Buy article online - an online subscription or single-article purchase is required to access this article.
Download citation
Download citation
link to html
N-(3-Phenyl­prop­yl)guanidinium bromide, C10H16N3+·Br, was synthesized by the reaction of 2-ethyl-2-pseudourea hydro­bromide with 3-phenyl-1-propyl­amine. N—H...Br hydrogen bonds stabilize the bromide anions in channels along the c axis.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S160053680701238X/hg2211sup1.cif
Contains datablocks global, I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S160053680701238X/hg2211Isup2.hkl
Contains datablock I

CCDC reference: 643030

Key indicators

  • Single-crystal X-ray study
  • T = 100 K
  • Mean [sigma](C-C) = 0.013 Å
  • R factor = 0.058
  • wR factor = 0.141
  • Data-to-parameter ratio = 21.3

checkCIF/PLATON results

No syntax errors found



Alert level C PLAT061_ALERT_3_C Tmax/Tmin Range Test RR' too Large ............. 0.88 PLAT094_ALERT_2_C Ratio of Maximum / Minimum Residual Density .... 2.78 PLAT152_ALERT_1_C Supplied and Calc Volume s.u. Inconsistent ..... ? PLAT341_ALERT_3_C Low Bond Precision on C-C bonds (x 1000) Ang ... 13
Alert level G REFLT03_ALERT_4_G Please check that the estimate of the number of Friedel pairs is correct. If it is not, please give the correct count in the _publ_section_exptl_refinement section of the submitted CIF. From the CIF: _diffrn_reflns_theta_max 28.25 From the CIF: _reflns_number_total 2724 Count of symmetry unique reflns 1489 Completeness (_total/calc) 182.94% TEST3: Check Friedels for noncentro structure Estimate of Friedel pairs measured 1235 Fraction of Friedel pairs measured 0.829 Are heavy atom types Z>Si present yes
0 ALERT level A = In general: serious problem 0 ALERT level B = Potentially serious problem 4 ALERT level C = Check and explain 1 ALERT level G = General alerts; check 1 ALERT type 1 CIF construction/syntax error, inconsistent or missing data 1 ALERT type 2 Indicator that the structure model may be wrong or deficient 2 ALERT type 3 Indicator that the structure quality may be low 1 ALERT type 4 Improvement, methodology, query or suggestion 0 ALERT type 5 Informative message, check

Computing details top

Data collection: SMART (Bruker, 2002); cell refinement: SAINT-Plus (Bruker, 2003); data reduction: SAINT-Plus; program(s) used to solve structure: SHELXTL (Bruker, 2003); program(s) used to refine structure: SHELXTL; molecular graphics: SHELXTL; software used to prepare material for publication: SHELXTL.

N-(3-Phenylpropyl)guanidinium bromide top
Crystal data top
C10H16N3+·BrF(000) = 528
Mr = 258.17Dx = 1.429 Mg m3
Monoclinic, CcMo Kα radiation, λ = 0.71073 Å
Hall symbol: C -2ycCell parameters from 5032 reflections
a = 10.5205 (18) Åθ = 2.7–30.5°
b = 11.784 (2) ŵ = 3.40 mm1
c = 10.3702 (17) ÅT = 100 K
β = 111.056 (3)°Plate, colorless
V = 1199.8 (3) Å30.33 × 0.23 × 0.02 mm
Z = 4
Data collection top
Bruker SMART APEX CCD
diffractometer
2724 independent reflections
Radiation source: fine-focus sealed tube2501 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.052
ω scansθmax = 28.3°, θmin = 2.7°
Absorption correction: multi-scan
(SADABS in SAINT-Plus; Bruker, 2003)
h = 1314
Tmin = 0.299, Tmax = 0.934k = 1515
5112 measured reflectionsl = 1313
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.058H-atom parameters constrained
wR(F2) = 0.141 w = 1/[σ2(Fo2) + (0.0309P)2 + 7.8027P]
where P = (Fo2 + 2Fc2)/3
S = 1.14(Δ/σ)max < 0.001
2724 reflectionsΔρmax = 2.19 e Å3
128 parametersΔρmin = 0.79 e Å3
2 restraintsAbsolute structure: Flack (1983), 1246 Friedel pairs
Primary atom site location: structure-invariant direct methodsAbsolute structure parameter: 0.09 (3)
Special details top

