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Geometric parameters of the title compound, C9H22P+·Cl, are in the usual ranges. Cations and anions are connected by a P—H...Cl hydrogen bond.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536807046417/at2409sup1.cif
Contains datablocks I, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536807046417/at2409Isup2.hkl
Contains datablock I

CCDC reference: 663829

Key indicators

  • Single-crystal X-ray study
  • T = 173 K
  • Mean [sigma](C-C) = 0.002 Å
  • R factor = 0.023
  • wR factor = 0.060
  • Data-to-parameter ratio = 20.9

checkCIF/PLATON results

No syntax errors found



Alert level C PLAT850_ALERT_2_C Check Flack Parameter Exact Value 0.00 and su .. 0.07
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 25.62 From the CIF: _reflns_number_total 2191 Count of symmetry unique reflns 1294 Completeness (_total/calc) 169.32% TEST3: Check Friedels for noncentro structure Estimate of Friedel pairs measured 897 Fraction of Friedel pairs measured 0.693 Are heavy atom types Z>Si present yes
0 ALERT level A = In general: serious problem 0 ALERT level B = Potentially serious problem 1 ALERT level C = Check and explain 1 ALERT level G = General alerts; check 0 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 0 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

Comment top

Very recently, we have reported that treatment of Ph2PCH3 with nBuLi led to the formation of the lithium methanide Li+[CH2PPh2]- (Ruth et al., 2007). Thereby Ph2PCH3 reacts as a Brønsted acid. Here we describe a Lewis-base reaction of tBu2PCH3 with NH4Cl which produces the phosphonium chloride [tBu2PHCH3]+ Cl-. X-ray quality crystals of the title compound have been obtained from a tetrahydrofuran solution at ambient temperature.

The title compound, C9H22P+.Cl-, is composed of di(t-butyl)-methylphosphonium cations and chloride anions. Geometric parameters are in the usual ranges. Cations and anions are connected by a P—H···Cl hydrogen bond.

Related literature top

For related literature, see: Ruth et al. (2007).

Experimental top

At room temperature, 3.5 ml of a 1.0 M solution of NH4Cl in water was added to a solution of 0.05 g (0.31 mmol) tBu2PCH3 in 3 ml pentane and 1 ml Et2O. After removal of the solvent from the organic layer the residue was dissolved in 0.5 ml tetrahydrofuran. Colourless crystals of title compound were grown from this tetrahydrofuran solution at ambient temperature.

Refinement top

H atoms were found in a difference map but those bonded to C were refined with fixed individual displacement parameters [Uiso(H) = 1.5 Ueq(C)] using a riding model with C—H = 0.98 Å. The H atom bonded to P was isotropically refined.

Structure description top

Very recently, we have reported that treatment of Ph2PCH3 with nBuLi led to the formation of the lithium methanide Li+[CH2PPh2]- (Ruth et al., 2007). Thereby Ph2PCH3 reacts as a Brønsted acid. Here we describe a Lewis-base reaction of tBu2PCH3 with NH4Cl which produces the phosphonium chloride [tBu2PHCH3]+ Cl-. X-ray quality crystals of the title compound have been obtained from a tetrahydrofuran solution at ambient temperature.

The title compound, C9H22P+.Cl-, is composed of di(t-butyl)-methylphosphonium cations and chloride anions. Geometric parameters are in the usual ranges. Cations and anions are connected by a P—H···Cl hydrogen bond.

For related literature, see: Ruth et al. (2007).

Computing details top

Data collection: X-AREA (Stoe & Cie, 2001); cell refinement: X-AREA (Stoe & Cie, 2001); data reduction: X-AREA (Stoe & Cie, 2001); program(s) used to solve structure: SHELXS97 (Sheldrick, 1990); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: XP in SHELXTL-Plus (Sheldrick, 1991); software used to prepare material for publication: SHELXL97 (Sheldrick, 1997).

