69451 weinheim, germany · table of contents s1. materials s2. techniques s3. synthesis of...
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Supporting Information © Wiley-VCH 2005
69451 Weinheim, Germany
Supplementary Information
for
The Internal Structure of Helical Pores Self-Assembled from Dendritic Dipeptides is Stereochemically
Programmed and Allosterically Regulated
Virgil Percec,* Andrés E. Dulcey, Mihai Peterca, Monica Ilies, Janine Ladislaw, Brad M. Rosen, Ulrica
Edlund, Paul A. Heiney
[*] Prof. V. Percec, A. Dulcey, Dr. M. Ilies, J. Ladislaw, B. M. Rosen, Dr. U. Edlund
Roy & Diana Vagelos Laboratories, Department of Chemistry
Laboratory for Research on the Structure of Matter
University of Pennsylvania
Philadelphia, PA 19104-6323 (USA)
Fax: (+1) 215-573-7888
E-mail: [email protected]
M. Peterca, Prof. P. A. Heiney
Department of Physics and Astronomy
Laboratory for Research on the Structure of Matter
University of Pennsylvania
Philadelphia, PA 19104-6396 (USA)
Table of Contents
S1. Materials
S2. Techniques
S3. Synthesis of Dendritic Dipeptides
S4. Analysis of Self-Assembly by CD and UV
Figure SF1. CD and UV spectra of dendritic dipeptides
Figure SF2. CD and UV spectra of model compounds for dendritic dipeptides
Scheme SF1. Model compounds and precursors for dendritic dipeptides
Figure SF3. UV spectra of molecular solutions of dendritic dipeptides and their precursors
Figure SF4. CD and UV spectra of dendritic dipeptides and model compounds at a single temperature
S5. Analysis of Supramolecular Structures by X-ray Diffraction Experiments
Figure SF5. Temperature dependence of X-ray diffraction stack plots for (4-3,4-3,5)12G2-CH2-Boc-L-
Tyr-L-Ala-OMe and for (4-3,4-3,5)12G2-CH2-Boc-D-Tyr-D-Ala-OMe
Figure SF6. Temperature dependence of X-ray diffraction stack plots for (4-3,4-3,5)12G2-CH2-Boc-L-
Tyr-D-Ala-OMe and for (4-3,4-3,5)12G2-CH2-Boc-D-Tyr-L-Ala-OMe
Figure SF7. Detailed view of the stereochemistry induced change in dipeptide conformation
S6. Determination of the Dependence of Dcol and Dpore on Temperature
Table ST1. X-ray diffraction data of dendritic dipeptides
Figure SF8. H-bonding network for L-L, D-D, L-D and D-L dendritic dipeptides and the formation of
the supramolecular pore structure
S7. References
2
S1. Materials
Methyl 4-hydroxybenzoate (99%) (from Lancaster Synthesis), thionyl chloride (99.5%), LiAlH4 (95%),
N-methyl morpholine (99%), methyl chloroformate (98%), anhydrous K2CO3 (all from Aldrich), 3,4-
dihydroxybenzoic acid (97%), 3,5-dihydroxybenzoic acid (97%), 1-bromododecane (98%), tyrosine (99%),
cyanuric chloride (99%), triphenylphosphine (99%) (all from Acros Organics), Boc-L-Tyr-OH (99%, [α]D24 = +
37.9o, 1% in dioxane), Boc-D-Tyr-OH (99%, [α]D24 = - 38.3o, 1% in dioxane), Boc-DL-Tyr-OH (99%), H2N-L-
Ala-OMe.HCl (99%, [α]D24 = + 7.2o, 2% in methanol), H2N-D-Ala-OMe.HCl (99%, [α]D
24 = - 7.5o, 2% in
methanol), H2N-DL-Ala-OMe.HCl (99%), (all from Bachem Peptides) were used as received. Acetone, N,N-
dimethylformamide, ethyl acetate, magnesium sulphate, methanol (all from Fisher, ACS reagents), silica gel
(Sorbent Technology) were used as received. Tetrahydrofuran (THF) and dichloromethane (Fisher, ACS reagent
grade) were refluxed over sodium/benzophenone and CaH2, respectively, and freshly distilled before use.
