Buy article online - an online subscription or single-article purchase is required to access this article.
Download citation
Download citation
link to html
A new substance, cis-amminedibromido(2-methyl­pyridine-κN)platinum(II), cis-[PtBr2(C6H7N)(NH3)], which is a potential platinum-based anti­neoplastic agent for the treatment of patients with solid tumors, has been synthesized and structurally characterized. There is one mol­ecule in the asymmetric unit and mol­ecules are linked via two symmetry-independent N—H...Br hydrogen bonds into zigzag chains running parallel to the c axis. C—H...Br hydrogen bonds crosslink these chains to give a layer parallel to (010). N—H...Br hydrogen bonds and π–π stacking inter­actions between pairs of pyridine rings stack the layers along b.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S0108270113004708/ln3155sup1.cif
Contains datablocks global, PicoPtBr2

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108270113004708/ln3155PicoPtBr2sup2.hkl
Contains datablock PicoPtBr2

CCDC reference: 934593

Computing details top

Data collection: CrysAlis PRO (Agilent, 2011); cell refinement: CrysAlis PRO (Agilent, 2011); data reduction: CrysAlis PRO (Agilent, 2011); program(s) used to solve structure: SUPERFLIP (Palatinus & Chapuis, 2007); program(s) used to refine structure: JANA2006 (Petříček et al., 2006); molecular graphics: ORTEP-3 (Farrugia, 2012) and Mercury (Macrae et al., 2006); software used to prepare material for publication: JANA2006 (Petříček et al., 2006).

