Supporting information
Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536807046417/at2409sup1.cif | |
Structure factor file (CIF format) https://doi.org/10.1107/S1600536807046417/at2409Isup2.hkl |
CCDC reference: 663829
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.
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.
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).
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).
C9H22P+·Cl− | F(000) = 432 |
Mr = 196.69 | Dx = 1.118 Mg m−3 |
Orthorhombic, P212121 | Mo Kα radiation, λ = 0.71073 Å |
Hall symbol: P 2ac 2ab | Cell parameters from 14606 reflections |
a = 7.0601 (6) Å | θ = 3.5–25.8° |
b = 10.5406 (6) Å | µ = 0.41 mm−1 |
c = 15.7074 (10) Å | T = 173 K |
V = 1168.91 (14) Å3 | Block, colourless |
Z = 4 | 0.42 × 0.37 × 0.35 mm |
Stoe IPDSII two-circle diffractometer | 2191 independent reflections |
Radiation source: fine-focus sealed tube | 2138 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.065 |
ω scans | θmax = 25.6°, θmin = 3.5° |
Absorption correction: multi-scan (MULABS; Spek, 2003; Blessing, 1995) | h = −8→8 |
Tmin = 0.846, Tmax = 0.869 | k = −12→12 |
16039 measured reflections | l = −19→18 |
Refinement on F2 | Hydrogen site location: inferred from neighbouring sites |
Least-squares matrix: full | H 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 = 1.08 | Δρmax = 0.22 e Å−3 |
2191 reflections | Δρmin = −0.21 e Å−3 |
105 parameters | Extinction correction: SHELXL97 (Sheldrick, 1997), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4 |
0 restraints | Extinction coefficient: 0.021 (2) |
Primary atom site location: structure-invariant direct methods | Absolute structure: Flack (1983), 905 Friedel pairs |
Secondary atom site location: difference Fourier map | Absolute structure parameter: 0.00 (7) |
C9H22P+·Cl− | V = 1168.91 (14) Å3 |
Mr = 196.69 | Z = 4 |
Orthorhombic, P212121 | Mo Kα radiation |
a = 7.0601 (6) Å | µ = 0.41 mm−1 |
b = 10.5406 (6) Å | T = 173 K |
c = 15.7074 (10) Å | 0.42 × 0.37 × 0.35 mm |
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 = 0.869 | Rint = 0.065 |
16039 measured reflections |
R[F2 > 2σ(F2)] = 0.023 | H atoms treated by a mixture of independent and constrained refinement |
wR(F2) = 0.060 | Δρmax = 0.22 e Å−3 |
S = 1.08 | Δρmin = −0.21 e Å−3 |
2191 reflections | Absolute structure: Flack (1983), 905 Friedel pairs |
105 parameters | Absolute structure parameter: 0.00 (7) |
0 restraints |
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. |
x | y | z | Uiso*/Ueq | ||
Cl1 | 0.22208 (5) | 0.43238 (4) | 0.79852 (3) | 0.02524 (12) | |
P1 | 0.64522 (5) | 0.49139 (4) | 0.65011 (2) | 0.01714 (11) | |
H1 | 0.512 (3) | 0.5180 (18) | 0.7049 (13) | 0.029 (5)* | |
C1 | 0.7006 (2) | 0.32277 (14) | 0.67016 (10) | 0.0190 (3) | |
C2 | 0.8916 (2) | 0.28544 (16) | 0.62979 (11) | 0.0255 (4) | |
H2A | 0.8829 | 0.2931 | 0.5677 | 0.038* | |
H2B | 0.9221 | 0.1976 | 0.6449 | 0.038* | |