Cyclohexane and trifluoroethanol for CD experiments, dichloromethane for HPLC assays and THF for MALDI-
TOF assignments and for UV spectra were HPLC grade (Fisher). Deuterated chloroform for NMR spectra was
from Cambridge Isotope Laboratories. All other chemicals were commercially available and were used as
received. 2,6–Di-tert-butyl-4-methylpyridine (DTBMP) was prepared using a literature procedure[1] and 2-
chloro-4,6-dimethoxy-1,3,5-triazene (CDMT) was obtained from cyanuric chloride following a literature
synthesis.[2]
S2. Techniques
The purity of the products was determined by a combination of thin-layer chromatography (TLC), high
pressure liquid chromatography (HPLC), 1H and 13C NMR, as well as by matrix-assisted laser
desorption/ionization time-of-flight (MALDI-TOF) mass spectrometry. TLC was carried on silica gel coated
aluminum plates (indicator, F254; layer thickness, 200 µm; particle size, 2-25 µm; pore size 60Å, SIGMA-
Aldrich). HPLC was performed in dichloromethane, on a Perkin-Elmer Series 10 high pressure liquid
chromatograph equipped with a LC-100 column oven, Nelson Analytical 900 Series integrator data station and
two Perkin-Elmer PL gel columns of 5 x 102 and 1 x 104 Å, using for detection the UV absorbance at 254 nm. 1H
NMR (500 MHz) and 13C NMR (125 MHz) spectra were recorded on a Bruker DRX 500 instrument.
3
UV spectra were registered on a Shimadzu-1601 UV spectrophotometer at 23 oC, in THF (1.6 x 10-5 M)
using a quartz cuvette of 0.1 cm path length.
Thermal transitions were measured on a Thermal Analysis (TA) Instrument modulated differential
scanning calorimeter (DSCQ100). In all cases the heating and the cooling rates were 10 °C min-1. The transition
temperatures were measured as the maxima and minima of their endothermic and exothermic peaks. Indium was
used as calibration standard. An Olympus BX51 thermal optical microscope (100X magnification) equipped
with a Mettler FP82HT hot stage and a Mettler Toledo FP90 Central Processor were used to verify thermal
transitions and to characterize anisotropic textures. Small parts of the aligned samples were heated on the hot
stage up to temperatures close but always bellow isotropic transition to avoid losing the sample alignment. After
a short annealing, image acquisitions were performed. Density measurements were carried out by floatation in
gradient columns at 20 oC.
Matrix-assisted laser desorption/ionization time-of-flight (MALDI-TOF) mass spectrometry was carried
out on a PerSeptive Biosystems-Voyager-DE (Framingham, MA) mass spectrometer operating in linear mode.
The spectrometer equipped with a nitrogen laser (337 nm) was calibrated using Angiotensin II and Bombesin as
standards. The laser steps and voltages applied were adjusted depending on both the molecular weight and the
nature of each analysed compound. Either 2,5-dihydroxybenzoic acid or 4-hydroxybenzylidenemalononitrile was
used as matrix. THF was used for dissolving both matrix and sample (working concentrations: 10 mg/ml for the
matrix and 5-10 mg/ml for the sample). The analytical sample was obtained my mixing sample and matrix
solutions in a 1/5 v/v ratio; 0.5 µL of this resulting solution were loaded onto the MALDI plate and allowed to
dry at 23 oC before performing the analysis.
Circular dichroism (CD) spectra were recorded on a Jasco J-720 spectrophotometer equipped with a
NESLAB RTE-111 variable temperature circulator. Each sample of dendritic dipeptides was dissolved in
cyclohexane (1.6 x 10-4 M) at 23 oC, then heated to 60 oC and allowed to cool at 23 oC when the solution
remained homogenous. (4-345)12G1-CO2-L-DEG* and (4-345)12G1-CO2-D-DEG* used as model compounds
were dissolved in trifluoroethanol (3 x 10-4 M). CD measurements were performed using a 1 ml quartz cuvette of
0.1 cm path length and the following parameters: scanned optical range, 210-320 nm; scan band width, 1 nm;
scanning speed, 100 nm/min; response, 1 sec; accumulations, 5; 3 scanned thermal ranges: 8-60 oC, 60-8 oC, 8-
4
60 oC, respectively (data pitch: 2 oC; temperature slope: 1 oC/min). Before starting the experiment the sample
was allowed to reach the 8 oC starting temperature (~ 10-15 minutes) but once started the 3 thermal cycles were
performed successively. Data were processed using Jasco Spectra Manager V. 1.51 software.