Figures top
[Figure 1] Fig. 1. Perspective view of the title compound with the atom numbering scheme. Displacement ellipsoids are at the 50% probability level. The H bond is drawn as a dashed line.
[Figure 2] Fig. 2. The formation of the title compound.
Di-tert-butylmethylphosphonium chloride top
Crystal data top
C9H22P+·ClF(000) = 432
Mr = 196.69Dx = 1.118 Mg m3
Orthorhombic, P212121Mo Kα radiation, λ = 0.71073 Å
Hall symbol: P 2ac 2abCell parameters from 14606 reflections
a = 7.0601 (6) Åθ = 3.5–25.8°
b = 10.5406 (6) ŵ = 0.41 mm1
c = 15.7074 (10) ÅT = 173 K
V = 1168.91 (14) Å3Block, colourless
Z = 40.42 × 0.37 × 0.35 mm
Data collection top
Stoe IPDSII two-circle
diffractometer
2191 independent reflections
Radiation source: fine-focus sealed tube2138 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.065
ω scansθmax = 25.6°, θmin = 3.5°
Absorption correction: multi-scan
(MULABS; Spek, 2003; Blessing, 1995)
h = 88
Tmin = 0.846, Tmax = 0.869k = 1212
16039 measured reflectionsl = 1918
Refinement top
Refinement on F2Hydrogen site location: inferred from neighbouring sites
Least-squares matrix: fullH atoms treated by a mixture of independent and constrained refinement
R[F2 > 2σ(F2)] = 0.023 w = 1/[σ2(Fo2) + (0.0316P)2 + 0.2388P]
where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.060(Δ/σ)max = 0.001
S = 1.08Δρmax = 0.22 e Å3
2191 reflectionsΔρmin = 0.21 e Å3
105 parametersExtinction correction: SHELXL97 (Sheldrick, 1997), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
0 restraintsExtinction coefficient: 0.021 (2)
Primary atom site location: structure-invariant direct methodsAbsolute structure: Flack (1983), 905 Friedel pairs
Secondary atom site location: difference Fourier mapAbsolute structure parameter: 0.00 (7)
Crystal data top
C9H22P+·ClV = 1168.91 (14) Å3
Mr = 196.69Z = 4
Orthorhombic, P212121Mo Kα radiation
a = 7.0601 (6) ŵ = 0.41 mm1
b = 10.5406 (6) ÅT = 173 K
c = 15.7074 (10) Å0.42 × 0.37 × 0.35 mm
Data collection top
Stoe IPDSII two-circle
diffractometer
2191 independent reflections
Absorption correction: multi-scan
(MULABS; Spek, 2003; Blessing, 1995)
2138 reflections with I > 2σ(I)
Tmin = 0.846, Tmax = 0.869Rint = 0.065
16039 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.023H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.060Δρmax = 0.22 e Å3
S = 1.08Δρmin = 0.21 e Å3
2191 reflectionsAbsolute structure: Flack (1983), 905 Friedel pairs
105 parametersAbsolute structure parameter: 0.00 (7)
0 restraints
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
Cl10.22208 (5)0.43238 (4)0.79852 (3)0.02524 (12)
P10.64522 (5)0.49139 (4)0.65011 (2)0.01714 (11)
H10.512 (3)0.5180 (18)0.7049 (13)0.029 (5)*
C10.7006 (2)0.32277 (14)0.67016 (10)0.0190 (3)
C20.8916 (2)0.28544 (16)0.62979 (11)0.0255 (4)
H2A0.88290.29310.56770.038*
H2B0.92210.19760.64490.038*
H2C0.99130.34190.65100.038*
C30.7165 (3)0.30947 (16)0.76817 (10)0.0253 (3)
H3A0.59530.33240.79450.038*
H3B0.81600.36610.78930.038*
H3C0.74810.22160.78270.038*
C40.5391 (2)0.23663 (16)0.63818 (12)0.0271 (4)
H4A0.41980.26220.66500.041*
H4B0.56710.14830.65290.041*
H4C0.52770.24470.57620.041*
C50.5531 (2)0.53377 (15)0.54320 (10)0.0206 (3)
C60.6720 (2)0.47265 (17)0.47158 (10)0.0284 (4)
H6A0.80450.49900.47730.043*
H6B0.62330.50010.41610.043*
H6C0.66370.38010.47580.043*
C70.5622 (3)0.67927 (16)0.53430 (12)0.0311 (4)
H7A0.48540.71860.57910.047*
H7B0.51300.70420.47840.047*
H7C0.69390.70750.53970.047*
C80.3434 (2)0.49260 (18)0.53649 (11)0.0291 (4)
H8A0.27060.53200.58260.044*
H8B0.33480.40010.54120.044*
H8C0.29190.51970.48150.044*
C90.8495 (3)0.58718 (16)0.67419 (12)0.0303 (4)
H9A0.82020.67660.66330.045*
H9B0.95580.56090.63820.045*
H9C0.88380.57620.73420.045*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Cl10.02263 (18)0.02150 (19)0.0316 (2)0.00030 (15)0.00044 (16)0.00198 (15)
P10.01824 (18)0.01498 (19)0.01820 (19)0.00116 (15)0.00001 (14)0.00105 (14)
C10.0221 (8)0.0142 (7)0.0206 (7)0.0002 (6)0.0004 (6)0.0001 (5)
C20.0263 (9)0.0228 (8)0.0274 (9)0.0063 (7)0.0021 (7)0.0004 (7)
C30.0281 (8)0.0262 (8)0.0216 (8)0.0025 (7)0.0002 (7)0.0035 (6)
C40.0302 (9)0.0197 (8)0.0313 (9)0.0054 (7)0.0058 (8)0.0021 (7)
C50.0223 (7)0.0205 (8)0.0191 (8)0.0006 (6)0.0002 (6)0.0030 (6)
C60.0317 (9)0.0345 (10)0.0191 (7)0.0036 (7)0.0038 (6)0.0013 (6)
C70.0363 (9)0.0221 (9)0.0348 (10)0.0022 (7)0.0027 (8)0.0062 (7)
C80.0229 (7)0.0353 (9)0.0290 (8)0.0007 (8)0.0048 (6)0.0020 (8)
C90.0297 (8)0.0198 (8)0.0413 (10)0.0039 (7)0.0114 (8)0.0002 (7)
Geometric parameters (Å, º) top
P1—C91.8009 (17)C5—C71.541 (2)
P1—C11.8470 (15)C5—C61.544 (2)
P1—C51.8554 (16)C5—C81.546 (2)
P1—H11.308 (19)C6—H6A0.9800
C1—C21.541 (2)C6—H6B0.9800
C1—C41.542 (2)C6—H6C0.9800
C1—C31.550 (2)C7—H7A0.9800
C2—H2A0.9800C7—H7B0.9800
C2—H2B0.9800C7—H7C0.9800
C2—H2C0.9800C8—H8A0.9800
C3—H3A0.9800C8—H8B0.9800
C3—H3B0.9800C8—H8C0.9800
C3—H3C0.9800C9—H9A0.9800
C4—H4A0.9800C9—H9B0.9800
C4—H4B0.9800C9—H9C0.9800
C4—H4C0.9800
C9—P1—C1109.51 (8)C7—C5—C6109.05 (14)
C9—P1—C5109.63 (8)C7—C5—C8108.23 (14)
C1—P1—C5117.40 (7)C6—C5—C8110.71 (14)
C9—P1—H1108.6 (8)C7—C5—P1107.88 (11)
C1—P1—H1104.3 (9)C6—C5—P1111.61 (11)
C5—P1—H1106.9 (8)C8—C5—P1109.25 (11)
C2—C1—C4111.26 (13)C5—C6—H6A109.5
C2—C1—C3108.81 (14)C5—C6—H6B109.5
C4—C1—C3108.89 (13)H6A—C6—H6B109.5
C2—C1—P1111.15 (11)C5—C6—H6C109.5
C4—C1—P1110.76 (11)H6A—C6—H6C109.5
C3—C1—P1105.77 (10)H6B—C6—H6C109.5
C1—C2—H2A109.5C5—C7—H7A109.5
C1—C2—H2B109.5C5—C7—H7B109.5
H2A—C2—H2B109.5H7A—C7—H7B109.5
C1—C2—H2C109.5C5—C7—H7C109.5
H2A—C2—H2C109.5H7A—C7—H7C109.5
H2B—C2—H2C109.5H7B—C7—H7C109.5
C1—C3—H3A109.5C5—C8—H8A109.5
C1—C3—H3B109.5C5—C8—H8B109.5
H3A—C3—H3B109.5H8A—C8—H8B109.5
C1—C3—H3C109.5C5—C8—H8C109.5
H3A—C3—H3C109.5H8A—C8—H8C109.5
H3B—C3—H3C109.5H8B—C8—H8C109.5
C1—C4—H4A109.5P1—C9—H9A109.5
C1—C4—H4B109.5P1—C9—H9B109.5
H4A—C4—H4B109.5H9A—C9—H9B109.5
C1—C4—H4C109.5P1—C9—H9C109.5
H4A—C4—H4C109.5H9A—C9—H9C109.5
H4B—C4—H4C109.5H9B—C9—H9C109.5
C9—P1—C1—C247.69 (14)C9—P1—C5—C741.13 (14)
C5—P1—C1—C278.12 (13)C1—P1—C5—C7166.88 (11)
C9—P1—C1—C4171.92 (12)C9—P1—C5—C678.65 (13)
C5—P1—C1—C446.11 (14)C1—P1—C5—C647.10 (14)
C9—P1—C1—C370.25 (13)C9—P1—C5—C8158.57 (12)
C5—P1—C1—C3163.93 (10)C1—P1—C5—C875.67 (13)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
P1—H1···Cl11.308 (19)2.675 (19)3.8400 (6)147.2 (12)