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

Refinement. Refinement of F2 against ALL reflections. The weighted R-factor wR and goodness of fit S are based on F2, conventional R-factors R are based on F, with F set to zero for negative F2. The threshold expression of F2 > σ(F2) is used only for calculating R-factors(gt) etc. and is not relevant to the choice of reflections for refinement. R-factors based on F2 are statistically about twice as large as those based on F, and R- factors based on ALL data will be even larger.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Br10.71055 (8)0.87770 (5)0.18953 (8)0.02567 (18)
C10.3989 (7)0.3219 (5)0.5799 (7)0.0221 (13)
C20.4699 (7)0.3874 (6)0.8195 (7)0.0245 (14)
H2A0.38620.36790.83740.029*
H2B0.46380.46810.79140.029*
C30.5931 (10)0.3703 (6)0.9501 (8)0.0237 (16)
H3A0.67610.39510.93410.028*
H3B0.60310.28870.97430.028*
C40.5783 (8)0.4381 (7)1.0694 (9)0.0316 (16)
H4A0.57260.51981.04600.038*
H4B0.49210.41621.08080.038*
C50.6925 (8)0.4200 (6)1.2018 (9)0.0241 (17)
C60.6836 (9)0.3459 (7)1.3034 (8)0.0331 (17)
H60.60160.30471.28690.040*
C70.7898 (12)0.3308 (9)1.4260 (9)0.040 (2)
H70.78080.27781.49120.048*
C80.9082 (11)0.3904 (8)1.4565 (9)0.040 (2)
H80.98050.38111.54280.048*
C90.9203 (9)0.4651 (8)1.3575 (9)0.0374 (18)
H91.00240.50671.37590.045*
C100.8159 (8)0.4793 (7)1.2346 (9)0.0327 (16)
H100.82680.53091.16900.039*
N10.2952 (6)0.3952 (4)0.5380 (6)0.0213 (11)
H1A0.28030.44110.59790.026*
H1B0.24180.39750.45040.026*
N20.4190 (6)0.2529 (5)0.4873 (6)0.0253 (12)
H2C0.48670.20400.51340.030*
H2D0.36470.25630.40020.030*
N30.4797 (6)0.3163 (5)0.7087 (6)0.0215 (12)
H30.54550.26560.73050.026*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Br10.0275 (3)0.0243 (3)0.0219 (3)0.0115 (4)0.0049 (2)0.0053 (4)
C10.019 (3)0.016 (3)0.030 (4)0.003 (2)0.007 (3)0.000 (3)
C20.025 (3)0.023 (3)0.026 (4)0.004 (3)0.009 (3)0.004 (3)
C30.027 (4)0.022 (4)0.018 (4)0.005 (3)0.003 (3)0.007 (3)
C40.033 (4)0.032 (4)0.031 (4)0.012 (3)0.012 (4)0.003 (3)
C50.016 (4)0.033 (3)0.019 (4)0.006 (3)0.002 (3)0.005 (3)
C60.041 (4)0.030 (4)0.032 (4)0.001 (3)0.018 (4)0.005 (3)
C70.063 (7)0.037 (5)0.020 (4)0.011 (5)0.013 (4)0.001 (4)
C80.043 (5)0.042 (5)0.026 (5)0.016 (4)0.002 (4)0.011 (4)
C90.031 (4)0.045 (5)0.038 (5)0.005 (4)0.015 (4)0.010 (4)
C100.033 (4)0.034 (4)0.033 (4)0.001 (3)0.014 (4)0.004 (3)
N10.022 (3)0.017 (3)0.020 (3)0.002 (2)0.002 (2)0.002 (2)
N20.027 (3)0.023 (3)0.022 (3)0.005 (2)0.003 (3)0.002 (2)
N30.021 (3)0.015 (3)0.027 (3)0.007 (2)0.006 (2)0.001 (2)
Geometric parameters (Å, º) top
C1—N31.302 (9)C6—C71.369 (13)
C1—N21.331 (9)C6—H60.9500
C1—N11.335 (9)C7—C81.364 (15)
C2—N31.455 (9)C7—H70.9500
C2—C31.515 (11)C8—C91.393 (14)
C2—H2A0.9900C8—H80.9500
