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Key Documents

GF78645022

Tin

foil, not light tested, 50x50mm, thickness 0.015mm, 99.75%

Synonym(s):

Tin, SN000170

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About This Item

Empirical Formula (Hill Notation):
Sn
CAS Number:
Molecular Weight:
118.71
MDL number:
UNSPSC Code:
12141745
PubChem Substance ID:
NACRES:
NA.23

Assay

99.75%

form

foil

manufacturer/tradename

Goodfellow 786-450-22

resistivity

11 μΩ-cm, 20°C

size × thickness

50 x 50 mm × 0.015 mm

bp

2270 °C (lit.)

mp

231.9 °C (lit.)

density

7.310 g/mL at 25 °C (lit.)

SMILES string

[Sn]

InChI

1S/Sn

InChI key

ATJFFYVFTNAWJD-UHFFFAOYSA-N

General description

For updated SDS information please visit www.goodfellow.com.

Legal Information

Product of Goodfellow

Certificates of Analysis (COA)

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Lis Danielsen et al.
Forensic science international, 134(2-3), 134-141 (2003-07-10)
Previously, electrical injuries have been suggested caused only by the concomitant heat developed during the passage of an electrical current. Recent experimental studies on fully anesthetized pigs and the study of one human case have, however, shown typical electrical alterations.
Britta A Jung et al.
Clinical oral implants research, 22(6), 664-668 (2010-11-04)
To evaluate the necessity of three-dimensional imaging (computed tomography [CT]/cone-beam computed tomography [CBCT]) for paramedian insertion of palatal implants. Lateral radiographs and CBCT scans were performed from 18 human skulls. For lateral cephalometry, the nasal floor (right/left) and the oral
Mercury contamination removed with tin foil.
R Grajower et al.
Operative dentistry, 9(3), 101-104 (1984-01-01)
K-H Utz et al.
Journal of oral rehabilitation, 29(5), 458-466 (2002-05-25)
In a dentate subject a jaw relation can either be determined in maximum intercuspation and is as such given by the occlusal morphology, or the mandibular position can be allocated according to the centric position of the condyles. For comprehensive
Andrey A Gurtovenko et al.
The Journal of chemical physics, 130(21), 215107-215107 (2009-06-11)
The electrostatic properties of lipid membranes are of profound importance as they are directly associated with membrane potential and, consequently, with numerous membrane-mediated biological phenomena. Here we address a number of methodological issues related to the computation of the electrostatic

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