X-ray diffraction (XRD) measurements were performed using Cu-Kα1 radiation (λ=1.54178 Å) from a
Bruker-Nonius FR-591 rotating anode X-ray source with a 0.2 x 0.2 mm2 filament operated at 3.4 kW. The beam
was collimated and focused by a single bent mirror and sagitally focusing Si (111) monochromator, resulting in a
0.3 x 0.4 mm2 spot on a Bruker-AXS Hi-Star multiwire area detector. To minimize attenuation and background
scattering, an integral vacuum was maintained along the length of the flight tube and within the sample chamber.
Powder or aligned samples were held in quartz capillaries (0.7 – 1.0 mm diameter), than mounted in a
temperature controlled oven (temperature precision: ± 0.1 oC, temperature range from -120°C to 270°C). Sample
to Bruker-AXS Hi-Star multiwire area detector distances are 12.0 cm for wide angles diffraction experiments,
and 54.0 cm for intermediate angles diffraction experiments. Aligned samples for fiber XRD experiments were
prepared using a custom made extrusion device. The powdered sample (~ 10 mg) was heated inside the extrusion
device to isotropic transition temperature. After cooling slowly from the isotropic phase, the fiber was extruded
in the mesophase and cooled to 23 oC. Typically the aligned samples have a thickness of ~ 0.3-0.7 mm and a
length of ~ 3-7 mm. All XRD measurements were done with the aligned sample axis perpendicular to the beam
direction. XRD peaks position and intensity analysis was performed using Datasqueeze Software (version 2.01)
that allows background elimination and Gaussian, Lorentzian, Lorentzian squared, or Voigt peak-shape fitting.
Molecular modelling and simulation experiments were performed using the Materials Studio Modelling
(version 3.1) software from Accelrys. Package’s Discover module was used to perform the energy minimizations
on the supramolecular structures with the following settings: PCFF or COMPASS force fields, and Flechter-
Reeves algorithm for the conjugate gradient method. Details were repoted previously.[3] The reported molecular
models are in agreement with the small and wide angle XRD results on oriented fibers and with the experimental
densities results.[3]
S3. Synthesis of Dendritic Dipeptides
Synthesis of dendritic dipeptides was carried out as previously described.[3] All samples were purified by
flash column chromatography (silica gel, eluent MeOH/CH2Cl2 1%) until the purity was higher than 99%,
5
followed by precipitation into methanol from a concentrated solution in CH2Cl2. The sample was filtered and
dried to constant weight under vacuum at 23 oC. The complete structural analysis for the newly synthesized
derivatives was also reported in the same paper.[3] The measured densities of the supramolecular structures
generated from dendritic dipeptides are between 0.99 – 1.02 g/cm3.
S4. Analysis of Self-Assembly by CD and UV
CD and UV spectra for all dendritic dipeptides during their self-assembly in cyclohexane are presented
in Figure SF1. Figure SF2 shows the self-assembly of a self-assembling benzyl ether dendritic molecule (4-
3,4,5)12G1-CO2-L and D-DEG* (Scheme SF1) that contains an aliphatic stereocenter attached to the dendron via
an ester group. Even if self-assembly of these two sets of moleculaes takes place in different solvophobic
solvents, comparison of the CD spectra from Figures SF1a,b and SF2a,b indicates that the CD spectra of L-L, D-
D, L-D and D-L are due to the aromatic part of the dendron. The CDs of the dipeptides and of the dendritic
dipeptides as molecular solutions show a weak Cotton effect at 232 nm that has an opposite sign to that of the
Cotton effects of the self-assembled dendrons from the same range of the spectrum (Figure SF1). The molecular
Cotton effect can be obtained in good solvent or in solvophobic solvents above 30oC.[3] The Cotton effect from
above 290 nm of the (4-3,4,5)12G1-CO2-L and D-DEG* (Figure SF2) is due to the benzoate moiety of the (4-
3,4,5)12G1-CO2-DEG* dendron (Figure SF3).
