chemistry in overcrowded systems —concept and...
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Chemistry in Overcrowded Systems—Concept and Application—
Organic Seminar 11/06/06Tatsuo Kojima (D2)PI: Prof. Nakamura
Steric Effect in Organic Chemistry1
Crowded
Ph o-Tol Mes Tip Mes* (Supermesityl)
R
R
A-value
Si
Me Et i-Pr Cy Me3Si t-Bu
1.74 ~1.75 ~2.15 2.15 ~2.5 4.9
Use of Steric Effect2
Development of XPhos
Isolation of Unstable Compounds
t-Bu OTs HN+
2% Pd(OAc)25% Ligand
toluene/t-BuOH(5/1)
110 ˚C, Cs2CO3
t-Bu
N
PR2
i-Pr i-Pr
PR2
Me Me
i-Pr
1: R = Cy2: R = t-Bu3: R = Et
4: R = Cy5: R = t-Bu
Yield (GC):
1 2 3 4 5
84% 38% 0% 8% 12%
Buchwald, S. L. et al. JACS, 2003, 125, 6653.
t-Bu
t-Bu
t-Bu
t-Bu
N NP P
Mes*
Mes*
Si Si
Mes
Mes Mes
Mes
West (1981) Yoshifuji (1981) Arduengo (1991)Maier (1978)
Kinetic stabilization
Kinetic Stabilization vs Thermodynamic Stabilization3
MM
M
kinetic thermodynamic
cyclobutadiene
NEt2
Et2N
EtO2C
CO2Et
t-Bu
t-Bu
t-Bu
t-Bu
Overcrowded Ligands for Kinetic Stabilization4
SiMe3
SiMe3
SiMe3
Me3Si
SiMe3
Me3Si
Tbt =i-Pri-Pr
Ar' =
i-Pr i-Pr
M
TbtTbt
MAr
Ch
M = Si, Ge, SnCh = S, Se, Te
Si
Si
Si
Si
Si
Bbi =
JACS, 2011, 133, 6890.
Co
!5-C60Ar5
ChCh
Ch
(Ch = S, Se)
Cr Cr
Ar'
Ar'
Si SiBbi
Bbi
Acc. Chem. Res, 2000, 33, 625.Acc. Chem. Res, 2004, 37, 86. Science, 2005, 310, 844.
Science, 2004, 305, 1755.
Thermodynamic Effect in Overcrowded Systems5
Biali et al. JACS, 1990, 112, 9300.
The thermodynamic stability can be reversedin overcrowded systems.
Conformation of all-trans-polyisopropylcyclohexane
all-eq all-ax
Crowded
all-eq all-ax
reverse order
i-Pr
i-Pri-Pr i-Pr
i-Pr
i-Pr ••••••i-Pr
i-Pri-Pr
i-Pr
i-Pr
i-Pr
Todayʼs Topic6
Crowded
The hidden nature of the molecule can be extractedin overcrowded systems.
Frustrated Lewis Pair Thermochromism of overcrowded alkenes Unidirectional molecular motor based on overcrowded alkenes
Frustrated Lewis Pair (FLP)7
Metal-free activation of H2
Classical Lewis pair Frustrated Lewis pair
P B+ P B P B+
Mes2P B(C6F5)2
F F
F F
H2
heatMes2P B(C6F5)2
F F
F FH
H
Stephan, D. W. et al. Science, 2006, 314, 1124.
R3P + B(C6F5)3
H2R3P + B(C6F5)3H H
Stephan, D. W. et al. JACS, 2007, 129, 1880.(R = t-Bu or Mes)
Theoretical Study of FLP8
The frustrated complex can be accessed only in an overcrowded pair.
P B
P B
Frustrated complex
Pápai et al. ACIE, 2008, 47, 2435; JACS, 2009,131, 2029.Grimme, S.; Erker, G. ACIE, 2010, 49, 1402.
Mechanism of the Activation9
P B
Frustrated complex(flexible)
P B
H2
Electronic fieldby donor and acceptor
HH
P BH
H!+
!–
P BH H
H–H is easily cleaved in the preorganized space.
Boundary of Two Complexes10
Does the boundary between theclassical adduct and thefrustrated complex exist ?
