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The zwitterionic, isomeric, title compounds, Gly-Met and Met-Gly are me­thio­nine-containing dipeptides, which show very different conformations in the solid state.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S2056989024005504/hb8099sup1.cif
Contains datablocks Gly-Met, Met-Gly, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2056989024005504/hb8099Gly-Metsup2.hkl
Contains datablock Gly-Met

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2056989024005504/hb8099Met-Glysup3.hkl
Contains datablock Met-Gly

CCDC references: 2361459; 2361458

Computing details top

L-Glycyl-L-methionine (Gly-Met) top
Crystal data top
C7H14N2O3SF(000) = 220
Mr = 206.26Dx = 1.369 Mg m3
Monoclinic, P21Mo Kα radiation, λ = 0.71073 Å
a = 6.2517 (2) ÅCell parameters from 5067 reflections
b = 5.4935 (2) Åθ = 2.8–40.1°
c = 14.5686 (6) ŵ = 0.30 mm1
β = 91.147 (4)°T = 90 K
V = 500.24 (3) Å3Plate, colourless
Z = 20.38 × 0.29 × 0.03 mm
Data collection top
Bruker Kappa APEXII DUO CCD
diffractometer
5922 independent reflections
Radiation source: fine-focus sealed tube5356 reflections with I > 2σ(I)
TRIUMPH curved graphite monochromatorRint = 0.026
φ and ω scansθmax = 40.3°, θmin = 2.8°
Absorption correction: multi-scan
(SADABS; Krause et al., 2015)
h = 911
Tmin = 0.836, Tmax = 0.991k = 99
11393 measured reflectionsl = 2626
Refinement top
Refinement on F2Hydrogen site location: mixed
Least-squares matrix: fullH atoms treated by a mixture of independent and constrained refinement
R[F2 > 2σ(F2)] = 0.033 w = 1/[σ2(Fo2) + (0.0417P)2]
where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.079(Δ/σ)max = 0.001
S = 1.04Δρmax = 0.53 e Å3
5922 reflectionsΔρmin = 0.30 e Å3
131 parametersAbsolute structure: Flack x determined using 2141 quotients [(I+)-(I-)]/[(I+)+(I-)] Parsons et al. (2013)
1 restraintAbsolute structure parameter: 0.02 (2)
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
S10.20146 (4)0.44474 (6)0.42848 (2)0.01468 (6)
O10.69310 (13)0.51962 (16)0.16278 (6)0.01361 (15)
O20.19251 (13)0.15688 (15)0.17287 (6)0.01189 (14)
O30.17853 (13)0.50896 (16)0.09597 (6)0.01188 (13)
N10.87880 (15)0.89936 (16)0.08355 (7)0.00999 (15)
H11N0.913 (3)0.757 (4)0.0948 (13)0.015*
H12N0.981 (3)0.994 (4)0.1072 (12)0.015*
H13N0.865 (3)0.912 (4)0.0257 (13)0.015*
N20.42247 (14)0.73584 (17)0.22578 (7)0.00962 (14)
H2N0.353 (3)0.863 (4)0.2171 (13)0.012*
C10.67091 (16)0.9440 (2)0.12752 (8)0.01317 (16)
H1D0.5632790.9950800.0806090.016*
H1E0.6863421.0762540.1733290.016*
C20.59716 (16)0.71258 (19)0.17425 (7)0.00938 (15)
C30.30874 (16)0.51654 (19)0.25172 (7)0.00890 (15)
H30.4102960.4060100.2853990.011*
C40.22080 (16)0.38311 (18)0.16587 (7)0.00835 (15)
C50.12523 (18)0.5846 (2)0.31603 (8)0.01112 (17)
H5A0.1843070.6755500.3694480.013*
H5B0.0230820.6925580.2829030.013*
C60.00678 (19)0.3600 (2)0.34991 (8)0.01315 (18)
H6A0.1093330.2490240.3813090.016*
H6B0.0575070.2721650.2968220.016*