6
7
8
9
10
11
12
The chemical structures of the compounds analyzed by UV spectra are shown in Scheme SF1.
HN
O
NH
OCH3
O
O
O
OH
HN
O
NH
OCH3
O
O
O
OH
HN
O
NH
OCH3
O
O
O
OH
HN
O
NH
OCH3
O
O
O
OH
HO HOOC12H25
HOO
O
OC12H25
OC12H25 HO
O
O
O
O
O
O
OC12H25
OC12H25
OC12H25
OC12H25
4-12G0-CH2OH C6H5-CH2-OH
Boc-D-Tyr-D-Ala-OMe Boc-L-Tyr-L-Ala-OMe
(4-3,4)12G1-CH2OH
Boc-L-Tyr-D-Ala-OMe Boc-D-Tyr-L-Ala-OMe (4-3,4-3,5)12G2-CH2OH
O
OO
OC12H25
OC12H25
OC12H25
OH3C
OO
OO
OC12H25
OC12H25
OC12H25
HO
OO
OO
OC12H25
OC12H25
OC12H25
HO
(4-3,4,5)12G1-COOCH3 (4-3,4,5)12G1-COOH (4-3,4,5)12G1-CH2OH
O
OO
OC12H25
OC12H25
OC12H25
O
OO
HO O
OO
OC12H25
OC12H25
OC12H25
O
OO
HO
(4-3,4,5)12G1-CO2- D-DEG* (4-3,4,5)12G1-CO2- L-DEG*
Scheme SF1. Model compounds and precursors for the dendritic dipeptides.
As shown in Figure SF3a, the higher the dendrimer generation the more intense the UV absorption, as
one should expect as a result of the increasing number of aromatic units in the structure. Figure SF3b illustrates
the UV absorption of the dendritic dipeptides as compared to the UV absorption of the dipeptides, whereas
Figure SF3c presents UV spectra for a dendron containing at its apex other structural moieties than the
dipeptides and for its precursors. The UV spectra in Figure SF3a,b demonstrate that the aromatic part of the
dendron absorbs below 290 nm. The addition of a carboxylic unit to the aromatic part of the dendron extends the
absorption above 290 nm (Figure SF3c).
13
220 230 240 250 260 270 280 290 300 310 3200.0
0.2
0.4
0.6
0.8
1.0
1.2
1.4
1.6
1.8
Abs
λ /nm
Benzyl Alcohol (4)-12G0CH2OH (4-3,4)12G1CH2OH (4-3,4-3,5)12G2CH2OH (4-3,4-3,5)12G2CH2Boc-D-Tyr-D-Ala-OMe (4-3,4-3,5)12G2CH2Boc-D-Tyr-L-Ala-OMe (4-3,4-3,5)12G2CH2Boc-L-Tyr-D-Ala-OMe (4-3,4-3,5)12G2CH2Boc-L-Tyr-L-Ala-OMe
in THF (1.6 x 10-5 M)
220 230 240 250 260 270 280 290 300 310 3200.0
0.2
0.4
0.6
0.8
1.0
1.2
1.4
1.6
Figure SF3. UV spectra of molecular solutions at 23°C: a) absorption increases with the increase of dendrimer generation,
i.e. increase number of aromatic units; b) absorption of dendritic dipeptide compared with dipeptide absorption; c)
absorption of (4-3,4,5)12G1 dendron containing different groups at the apex.
Figure SF4 compares the CD-UV spectra of (4-3,4-3,5)12G2-CH2-Boc-L-Tyr-L-Ala-OMe and of (4-
3,4,5)12G1-CO2-L-DEG* ( both in cyclohexane) at the temperature at which their CD signal was most intense.
