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Boron Carbide Powder for Nuclear Applications

Boron Carbide Powder for Nuclear Applications

Boron is an important material for nuclear applications due to its high neutron absorption cross section (760 barn* at neutron velocity of 2200 m/sec). The cross section of the B10 isotope in boron is considerably higher (3800 barn). In addition, boron doesn’t contain decay products with a long half-life and high-energy secondary radioactive materials. Since pure boron is extremely brittle and difficult to produce in shapes (for example: control rods) boron carbide is the material of choice to use since it provides a high concentration of boron atoms in a strong and refractory form and is relatively easy to fabricate.

Technical data
• Appearance (dry state): Color Black
• Chemical composition: Chemical formula: B4C Application
Grade NG (Nuclear)
B + C min. 98
B (Boron) min. 76
C (Carbon) max. 24
B2O3 0.1
Fe (Iron) max. 0.1
Si (Silicon) 0.01
N (Nitrogen) 0.5
Isotope B10 (atomic weight) 19.5-21.5%
• Physical data: Knoop hardness (0.1) 3000
Mohs hardness < 9.5
Specific gravity: 2.51
Melting point: 2723 °F
Structure: Monocrystalline

Note: 1. Diamond’s Mohs hardness is 10.
2. *Barn is unit of area equal to 10-24 sq. centimeters, used to measure cross sections in nuclear physics.



UKA Grade Average
Particle Size
Typical Application Notes
1. NG112M 112 micron Additive to concrete B<75%
2. NG36L 36 micron B<70%
3. NG24H 24 micron Nuclear Shielding Panels, Reaction Control Rods,
Etc.
B>76%
4. NG24HE 24 micron B>76% + Enhanced Heat Transfer Capability
5. NG100H 100 micron B>76%
6. NG100HE 100 micron B>76% + Enhanced Heat Transfer Capability
7. NG6H 6 micron B>76%
8. NG6HE 6 micron B>76% + Enhanced Heat Transfer Capability

Note: 1. Custom products are available on request.
2. Standard packaging in 100 lb (30 gal.) fiber drums. Custom packaging is available on request.

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