cis-amminedibromido(2-methylpyridine-κN)platinum(II) top
Crystal data top
[PtBr2(C6H7N)(NH3)]F(000) = 832
Mr = 465Dx = 3.018 Mg m3
Monoclinic, P21/cCu Kα radiation, λ = 1.5418 Å
Hall symbol: -P 2ybcCell parameters from 13149 reflections
a = 10.0371 (3) Åθ = 4.5–77.0°
b = 9.0733 (3) ŵ = 34.36 mm1
c = 11.4901 (4) ÅT = 190 K
β = 102.120 (3)°Block, yellow
V = 1023.07 (6) Å30.23 × 0.17 × 0.10 mm
Z = 4
Data collection top
Oxford Diffraction Xcalibur
diffractometer with an Onyx detector
2148 independent reflections
Radiation source: Enhance (Cu) X-ray Source1822 reflections with I > 3σ(I)
Graphite monochromatorRint = 0.090
Detector resolution: 8.1917 pixels mm-1θmax = 77.3°, θmin = 4.5°
ω scansh = 1212
Absorption correction: multi-scan
[CrysAlis PRO (Agilent, 2011) using spherical harminics]
k = 1111
Tmin = 0.212, Tmax = 1l = 1414
25523 measured reflections
Refinement top
Refinement on F40 constraints
R[F > 3σ(F)] = 0.030H-atom parameters constrained
wR(F) = 0.036Weighting scheme based on measured s.u.'s w = 1/(σ2(F) + 0.0001F2)
S = 1.69(Δ/σ)max = 0.013
2148 reflectionsΔρmax = 1.35 e Å3
100 parametersΔρmin = 2.43 e Å3
0 restraints
Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Pt10.37243 (3)0.67977 (3)0.19269 (2)0.01751 (9)
Br10.25429 (7)0.54401 (9)0.32423 (7)0.0241 (2)
Br20.58974 (7)0.67033 (10)0.33290 (7)0.0292 (2)
N10.1947 (6)0.6881 (6)0.0673 (5)0.0197 (17)
N20.4656 (7)0.8066 (7)0.0871 (6)0.031 (2)
C20.0253 (8)0.7924 (10)0.0069 (8)0.037 (3)
C40.0498 (7)0.6082 (9)0.1112 (7)0.026 (2)
C60.2841 (8)0.5045 (9)0.0506 (7)0.033 (3)
C30.0517 (8)0.7047 (9)0.0912 (8)0.037 (3)
C50.1741 (7)0.6022 (8)0.0307 (6)0.022 (2)
C10.0980 (8)0.7816 (9)0.0853 (7)0.033 (3)
H1c20.092480.8614250.021280.0444*
H1c40.0336810.5462790.1804660.0312*
H1c60.2466210.4286010.1061090.0395*
H3c60.3494940.5606230.0820710.0395*
H2c60.3279470.4603250.0235370.0395*
H1c30.1384230.7089380.1457110.0443*
H1c10.1153070.8428990.1549750.0396*
H1n20.4967370.7504710.0374250.0377*
H3n20.4072110.8688090.0476420.0377*
H2n20.5328220.8545640.1311170.0377*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Pt10.01468 (14)0.02128 (15)0.01572 (16)0.00189 (12)0.00125 (10)0.00082 (12)
Br10.0180 (3)0.0318 (4)0.0222 (4)0.0043 (3)0.0033 (3)0.0025 (3)
Br20.0171 (3)0.0461 (5)0.0218 (4)0.0092 (3)0.0018 (3)0.0026 (4)
N10.023 (3)0.018 (3)0.018 (3)0.003 (2)0.003 (2)0.002 (2)
N20.031 (3)0.035 (4)0.028 (4)0.008 (3)0.005 (3)0.007 (3)
C20.020 (4)0.041 (5)0.049 (5)0.013 (4)0.006 (4)0.002 (4)
C40.017 (3)0.036 (4)0.024 (4)0.007 (3)0.003 (3)0.004 (3)
C60.032 (4)0.032 (4)0.034 (5)0.008 (4)0.005 (4)0.008 (4)
C30.020 (4)0.041 (5)0.046 (5)0.002 (3)0.000 (4)0.010 (4)
C50.023 (3)0.025 (4)0.018 (3)0.002 (3)0.004 (3)0.003 (3)
C10.032 (4)0.035 (4)0.031 (4)0.013 (4)0.005 (3)0.003 (4)
Geometric parameters (Å, º) top
Pt1—Br12.4414 (9)N2—H2n20.87
Pt1—Br22.4258 (7)C2—C31.360 (13)
Pt1—N12.045 (5)C2—C11.373 (11)
Pt1—N22.037 (7)C2—H1c20.96
Br1—N13.169 (6)C4—C31.399 (12)
Br1—N2i3.518 (7)C4—C51.389 (9)
Br1—N2ii3.574 (6)C4—H1c40.96
Br2—N23.095 (6)C6—C51.471 (12)
Br2—N2i3.502 (7)C6—H1c60.96
Br2—N2ii3.414 (7)C6—H3c60.96
N1—C51.349 (9)C6—H2c60.96
N1—C11.338 (11)C3—H1c30.96
N2—H1n20.87C1—H1c10.96
N2—H3n20.87
Br1—Pt1—Br293.26 (3)Br1iv—N2—Br2iv60.79 (11)
Br1—Pt1—N189.42 (18)Br1iv—N2—H1n284.17
Br1—Pt1—N2175.9 (2)Br1iv—N2—H3n225.53
Br2—Pt1—N1176.94 (18)Br1iv—N2—H2n2123.47
Br2—Pt1—N287.37 (18)Br2—N2—Br2iii101.10 (18)
N1—Pt1—N290.1 (2)Br2—N2—Br2iv131.0 (2)
Pt1—Br1—N140.20 (11)Br2—N2—H1n2103.53
Pt1—Br1—N2i91.48 (12)Br2—N2—H3n2146.4
Pt1—Br1—N2ii93.01 (12)Br2—N2—H2n263.59
N1—Br1—N2i120.35 (16)Br2iii—N2—Br2iv105.86 (18)
N1—Br1—N2ii126.39 (15)Br2iii—N2—H1n2145.3
N2i—Br1—N2ii72.01 (15)Br2iii—N2—H3n252.99
Pt1—Br2—N241.10 (13)Br2iii—N2—H2n261.44
Pt1—Br2—N2i92.15 (11)Br2iv—N2—H1n239.57
Pt1—Br2—N2ii97.31 (11)Br2iv—N2—H3n280.88
N2—Br2—N2i124.08 (16)Br2iv—N2—H2n295.12
N2—Br2—N2ii127.37 (18)H1n2—N2—H3n2109.47
N2i—Br2—N2ii74.14 (16)H1n2—N2—H2n2109.47
Pt1—N1—Br150.38 (12)H3n2—N2—H2n2109.47
Pt1—N1—C5121.7 (5)C3—C2—C1119.7 (8)
Pt1—N1—C1117.9 (5)C3—C2—H1c2120.17
Br1—N1—C5120.3 (4)C1—C2—H1c2120.17
Br1—N1—C196.8 (5)C3—C4—C5119.9 (7)
C5—N1—C1120.4 (6)C3—C4—H1c4120.04
Pt1—N2—Br1iii127.8 (3)C5—C4—H1c4120.03
Pt1—N2—Br1iv116.9 (3)C5—C6—H1c6109.47
Pt1—N2—Br251.53 (14)C5—C6—H3c6109.47
Pt1—N2—Br2iii104.9 (3)C5—C6—H2c6109.47
Pt1—N2—Br2iv147.2 (3)H1c6—C6—H3c6109.47
Pt1—N2—H1n2109.47H1c6—C6—H2c6109.47
Pt1—N2—H3n2109.47H3c6—C6—H2c6109.47
Pt1—N2—H2n2109.47C2—C3—C4118.7 (7)
Br1iii—N2—Br1iv107.99 (18)C2—C3—H1c3120.66
Br1iii—N2—Br280.58 (14)C4—C3—H1c3120.66
Br1iii—N2—Br2iii60.53 (11)N1—C5—C4119.5 (7)
Br1iii—N2—Br2iv78.31 (16)N1—C5—C6119.3 (6)
Br1iii—N2—H1n299.98C4—C5—C6121.3 (7)
Br1iii—N2—H3n299.42N1—C1—C2121.8 (8)
Br1iii—N2—H2n218.3N1—C1—H1c1119.1
Br1iv—N2—Br2167.6 (3)C2—C1—H1c1119.1
Br1iv—N2—Br2iii76.44 (13)
Symmetry codes: (i) x+1, y1/2, z+1/2; (ii) x, y+3/2, z+1/2; (iii) x+1, y+1/2, z+1/2; (iv) x, y+3/2, z1/2.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N2—H1N2···Br2iv0.872.803.414 (7)129
N2—H3N2···Br1iv0.872.813.574 (6)147
C3—H1C3···Br2v0.962.903.698 (8)141
N2—H3N2···Br2iii0.873.063.502 (7)114
N2—H2N2···Br1iii0.872.713.518 (7)156
Symmetry codes: (iii) x+1, y+1/2, z+1/2; (iv) x, y+3/2, z1/2; (v) x1, y+3/2, z1/2.
 

Subscribe to Acta Crystallographica Section C: Structural Chemistry

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