C70.3286 (2)0.1514 (2)0.43812 (9)0.0175 (2)
H7A0.3813350.0989190.3774880.026*
H7B0.4487520.1632810.4800640.026*
H7C0.2247430.0324880.4620530.026*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
S10.01416 (11)0.01407 (11)0.01605 (12)0.00108 (10)0.00637 (8)0.00091 (10)
O10.0117 (3)0.0077 (3)0.0216 (4)0.0011 (3)0.0036 (3)0.0016 (3)
O20.0114 (3)0.0072 (3)0.0170 (4)0.0006 (2)0.0009 (3)0.0006 (3)
O30.0144 (3)0.0112 (3)0.0100 (3)0.0016 (3)0.0009 (2)0.0005 (3)
N10.0094 (3)0.0088 (4)0.0118 (4)0.0009 (3)0.0007 (3)0.0011 (3)
N20.0087 (3)0.0068 (3)0.0133 (4)0.0008 (3)0.0007 (3)0.0006 (3)
C10.0119 (4)0.0079 (3)0.0199 (4)0.0005 (4)0.0050 (3)0.0024 (4)
C20.0085 (4)0.0074 (3)0.0121 (4)0.0012 (3)0.0009 (3)0.0003 (3)
C30.0086 (3)0.0077 (3)0.0104 (4)0.0009 (3)0.0001 (3)0.0014 (3)
C40.0068 (3)0.0076 (3)0.0107 (4)0.0006 (3)0.0011 (3)0.0006 (3)
C50.0121 (4)0.0104 (4)0.0110 (4)0.0013 (3)0.0021 (3)0.0007 (3)
C60.0141 (4)0.0113 (4)0.0142 (4)0.0011 (3)0.0054 (3)0.0003 (3)
C70.0147 (5)0.0183 (5)0.0194 (5)0.0046 (4)0.0030 (4)0.0025 (4)
Geometric parameters (Å, º) top
S1—C71.8037 (13)C1—H1D0.9900
S1—C61.8114 (11)C1—H1E0.9900
O1—C21.2310 (13)C3—C41.5415 (15)
O2—C41.2598 (13)C3—C51.5417 (15)
O3—C41.2546 (13)C3—H31.0000
N1—C11.4809 (14)C5—C61.5262 (16)
N1—H11N0.83 (2)C5—H5A0.9900
N1—H12N0.886 (19)C5—H5B0.9900
N1—H13N0.849 (19)C6—H6A0.9900
N2—C21.3437 (14)C6—H6B0.9900
N2—C31.4527 (14)C7—H7A0.9800
N2—H2N0.832 (19)C7—H7B0.9800
C1—C21.5181 (16)C7—H7C0.9800
C7—S1—C698.22 (6)C4—C3—H3108.8
C1—N1—H11N107.2 (13)C5—C3—H3108.8
C1—N1—H12N111.5 (12)O3—C4—O2125.57 (10)
H11N—N1—H12N107.1 (19)O3—C4—C3117.55 (9)
C1—N1—H13N110.1 (12)O2—C4—C3116.86 (9)
H11N—N1—H13N107.3 (19)C6—C5—C3111.85 (9)
H12N—N1—H13N113.3 (18)C6—C5—H5A109.2
C2—N2—C3118.29 (9)C3—C5—H5A109.2
C2—N2—H2N115.1 (13)C6—C5—H5B109.2
C3—N2—H2N118.5 (13)C3—C5—H5B109.2
N1—C1—C2109.41 (9)H5A—C5—H5B107.9
N1—C1—H1D109.8C5—C6—S1110.86 (8)
C2—C1—H1D109.8C5—C6—H6A109.5
N1—C1—H1E109.8S1—C6—H6A109.5
C2—C1—H1E109.8C5—C6—H6B109.5
H1D—C1—H1E108.2S1—C6—H6B109.5
O1—C2—N2124.15 (10)H6A—C6—H6B108.1
O1—C2—C1120.47 (9)S1—C7—H7A109.5
N2—C2—C1115.37 (9)S1—C7—H7B109.5
N2—C3—C4110.59 (8)H7A—C7—H7B109.5
N2—C3—C5109.33 (9)S1—C7—H7C109.5
C4—C3—C5110.53 (8)H7A—C7—H7C109.5
N2—C3—H3108.8H7B—C7—H7C109.5
C3—N2—C2—O115.40 (16)C5—C3—C4—O393.47 (11)
C3—N2—C2—C1163.44 (9)N2—C3—C4—O2153.99 (9)
N1—C1—C2—O18.46 (15)C5—C3—C4—O284.80 (11)
N1—C1—C2—N2172.66 (9)N2—C3—C5—C6176.94 (9)
C2—N2—C3—C462.19 (12)C4—C3—C5—C661.10 (12)
C2—N2—C3—C5175.89 (9)C3—C5—C6—S1177.94 (8)
N2—C3—C4—O327.75 (13)C7—S1—C6—C5171.26 (9)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N1—H11N···O3i0.83 (2)2.15 (2)2.8513 (13)143.0 (18)
N1—H11N···O10.83 (2)2.15 (2)2.6619 (13)120.1 (16)
N1—H12N···O2ii0.886 (19)1.850 (19)2.7275 (12)170.7 (18)
N1—H13N···O3iii0.849 (19)1.86 (2)2.7006 (13)168 (2)
N2—H2N···O2iv0.832 (19)2.000 (19)2.8225 (12)170.0 (18)
Symmetry codes: (i) x+1, y, z; (ii) x+1, y+1, z; (iii) x+1, y+1/2, z; (iv) x, y+1, z.