Experimental details

Crystal data
Chemical formulaC9H22P+·Cl
Mr196.69
Crystal system, space groupOrthorhombic, P212121
Temperature (K)173
a, b, c (Å)7.0601 (6), 10.5406 (6), 15.7074 (10)
V3)1168.91 (14)
Z4
Radiation typeMo Kα
µ (mm1)0.41
Crystal size (mm)0.42 × 0.37 × 0.35
Data collection
DiffractometerStoe IPDSII two-circle
Absorption correctionMulti-scan
(MULABS; Spek, 2003; Blessing, 1995)
Tmin, Tmax0.846, 0.869
No. of measured, independent and
observed [I > 2σ(I)] reflections
16039, 2191, 2138
Rint0.065
(sin θ/λ)max1)0.608
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.023, 0.060, 1.08
No. of reflections2191
No. of parameters105
H-atom treatmentH atoms treated by a mixture of independent and constrained refinement
Δρmax, Δρmin (e Å3)0.22, 0.21
Absolute structureFlack (1983), 905 Friedel pairs
Absolute structure parameter0.00 (7)

Computer programs: X-AREA (Stoe & Cie, 2001), SHELXS97 (Sheldrick, 1990), SHELXL97 (Sheldrick, 1997), XP in SHELXTL-Plus (Sheldrick, 1991).

Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
P1—H1···Cl11.308 (19)2.675 (19)3.8400 (6)147.2 (12)
 

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