Beryllium Sputtering Target, 3mm Thickness
Beryllium Sputtering Target, 3mm Thickness
SKU:BER-9ea684
High-purity 3mm Beryllium Sputtering Target for efficient ion bombardment, ensuring precise sputtering processes.
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$299.99
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$299.99
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Beryllium Sputtering Target, 3mm Thickness
$299.99
Quantity: 1
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Beryllium Sputtering Target, 3mm Thickness
$299.99
Quantity: 1
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The 3mm Thickness Beryllium Sputtering Target, manufactured by Goodfellow Corp., offers a purity of 99.0%. This high-quality material is ideal for sputtering processes, ensuring efficient atom removal by ion bombardment. With low impurity levels including Aluminum, Calcium, and Nickel, this target guarantees precise performance. Beryllium's exceptional thermal conductivity and resistance to corrosion make it a superior choice for applications requiring thermal, mechanical, and electrical properties.
Product Specifications
Atomic Properties Atomic Number
4
Atomic Properties Atomic Radius Goldschmidt
0 nm
Atomic Properties Atomic Weight
9.01218 amu
Atomic Properties Crystal Structure
Hexagonal Close Packed
Atomic Properties Electronic Structure
He2s2
Atomic Properties Ionization Potential Number
1 | 2 | 3 | 4
Atomic Properties Ionization Potential Number 1
9.32 eV
Atomic Properties Ionization Potential Number 2
18.2 eV
Atomic Properties Ionization Potential Number 3
154 eV
Atomic Properties Ionization Potential Number 4
218 eV
Atomic Properties Photo Electric Work Function
3.40 eV
Atomic Properties Thermal Neutron Absorption Cross Section
0.0092 Barns
Atomic Properties Valences Shown
2
Electrical Properties Electrical Resistivity At 20 Degree Celsiu
3.3 µΩ·cm
Electrical Properties Superconductivity Critical Temperature
0.0260 K
Electrical Properties Temperature Coefficient At 0 To 100 Degree
0.00900 k-1
Material Material
BerylliumDiscovered in 1797 by N.L. Vauquelin in Paris, but not extracted until 1828 by Wöhler (Berlin) and A.A.B. Bussy (Paris). Beryllium is a light and lustrous metal which is obtained by the electrolysis of a fused halide (e.g. BeClâ). It is resistant to attack by air or water, even at elevated temperatures (red heat). Beryllium is non-magnetic, is a good thermal conductor and is used as an alloying addition to copper or nickel, the alloys having excellent thermal, mechanical and electrical properties; in addition, when alloyed with nickel, the resultant Be/Ni alloy has the highest coefficient for secondary electron emission (12.3). Applications for pure beryllium include its use as windows in X-ray tubes and as a source of neutrons when bombarded with alpha particles, a technique used by Chadwick in 1932 in their discovery. Beryllium and its compounds are highly toxic, inhalation of the dust resulting in berylliosis, an inflammation of the lungs.
Mechanical Properties Bulk Modulus Hard
110.0 GPa
Mechanical Properties Bulk Modulus Soft
110.0 GPa
Mechanical Properties Hardness Vickers Hard
200 Kgf mm-2
Mechanical Properties Hardness Vickers Soft
150 Kgf mm-2
Mechanical Properties Material Condition
Hard | Soft
Mechanical Properties Poissons Ratio Hard
0.020
Mechanical Properties Poissons Ratio Soft
0.020
Mechanical Properties Tensile Modulus Hard
318.00 GPa
Mechanical Properties Tensile Modulus Soft
318.00 GPa
Mechanical Properties Tensile Strength Hard
550.00 MPa
Mechanical Properties Tensile Strength Soft
310.00 MPa
Mechanical Properties Yield Strength Hard
345.0 MPa
Mechanical Properties Yield Strength Soft
240.0 MPa
Note Note
These targets are normally available for immediate shipment from stock. Other sizes are available to special order.
Physical Properties Boiling Point
2470 ºC
Physical Properties Density At 20 Degree Celsius C Temperature
1.848 g·cm-3
Specifications Diameter
25 to 50 mm
Specifications Purity
99.0 %
Specifications Thickness
3 mm
Thermal Properties Coefficient Of Thermal Expansion At 0 To 100
12.000 x10-6 K-1
Thermal Properties Latent Heat Of Evaporation
32470 Jg-1
Tolerances Disc Diameter Tolerance
0.5 mm