L-Methionyl-L-glycine (Met-Gly) top
Crystal data top
C7H14N2O3SDx = 1.382 Mg m3
Mr = 206.26Mo Kα radiation, λ = 0.71073 Å
Orthorhombic, P212121Cell parameters from 9827 reflections
a = 5.2521 (3) Åθ = 3.0–40.2°
b = 11.4126 (7) ŵ = 0.31 mm1
c = 16.5403 (10) ÅT = 90 K
V = 991.43 (10) Å3Needle fragment, colourless
Z = 40.25 × 0.24 × 0.17 mm
F(000) = 440
Data collection top
Bruker Kappa APEXII DUO CCD
diffractometer
6231 independent reflections
Radiation source: fine-focus sealed tube5939 reflections with I > 2σ(I)
TRIUMPH curved graphite monochromatorRint = 0.030
φ and ω scansθmax = 40.3°, θmin = 2.2°
Absorption correction: multi-scan
(SADABS; Krause et al., 2015)
h = 89
Tmin = 0.872, Tmax = 0.950k = 2020
33593 measured reflectionsl = 3030
Refinement top
Refinement on F2Hydrogen site location: mixed
Least-squares matrix: fullH atoms treated by a mixture of independent and constrained refinement
R[F2 > 2σ(F2)] = 0.023 w = 1/[σ2(Fo2) + (0.0356P)2 + 0.0451P]
where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.061(Δ/σ)max = 0.001
S = 1.06Δρmax = 0.44 e Å3
6231 reflectionsΔρmin = 0.20 e Å3
131 parametersAbsolute structure: Flack x determined using 2494 quotients [(I+)-(I-)]/[(I+)+(I-)] Parsons et al. (2013)
0 restraintsAbsolute structure parameter: 0.011 (11)
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
S10.29353 (4)0.65791 (2)0.59184 (2)0.01687 (4)
O10.56607 (10)0.47315 (6)0.32954 (3)0.01617 (10)
O20.07675 (10)0.65590 (6)0.16589 (4)0.01625 (10)
O30.24892 (10)0.71309 (4)0.08834 (3)0.01128 (8)
N10.29316 (11)0.32887 (5)0.42498 (3)0.00925 (8)
H11N0.230 (3)0.2667 (12)0.4002 (8)0.014*
H12N0.280 (3)0.3155 (11)0.4782 (8)0.014*
H13N0.461 (3)0.3287 (11)0.4122 (7)0.014*
N20.21065 (12)0.55612 (5)0.27617 (3)0.01213 (9)
H2N0.044 (3)0.5631 (11)0.2749 (8)0.015*
C10.37117 (14)0.56727 (6)0.50511 (4)0.01293 (10)
H1D0.4712360.6132180.4655190.016*
H1E0.4750360.4994020.5224920.016*
C20.12412 (13)0.52445 (6)0.46605 (4)0.01108 (9)
H2A0.0289030.5930140.4453080.013*
H2B0.0178120.4864940.5079710.013*
C30.16563 (12)0.43738 (5)0.39633 (3)0.00966 (9)
H30.0033670.4162450.3726060.012*
C40.33345 (12)0.48982 (6)0.32997 (4)0.01035 (9)
C50.34421 (13)0.61524 (6)0.21120 (4)0.01259 (10)
H5A0.4594620.5592600.1837930.015*
H5B0.4489800.6795430.2337240.015*
C60.15608 (12)0.66476 (6)0.15042 (3)0.00962 (9)
C70.59992 (18)0.66260 (8)0.64043 (6)0.02365 (16)
H7A0.6624810.5825650.6485610.035*
H7B0.5841320.7018840.6928820.035*
H7C0.7199970.7059150.6063240.035*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
S10.01555 (8)0.01596 (7)0.01911 (8)0.00057 (6)0.00040 (6)0.00632 (6)
O10.00866 (19)0.0242 (2)0.0157 (2)0.00274 (18)0.00070 (17)0.00795 (19)
O20.00915 (19)0.0230 (2)0.0166 (2)0.00048 (18)0.00041 (16)0.01047 (19)