H2C | 0.9913 | 0.3419 | 0.6510 | 0.038* | |
C3 | 0.7165 (3) | 0.30947 (16) | 0.76817 (10) | 0.0253 (3) | |
H3A | 0.5953 | 0.3324 | 0.7945 | 0.038* | |
H3B | 0.8160 | 0.3661 | 0.7893 | 0.038* | |
H3C | 0.7481 | 0.2216 | 0.7827 | 0.038* | |
C4 | 0.5391 (2) | 0.23663 (16) | 0.63818 (12) | 0.0271 (4) | |
H4A | 0.4198 | 0.2622 | 0.6650 | 0.041* | |
H4B | 0.5671 | 0.1483 | 0.6529 | 0.041* | |
H4C | 0.5277 | 0.2447 | 0.5762 | 0.041* | |
C5 | 0.5531 (2) | 0.53377 (15) | 0.54320 (10) | 0.0206 (3) | |
C6 | 0.6720 (2) | 0.47265 (17) | 0.47158 (10) | 0.0284 (4) | |
H6A | 0.8045 | 0.4990 | 0.4773 | 0.043* | |
H6B | 0.6233 | 0.5001 | 0.4161 | 0.043* | |
H6C | 0.6637 | 0.3801 | 0.4758 | 0.043* | |
C7 | 0.5622 (3) | 0.67927 (16) | 0.53430 (12) | 0.0311 (4) | |
H7A | 0.4854 | 0.7186 | 0.5791 | 0.047* | |
H7B | 0.5130 | 0.7042 | 0.4784 | 0.047* | |
H7C | 0.6939 | 0.7075 | 0.5397 | 0.047* | |
C8 | 0.3434 (2) | 0.49260 (18) | 0.53649 (11) | 0.0291 (4) | |
H8A | 0.2706 | 0.5320 | 0.5826 | 0.044* | |
H8B | 0.3348 | 0.4001 | 0.5412 | 0.044* | |
H8C | 0.2919 | 0.5197 | 0.4815 | 0.044* | |
C9 | 0.8495 (3) | 0.58718 (16) | 0.67419 (12) | 0.0303 (4) | |
H9A | 0.8202 | 0.6766 | 0.6633 | 0.045* | |
H9B | 0.9558 | 0.5609 | 0.6382 | 0.045* | |
H9C | 0.8838 | 0.5762 | 0.7342 | 0.045* |
U11 | U22 | U33 | U12 | U13 | U23 | |
Cl1 | 0.02263 (18) | 0.02150 (19) | 0.0316 (2) | −0.00030 (15) | 0.00044 (16) | −0.00198 (15) |
P1 | 0.01824 (18) | 0.01498 (19) | 0.01820 (19) | 0.00116 (15) | 0.00001 (14) | −0.00105 (14) |
C1 | 0.0221 (8) | 0.0142 (7) | 0.0206 (7) | 0.0002 (6) | −0.0004 (6) | 0.0001 (5) |
C2 | 0.0263 (9) | 0.0228 (8) | 0.0274 (9) | 0.0063 (7) | 0.0021 (7) | −0.0004 (7) |
C3 | 0.0281 (8) | 0.0262 (8) | 0.0216 (8) | 0.0025 (7) | 0.0002 (7) | 0.0035 (6) |
C4 | 0.0302 (9) | 0.0197 (8) | 0.0313 (9) | −0.0054 (7) | −0.0058 (8) | 0.0021 (7) |
C5 | 0.0223 (7) | 0.0205 (8) | 0.0191 (8) | 0.0006 (6) | −0.0002 (6) | 0.0030 (6) |
C6 | 0.0317 (9) | 0.0345 (10) | 0.0191 (7) | 0.0036 (7) | 0.0038 (6) | 0.0013 (6) |
C7 | 0.0363 (9) | 0.0221 (9) | 0.0348 (10) | 0.0022 (7) | −0.0027 (8) | 0.0062 (7) |
C8 | 0.0229 (7) | 0.0353 (9) | 0.0290 (8) | −0.0007 (8) | −0.0048 (6) | 0.0020 (8) |
C9 | 0.0297 (8) | 0.0198 (8) | 0.0413 (10) | −0.0039 (7) | −0.0114 (8) | 0.0002 (7) |
P1—C9 | 1.8009 (17) | C5—C7 | 1.541 (2) |
P1—C1 | 1.8470 (15) | C5—C6 | 1.544 (2) |
P1—C5 | 1.8554 (16) | C5—C8 | 1.546 (2) |
P1—H1 | 1.308 (19) | C6—H6A | 0.9800 |
C1—C2 | 1.541 (2) | C6—H6B | 0.9800 |
C1—C4 | 1.542 (2) | C6—H6C | 0.9800 |
C1—C3 | 1.550 (2) | C7—H7A | 0.9800 |
C2—H2A | 0.9800 | C7—H7B | 0.9800 |
C2—H2B | 0.9800 | C7—H7C | 0.9800 |
C2—H2C | 0.9800 | C8—H8A | 0.9800 |
C3—H3A | 0.9800 | C8—H8B | 0.9800 |
C3—H3B | 0.9800 | C8—H8C | 0.9800 |
C3—H3C | 0.9800 | C9—H9A | 0.9800 |
C4—H4A | 0.9800 | C9—H9B | 0.9800 |
C4—H4B | 0.9800 | C9—H9C | 0.9800 |
C4—H4C | 0.9800 | ||
C9—P1—C1 | 109.51 (8) | C7—C5—C6 | 109.05 (14) |
C9—P1—C5 | 109.63 (8) | C7—C5—C8 | 108.23 (14) |