As it can be seen, below 290 nm both spectra present similar patterns. The UV absorption and the CD signal of
(4-3,4,5)12G1-CO2-L and D-DEG* above 290 nm are due to its benzoate ester part.
1.8
in THF (1.6 x 10-5 M)
(4-3,4-3,5)12G2-CH2-Boc-L-Tyr-L-Ala-OMe Boc-D-Tyr-D-Ala-OMe Boc-D-Tyr-L-Ala-OMe Boc-L-Tyr-D-Ala-OMe Boc-L-Tyr-L-Ala-OMe
Abs
λ /nm
220 230 240 250 260 270 280 290 300 310 320 330 340 350
b) a)
c)
0.0
0.2
0.4
0.6
0.8
1.0
1.2
in THF (1.6 x 10-5 M)
λ /nm
Abs
(4-3,4,5) 12G1-CH2OH
(4-3,4,5) 12G1-COOCH3
(4-3,4,5) 12G1-COOH (4-3,4,5) 12G1-CO2-D-DEG*
14
220 240 260 280 300 320 3400.0
0.5
1.0
1.5
2.0
2.5
3.0
3.5
4.0
4.5
220 240 260 280 300 320 340
-200-180-160-140-120-100-80-60-40-20020406080
Θ x10-3/degcm2dmol-1
Abs
λ /nm
(4-3,4-3,5)12G2-CH2-Boc-L-Tyr-L-Ala-OMe in cyclohexane at 8°C (1.6 x 10-4 M)
UV
CD
220 240 260 280 300 320 3400.0
0.5
1.0
1.5
2.0
2.5
3.0
3.5
4.0
4.5
220 240 260 280 300 320 340
-140-120-100-80-60-40-20
020406080
Θ x10-3/degcm2dmol-1
Abs
λ /nm
(4-3,4,5)12G1-CO2-L-DEG* in trifluoroethanol at 10°C (3.0 x 10-4 M)
CD
UV
a)
b)
Figure SF4. Combined CD-UV spectra of: a) (4-3,4-3,5)12G2-CH2-Boc-L-Tyr-L-Ala-OMe in cyclohexane (1.6 x 10-4 M)
and b) (4-3,4,5)12G1-CO2-L-DEG* in trifluoroethanol (3 x 10-4 M).
15
S5. Analysis of Supramolecular Structures by X-ray Diffraction Experiments
Supporting X-ray data are shown in Figures SF5 and SF6, while Figure SF7 shows a detailed view of the
dipeptide and dendron conformations.
(10) (10)
I (11) (11) / a.u. (20) I (20)
/ a.u.(21) (21)
(10) (10)
I (11) (11) / a.u.(20) I (20) / a.u.
(21) (21)
Figure SF5. Stacked plots showing temperature dependence of X-ray diffraction for (4-3,4-3,5)12G2-CH2-Boc-L-Tyr-L-
Ala-OMe (top): second heating (left), second cooling (right) and for (4-3,4-3,5)12G2-CH2-Boc-D-Tyr-D-Ala-OMe (bottom):
second heating (left), second cooling (right).
16
(10) (10)
I I (11) / a.u.(11)
(20) / a.u.(20) (21) (21)
(10) (10)
I (11) I (11) (20) / a.u. / a.u.(20) (21) (21)
Figure SF6. Stacked plots showing temperature dependence of X-ray diffraction for (4-3,4-3,5)12G2-CH2-Boc-L-Tyr-D-
Ala-OMe (top): second heating (left), second cooling (right) and for (4-3,4-3,5)12G2-CH2-Boc-D-Tyr-L-Ala-OMe (bottom):
second heating (left), second cooling (right).
17
L- L D-D
L-D D-L
Figure SF7. Detailed view of the stereochemistry induced change in dipeptide conformation: for simplicity the (4-3,4-
3,5)12G2-CH2-dendron is shown without the aliphatic tails, dashed squares indicate Tyr stereocenter that dictates the
supramolecular helix sense.