O30.0129 (2)0.01408 (18)0.00689 (15)0.00366 (14)0.00063 (14)0.00177 (14)
N10.00953 (18)0.01015 (17)0.00807 (17)0.00097 (16)0.00063 (15)0.00075 (14)
N20.0095 (2)0.0172 (2)0.00969 (19)0.00194 (19)0.00069 (17)0.00605 (17)
C10.0123 (2)0.0118 (2)0.0147 (2)0.0001 (2)0.0012 (2)0.00119 (19)
C20.0104 (2)0.0112 (2)0.0117 (2)0.00167 (18)0.00146 (18)0.00075 (18)
C30.0085 (2)0.0115 (2)0.0090 (2)0.00079 (17)0.00053 (16)0.00217 (16)
C40.0096 (2)0.0131 (2)0.00842 (19)0.00101 (18)0.00038 (17)0.00254 (17)
C50.0094 (2)0.0181 (3)0.0103 (2)0.0009 (2)0.00068 (18)0.00519 (19)
C60.0102 (2)0.0109 (2)0.00774 (19)0.00110 (18)0.00008 (16)0.00155 (17)
C70.0228 (4)0.0199 (3)0.0283 (4)0.0025 (3)0.0075 (3)0.0061 (3)
Geometric parameters (Å, º) top
S1—C71.7995 (9)C1—H1D0.9900
S1—C11.8150 (7)C1—H1E0.9900
O1—C41.2365 (8)C2—C31.5379 (9)
O2—C61.2534 (9)C2—H2A0.9900
O3—C61.2635 (8)C2—H2B0.9900
N1—C31.4855 (8)C3—C41.5297 (9)
N1—H11N0.885 (14)C3—H31.0000
N1—H12N0.896 (13)C5—C61.5186 (9)
N1—H13N0.907 (14)C5—H5A0.9900
N2—C41.3342 (8)C5—H5B0.9900
N2—C51.4499 (9)C7—H7A0.9800
N2—H2N0.879 (15)C7—H7B0.9800
C1—C21.5296 (10)C7—H7C0.9800
C7—S1—C199.74 (4)N1—C3—C2111.31 (5)
C3—N1—H11N110.5 (9)C4—C3—C2111.53 (5)
C3—N1—H12N114.9 (8)N1—C3—H3108.9
H11N—N1—H12N106.8 (12)C4—C3—H3108.9
C3—N1—H13N111.5 (8)C2—C3—H3108.9
H11N—N1—H13N105.0 (12)O1—C4—N2124.13 (6)
H12N—N1—H13N107.6 (12)O1—C4—C3120.88 (6)
C4—N2—C5121.62 (6)N2—C4—C3114.95 (6)
C4—N2—H2N123.3 (8)N2—C5—C6110.43 (6)
C5—N2—H2N115.0 (8)N2—C5—H5A109.6
C2—C1—S1108.98 (5)C6—C5—H5A109.6
C2—C1—H1D109.9N2—C5—H5B109.6
S1—C1—H1D109.9C6—C5—H5B109.6
C2—C1—H1E109.9H5A—C5—H5B108.1
S1—C1—H1E109.9O2—C6—O3125.28 (6)
H1D—C1—H1E108.3O2—C6—C5118.01 (5)
C1—C2—C3113.76 (6)O3—C6—C5116.70 (6)
C1—C2—H2A108.8S1—C7—H7A109.5
C3—C2—H2A108.8S1—C7—H7B109.5
C1—C2—H2B108.8H7A—C7—H7B109.5
C3—C2—H2B108.8S1—C7—H7C109.5
H2A—C2—H2B107.7H7A—C7—H7C109.5
N1—C3—C4107.17 (5)H7B—C7—H7C109.5
C7—S1—C1—C2165.35 (5)C2—C3—C4—O193.98 (8)
S1—C1—C2—C3174.71 (4)N1—C3—C4—N2154.05 (6)
C1—C2—C3—N162.23 (7)C2—C3—C4—N283.89 (7)
C1—C2—C3—C457.41 (7)C4—N2—C5—C6169.26 (6)
C5—N2—C4—O10.09 (11)N2—C5—C6—O24.52 (9)
C5—N2—C4—C3177.89 (6)N2—C5—C6—O3176.26 (6)
N1—C3—C4—O128.08 (9)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N1—H11N···O2i0.885 (14)1.854 (14)2.7290 (8)169.5 (13)
N1—H11N···O3i0.885 (14)2.593 (15)3.1465 (8)121.4 (11)
N1—H12N···O3ii0.896 (13)1.857 (13)2.7531 (7)179.6 (14)
N1—H13N···O3iii0.907 (14)2.015 (14)2.7529 (8)137.5 (11)
N1—H13N···O10.907 (14)2.211 (13)2.6940 (8)112.7 (10)
N2—H2N···O20.879 (15)2.185 (13)2.6273 (8)110.6 (10)
Symmetry codes: (i) x, y1/2, z+1/2; (ii) x+1/2, y+1, z+1/2; (iii) x+1, y1/2, z+1/2.
 

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