C2—H2B0.9900C9—C101.361 (13)
C3—C41.527 (11)C9—H90.9500
C3—H3A0.9900C10—H100.9500
C3—H3B0.9900N1—H1A0.8800
C4—C51.480 (13)N1—H1B0.8800
C4—H4A0.9900N2—H2C0.8800
C4—H4B0.9900N2—H2D0.8800
C5—C61.398 (11)N3—H30.8800
C5—C101.404 (11)
N3—C1—N2119.6 (6)C7—C6—C5121.8 (8)
N3—C1—N1121.5 (6)C7—C6—H6119.1
N2—C1—N1118.9 (6)C5—C6—H6119.1
N3—C2—C3110.4 (6)C8—C7—C6121.4 (9)
N3—C2—H2A109.6C8—C7—H7119.3
C3—C2—H2A109.6C6—C7—H7119.3
N3—C2—H2B109.6C7—C8—C9118.2 (9)
C3—C2—H2B109.6C7—C8—H8120.9
H2A—C2—H2B108.1C9—C8—H8120.9
C2—C3—C4110.5 (7)C10—C9—C8120.7 (9)
C2—C3—H3A109.5C10—C9—H9119.6
C4—C3—H3A109.5C8—C9—H9119.6
C2—C3—H3B109.5C9—C10—C5122.1 (9)
C4—C3—H3B109.5C9—C10—H10119.0
H3A—C3—H3B108.1C5—C10—H10119.0
C5—C4—C3113.0 (6)C1—N1—H1A120.0
C5—C4—H4A109.0C1—N1—H1B120.0
C3—C4—H4A109.0H1A—N1—H1B120.0
C5—C4—H4B109.0C1—N2—H2C120.0
C3—C4—H4B109.0C1—N2—H2D120.0
H4A—C4—H4B107.8H2C—N2—H2D120.0
C6—C5—C10115.8 (8)C1—N3—C2125.1 (6)
C6—C5—C4122.5 (7)C1—N3—H3117.4
C10—C5—C4121.7 (7)C2—N3—H3117.4
N3—C2—C3—C4175.9 (6)C7—C8—C9—C100.9 (12)
C2—C3—C4—C5177.0 (6)C8—C9—C10—C50.1 (11)
C3—C4—C5—C699.5 (8)C6—C5—C10—C90.2 (10)
C3—C4—C5—C1082.4 (9)C4—C5—C10—C9178.5 (7)
C10—C5—C6—C71.1 (11)N2—C1—N3—C2179.3 (6)
C4—C5—C6—C7179.4 (7)N1—C1—N3—C21.0 (10)
C5—C6—C7—C82.0 (13)C3—C2—N3—C1171.0 (6)
C6—C7—C8—C91.8 (13)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N1—H1A···Br1i0.882.553.382 (5)158
N1—H1B···Br1ii0.882.623.403 (6)149
N2—H2C···Br1iii0.882.593.399 (6)153
N2—H2D···Br1ii0.882.633.412 (6)149
N3—H3···Br1iii0.882.563.393 (5)157
Symmetry codes: (i) x1/2, y+3/2, z+1/2; (ii) x1/2, y1/2, z; (iii) x, y+1, z+1/2.
 

Subscribe to Acta Crystallographica Section E: Crystallographic Communications

The full text of this article is available to subscribers to the journal.

If you have already registered and are using a computer listed in your registration details, please email support@iucr.org for assistance.

Buy online

You may purchase this article in PDF and/or HTML formats. For purchasers in the European Community who do not have a VAT number, VAT will be added at the local rate. Payments to the IUCr are handled by WorldPay, who will accept payment by credit card in several currencies. To purchase the article, please complete the form below (fields marked * are required), and then click on `Continue'.
E-mail address* 
Repeat e-mail address* 
(for error checking) 

Format*   PDF (US $40)
   HTML (US $40)
   PDF+HTML (US $50)
In order for VAT to be shown for your country javascript needs to be enabled.

VAT number 
(non-UK EC countries only) 
Country* 
 

Terms and conditions of use
Contact us

Follow Acta Cryst. E
Sign up for e-alerts
Follow Acta Cryst. on Twitter
Follow us on facebook
Sign up for RSS feeds