C1—P1—C5 | 117.40 (7) | C6—C5—C8 | 110.71 (14) |
C9—P1—H1 | 108.6 (8) | C7—C5—P1 | 107.88 (11) |
C1—P1—H1 | 104.3 (9) | C6—C5—P1 | 111.61 (11) |
C5—P1—H1 | 106.9 (8) | C8—C5—P1 | 109.25 (11) |
C2—C1—C4 | 111.26 (13) | C5—C6—H6A | 109.5 |
C2—C1—C3 | 108.81 (14) | C5—C6—H6B | 109.5 |
C4—C1—C3 | 108.89 (13) | H6A—C6—H6B | 109.5 |
C2—C1—P1 | 111.15 (11) | C5—C6—H6C | 109.5 |
C4—C1—P1 | 110.76 (11) | H6A—C6—H6C | 109.5 |
C3—C1—P1 | 105.77 (10) | H6B—C6—H6C | 109.5 |
C1—C2—H2A | 109.5 | C5—C7—H7A | 109.5 |
C1—C2—H2B | 109.5 | C5—C7—H7B | 109.5 |
H2A—C2—H2B | 109.5 | H7A—C7—H7B | 109.5 |
C1—C2—H2C | 109.5 | C5—C7—H7C | 109.5 |
H2A—C2—H2C | 109.5 | H7A—C7—H7C | 109.5 |
H2B—C2—H2C | 109.5 | H7B—C7—H7C | 109.5 |
C1—C3—H3A | 109.5 | C5—C8—H8A | 109.5 |
C1—C3—H3B | 109.5 | C5—C8—H8B | 109.5 |
H3A—C3—H3B | 109.5 | H8A—C8—H8B | 109.5 |
C1—C3—H3C | 109.5 | C5—C8—H8C | 109.5 |
H3A—C3—H3C | 109.5 | H8A—C8—H8C | 109.5 |
H3B—C3—H3C | 109.5 | H8B—C8—H8C | 109.5 |
C1—C4—H4A | 109.5 | P1—C9—H9A | 109.5 |
C1—C4—H4B | 109.5 | P1—C9—H9B | 109.5 |
H4A—C4—H4B | 109.5 | H9A—C9—H9B | 109.5 |
C1—C4—H4C | 109.5 | P1—C9—H9C | 109.5 |
H4A—C4—H4C | 109.5 | H9A—C9—H9C | 109.5 |
H4B—C4—H4C | 109.5 | H9B—C9—H9C | 109.5 |
C9—P1—C1—C2 | −47.69 (14) | C9—P1—C5—C7 | −41.13 (14) |
C5—P1—C1—C2 | 78.12 (13) | C1—P1—C5—C7 | −166.88 (11) |
C9—P1—C1—C4 | −171.92 (12) | C9—P1—C5—C6 | 78.65 (13) |
C5—P1—C1—C4 | −46.11 (14) | C1—P1—C5—C6 | −47.10 (14) |
C9—P1—C1—C3 | 70.25 (13) | C9—P1—C5—C8 | −158.57 (12) |
C5—P1—C1—C3 | −163.93 (10) | C1—P1—C5—C8 | 75.67 (13) |
D—H···A | D—H | H···A | D···A | D—H···A |
P1—H1···Cl1 | 1.308 (19) | 2.675 (19) | 3.8400 (6) | 147.2 (12) |
Experimental details
Crystal data | |
Chemical formula | C9H22P+·Cl− |
Mr | 196.69 |
Crystal system, space group | Orthorhombic, P212121 |
Temperature (K) | 173 |
a, b, c (Å) | 7.0601 (6), 10.5406 (6), 15.7074 (10) |
V (Å3) | 1168.91 (14) |
Z | 4 |
Radiation type | Mo Kα |
µ (mm−1) | 0.41 |
Crystal size (mm) | 0.42 × 0.37 × 0.35 |
Data collection | |
Diffractometer | Stoe IPDSII two-circle |
Absorption correction | Multi-scan (MULABS; Spek, 2003; Blessing, 1995) |
Tmin, Tmax | 0.846, 0.869 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 16039, 2191, 2138 |
Rint | 0.065 |
(sin θ/λ)max (Å−1) | 0.608 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.023, 0.060, 1.08 |
No. of reflections | 2191 |
No. of parameters | 105 |
H-atom treatment | H atoms treated by a mixture of independent and constrained refinement |
Δρmax, Δρmin (e Å−3) | 0.22, −0.21 |
Absolute structure | Flack (1983), 905 Friedel pairs |
Absolute structure parameter | 0.00 (7) |
Computer programs: X-AREA (Stoe & Cie, 2001), SHELXS97 (Sheldrick, 1990), SHELXL97 (Sheldrick, 1997), XP in SHELXTL-Plus (Sheldrick, 1991).
D—H···A | D—H | H···A | D···A | D—H···A |
P1—H1···Cl1 | 1.308 (19) | 2.675 (19) | 3.8400 (6) | 147.2 (12) |
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.