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Merck

GF42290939

Carbon

foil, not light tested, 150x150mm, thickness 0.125mm, flexible graphite, 99.8%

Sinónimos:

Activated charcoal, C 000208, Charcoal activated

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About This Item

Fórmula empírica (notación de Hill):
C
Número de CAS:
Peso molecular:
12.01
MDL number:
UNSPSC Code:
12141908
PubChem Substance ID:
NACRES:
NA.23

vapor pressure

<0.1 mmHg ( 20 °C)

assay

99.8%

form

foil

autoignition temp.

842 °F

manufacturer/tradename

Goodfellow 422-909-39

resistivity

1375 μΩ-cm, 20°C (graphite)

size × thickness

150x150 mm × 0.125 mm

mp

3550 °C (lit.)

SMILES string

[C]

InChI

1S/C

InChI key

OKTJSMMVPCPJKN-UHFFFAOYSA-N

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General description

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

Legal Information

Product of Goodfellow

Storage Class

13 - Non Combustible Solids

wgk_germany

nwg

flash_point_f

Not applicable

flash_point_c

Not applicable


Certificados de análisis (COA)

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Investigation of delta -electron emission in collisions of highly charged fast Ne projectiles with carbon-foil targets.
Schiwietz et al.
Physical review. B, Condensed matter, 41(10), 6262-6271 (1990-04-01)
I Dietrich et al.
Ultramicroscopy, 3(2), 185-189 (1978-01-01)
Radiation damage on a holey carbon foil was investigated in an electron microscope with a superconducting lens system, where the temperature of the specimen and its environment initially was 4 K. Due to an electron dose of 2 X 10(4)
Doubly differential secondary-electron yields following 8-MeV/u U68+- and 3.5-MeV/u U38+-ion impact on a thin carbon-foil target.
Schneider et al.
Physical review. A, Atomic, molecular, and optical physics, 47(5), 3945-3950 (1993-05-01)
M C Ledbetter et al.
Proceedings of the National Academy of Sciences of the United States of America, 84(1), 85-88 (1987-01-01)
Cluster ions containing 50, 100, or 200 water molecules and one proton are accelerated to over 275 kV and impacted on thin carbon films on which tobacco mosaic virus has been dispersed. After bombardment the films are examined with a
D J McComas et al.
Proceedings of the National Academy of Sciences of the United States of America, 88(21), 9598-9602 (1991-11-01)
Global imaging of the magnetospheric charged particle population can be achieved by remote measurement of the neutral atoms produced when magnetospheric ions undergo charge exchange with cold exospheric neutral atoms. Previously suggested energetic neutral atom imagers were only able to

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