Two types of the complexes are not mutually exclusive.
N B(C6F5)3 N B(C6F5)3+ N B(C6F5)3+H HH2
Stephan, D. W. et al. JACS, 2009,131, 3476.
Application of FLP11
Metal-free catalytic hydrogenation
Activation of alkenes and CO2
Ph R
Nt-Bu
R = Me or H
Ph R
HNt-Bu
toluene, 25 ˚C
H2 (1.5 bar)
Mes2PB(C6F5)2
Mes2PB(C6F5)2
H
H
(5-20 mol%)
ca.80%
Stephan, D. W. Erker, G.et al. ACIE, 2008, 47, 7543.
Stephan, D. W. et al. ACIE, 2007, 47, 4968.Stephan, D. W. Erker, G.et al. ACIE, 2009, 49, 6643.
(t-Bu)3P + B(C6F5)3B(C6F5)3
(t-Bu)3P OO
(t-Bu)3P B(C6F5)3+CO2, rt
–CO2, 70 ˚C
Overcrowded Alkenes12
M
M
HH HHCrowded Steric hindranceAround fjord region
planar planar
ΔE
twist anti syn
We can use various conformations of the alkenein overcrowded alkenes.
Themochromism of Overcrowded Alkenes13
O
O
The availability and the order of the stabilityof the conformations are important.
A
heat
Byellow green / blue
Thermochromic
O
O
Thermochromic Not thermochromic
twist anti syn
Colored Coloreless or pale yellow
(Meyer, 1909)
Agranat, I. et al. Chem. Commun. 2001, 954.
twist
anti twist
ΔE < 30 kJ/mol
Molecular Motors Based on Overcrowded Alkenes14
The nonplanar conformation leads to helical chiralityand two diastreomers.
1st generation motorFeringa, B. L. et al. Nature, 1999, 401, 152.
2nd generation motorFeringa, B. L. et al. JACS, 2000, 122, 12005.
+
S
S
rotor
axle
stator
Unidirectional Rotation of Molecular Motors15
Meax Meeq
MeaxMeeq
hv
thermalhelix inversion
thermalhelix inversion
hv
Acceleration of Molecular Motors16
Review: Adv. Funct. Mater. 2007, 17, 819.Recent acceleration: CEJ, 2009, 15, 2768.
S
R
OMe
t1/2 = 0.67 h
makelower partflexible
109 fold
acceleration
decrease
ring size
3x104 fold
acceleration
increase
substituent size
t1/2 = >1300 year
107 fold
acceleration
t1/2 = 190 s t1/2 = 5.74 ms
decreasehelicenesize
13 foldacceleration
t1/2 = 15 s t1/2 = 0.16 ms(R = PhCC-)
1x106 fold
acceleration
decrease
helicene size
44 rotation/s(cf. F1-ATPase130 rotation/s)
S
S
OMe OMe
S
S
O O
(CH2)8 (CH2)8
HS HS
Brust-Schiffrinmethod
S
S
O O
(CH2)8 (CH2)8
S S
Toward a Realistic Application17
Rotating speed fast enough against “Brownian storm” Unidirectionally controlled axles
Molecular motors on the gold surface
Feringa, B. L. et al. Nature, 2005, 437, 1337.
Au251(motor)26t1/2 = 1.2x103 s
Aut1/2 = 5.6x102 s
Nano Car with a Molecular Motor18
S S
Proposed propulsion scheme on a heated substrate
Tour, J. M. et al. OL, 2006, 8, 1713..
Asymmetric Synthesis with the Molecular Motor19
Feringa, B. L. et al. Science, 2011, 331, 1429.
R
R
NH
HN
N
NMe2 HN
S
CF3
CF3
(2R,2R')-(P,P)-trans-1
A B
Asymmetric Synthesis with the Molecular Motor20
Feringa, B. L. et al. Science, 2011, 331, 1429.
(P,P)-trans-1
(M,M)-cis-1
(P,P)-cis-1
Summary21
Crowded
The hidden nature of the molecule can be extractedin overcrowded systems.
P B
Frustrated complex
twist
anti
Colored
Colorless
Two conformations forthemochromism Unidirectional motor