The Tin(II) bromide Lewis structure is Sn–Br single bond and Sn–Br single bond; the central Sn has 3 electron domains (1 lone pair), giving a trigonal planar electron-domain arrangement and a bent molecular geometry with a ≈119° bond angle. Sn is best described as sp2-hybridized, and Tin(II) bromide is polar because the bent shape (and/or unequal terminal atoms) prevents cancellation of the bond dipoles.
Figure 1: Lewis Structure of Tin(II) bromide (Br2Sn)
| Chemical Formula | Br2Sn |
| CAS Number | 13465-43-5 |
| Total Valence Electrons | 18 |
| Lewis Structure | Sn–Br single bond and Sn–Br single bond |
| Electron-Domain Geometry | trigonal planar |
| Molecular Geometry | bent |
| Hybridization Model | sp2 (central Sn) |
| Bond Angle | ≈119° |
| Polarity | Polar molecule |
Tin(II) bromide is encountered as a reagent, intermediate or specialty chemical in inorganic, organometallic and materials synthesis. Confirm grade, purity and supplier documentation (SDS) before specifying for a process.
To draw the Tin(II) bromide Lewis structure we first count the total valence electrons. Br2Sn contains 2×7 (Br) + 4 (Sn); the net charge of 0 gives a total of 18 valence electrons to place.
The central atom is Sn. It is the least electronegative atom capable of forming multiple bonds and is surrounded by the more electronegative terminal atom(s); hydrogen, when present, always occupies a terminal position. Electronegativity considerations place the electron density toward the terminal atom(s).
Total valence electrons = 2×7 (Br) + 4 (Sn) = 18 electrons.
Place Sn at the center and connect each surrounding atom with a single bond, complete octets on the terminal atoms, and place any remaining electrons on the central atom. The resulting electron distribution is: Sn–Br single bond and Sn–Br single bond; one lone pair on Sn.
Counting bonding and nonbonding electrons around Sn therefore satisfies the octet/expanded-octet requirement for the drawn structure.
VSEPR theory states that the 3 electron domains around Sn arrange to minimize mutual repulsion, giving an trigonal planar electron-domain geometry.
Because 1 of these domains are lone pair(s) — and lone pairs repel more strongly than bonding pairs — the observed molecular geometry is bent; the Sn bond angle is set to ≈119° rather than the ideal value for the electron-domain geometry.
A useful VSEPR approximation is: lone pair–lone pair repulsion > lone pair–bonding pair repulsion > bonding pair–bonding pair repulsion. With 1 lone pair(s) on Sn, the lone-pair domains occupy positions that minimize overall repulsion while pushing the bonding domains (and therefore the bonded atoms) closer together.
In the conventional localized-bond model, Sn uses sp2 hybrid orbitals to form the 3 equivalent electron-domain directions (2 bonding + 1 lone pair).
Formal charge on central Sn = V − N − ½B = 4 − 2 − ½×4 = 0. The preferred Lewis structure carries zero formal charge on the central atom (and on the terminals), so it is the dominant contributor.
Tin(II) bromide is polar. The bent shape prevents cancellation of the bond dipoles. The bond dipoles do not cancel, leaving a net molecular dipole, which strongly influences solvation behavior and intermolecular interactions.
The decisive structural fact is not simply that the individual bonds are polar; it is whether molecular symmetry allows their vector sum to vanish. In Tin(II) bromide the bent arrangement prevents cancellation, so a permanent dipole remains.
Interpretation consistent with standard VSEPR / molecular-geometry references.This polarity profile underpins its behavior as a solvent, reactant or process intermediate; when sourcing, specify grade and container compatibility.
| Species | Formula | Central Atom | Electron Domains | Molecular Geometry | Polarity |
|---|---|---|---|---|---|
| Tin(II) bromide | Br2Sn | Sn | 3 | bent | Polar |
| Carbon dioxide | CO2 | C | 2 | linear | Nonpolar |
| Carbon monoxide | CO | C | 2 | linear (diatomic) | Polar |
| Carbon disulfide | CS2 | C | 2 | linear | Nonpolar |
Tin(II) bromide is polar. Its bent geometry (and/or unequal terminal atoms) stops the bond dipoles from cancelling.
Sn–Br single bond and Sn–Br single bond; one lone pair on Sn. It uses all 18 valence electrons and the preferred structure carries zero formal charge on the central atom.
The Sn angle is about ≈119°. Lone-pair repulsion compresses the angle from the ideal trigonal planar value.
The conventional model is sp2. Tin(II) bromide has 3 electron domains around the central Sn.
The CAS number is 13465-43-5. PubChem (CID 66224) and NIST identify this with Br2Sn; use it to locate suppliers and database records.
Technical scope: Lewis structures, VSEPR and hybridization are model-based descriptions for chemical communication and structure prediction; actual molecular electronic structure is more accurately represented by molecular-orbital and quantum-chemical methods. Commercial grades vary substantially by supplier and intended use; CAS 13465-43-5 identifies the substance, not a universal purity specification.
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