S6. Determination of the Dependence of Dcol and Dpore on Temperature
The dependence of Dcol and Dpore on temperature was obtained from powder small angle X-ray
diffraction experiments performed at various temperatures (see Table ST1). Dcol was calculated from the X-ray
diffractograms data by averaging the lattice parameter a calculated from (10), (11), and (20) peaks position: Dcol
= a = {4*π/[3*sqrt(3)]}*(1/q10+sqrt(3)/q11+2/q20) Å, where qhk is the scattering vector for the (hk) reflection.
Dpore was calculated from the integrated (hk0) peaks intensities using the method reported in detail in the
Supplementary Material to ref. [3] and in reference [4]. The X-ray diffractograms used for these calculations are
presented in Figures SF5 and SF6.
Figure SF8 presents in detail H-bonding network (lengths in Å) for L-L, D-D, L-D and D-L dendritic
dipeptides and the formation of the supramolecular pore structure.
18
Table ST1: X-ray diffraction data collected at 20°C.
Compound T [°C]
d10a [Å]
(I10b a.u.)
d11a [Å]
(I11b a.u.)
d20a [Å]
(I20b a.u.)
d21a [Å]
(I21b a.u.)
a=Dcol[Å]
Dpore [Å]
(4-3,4-3,5) 12G2 CH2 Boc -
L-Tyr-L-Ala 20 67.0 (43.72)
38.4 (26.63)
33.5 (24.27)
25.5 (5.36) 77.1±0.4 13.3±1.2
D-Tyr-D-Ala 20 68.5 (43.25)
39.4 (26.0)
34.2 (24.23)
26.1 (6.51) 78.9±0.4 13.9±1.2
L-Tyr-D-Ala 20 69.7 (42.01)
40.0 (26.46)
34.7 (25.0)
27.4 (5.37) 80.2±0.4 14.6±1.4
D-Tyr-L-Ala 20 69.4 (40.7)
39.8 (26.61)
34.4 (23.5)
27.2 (9.17) 79.8±0.4 15.4±1.4
[a] columnar hexagonal phase d-spacings; [b] peak intensity scaled to the sum of the observed diffraction peaks (a.u.=arbitrary units).
Figure SF8. H-bonding network (lengths in Å) for a) L-L, b) D-D, c) L-D and d) D-L dendritic dipeptides and the formation
of the supramolecular pore structure. The strongest in layer directional H-bonds are labeled by the same convention as in
Figure 5: j-k and l-m, respectively. Column axis is vertical; for simplicity only the N-hydrogen atoms are shown (colored in
white in a), b), c), d) and green in e), f), g) and h), while the carbon atoms of each dipeptide are shown in different colors
(same color for one dipeptide) and the phenyl ring of Tyr is omitted. The helical H-bonded supramolecular structure
resulted from the j-k and l-m hydrogen bonds:e) and f) - side view and g) - top view. Complete pore structure in h) - side
view and i) - top view (dendron is not shown, color code: C - gray, H – white, N-H – green, Boc – blue, O – red).
D-L
2.21
2.04 1.31 1.32
2.21
2.15
1.16
2.04
k j
l m
m L-L
2.33
2.09
1.88
1.96
1.79
2.3
j k
j
m
k
l
L-D
2.23
2.33 1.1
2.2
2.16
1.28
2.46
1.15 j k
m
l
2.3
e) f) a) b) h) D-D
l
2.43 2.43 2.12
2.21 2.12
k j
d) c)
k i) g)
k j
m j
l
19
S7. References. [1] P.J. Stang, A.G. Anderson, J. Org. Chem. 1976, 41, 3034-3036.
[2] J.S. Kronin, F.O. Ginah, A.R. Murray, J.D. Copp, Synthetic Commun. 1996, 26,3491-3494
[3] V. Percec, A.E. Dulcey, V.S.K. Balagurusamy, Y. Miura, J. Smidrkal, M. Peterca, S. Nummelin, U. Edlund,
S.D. Hudson, P.A. Heiney, H. Duan, S.N. Maganov, S.A. Vinogradov Nature 2004, 430, 764-768.
[4] D.C. Turner, S.M. Gruner, Biochemistry 1992, 31, 1340-1355.
20