at the railway station
See animation at http//mc11.mcri.ac.uk/wrongtrous
ers.html
42Myosin
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/molbioc
hem/MBWeb/mb2/part1/myosin.htm
43Synthetic Molecular Motors
44Rotaxane
45Electron Removal
46Proton Addition
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48Catenanes
49Switching by Oxidation-Reduction Reations
50Catenanes how to have light driven motor?
station
shuttle
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52K.L. Sebastian Current Science, 87, 232 (2004)
53Can one have?
Cis-trans isomerization as in Azobenzene could be
useful
54Molecular Ratchets, Second Law and Detailed
Balance
55 It can undergo ratchet-like internal rotation!
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57The 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!
58K.L. Sebastian, Physical Review E61, 937 (2000)
59CONCLUSIONS
Fluxional behavior can be used to get interesting
mechanical motion
Ratchets, Light driven motor
60 Acknowledgements
Dr. Bidisa Das Prof. Ashoka Samuelson