Bottom price Alpha Alumina Alpha - Calcined Alumina (FA) Series for Heat Conduction – Yufa
Bottom price Alpha Alumina Alpha - Calcined Alumina (FA) Series for Heat Conduction – Yufa Detail:
Applications
| Chemical Composition (%) | Ture Density | Apparent Density | Grain Size | Original Crystal | Oil Absorption Rate | Conversion Rate | +325 | Residual Boron | Features | Recommended Applications | |||||
| Model No. | Al2O3 ≥% |
SiO2 ≤% |
Fe2O3 ≤% |
Na2O ≤% |
LOI ≤% |
g/cm3 ≥ |
g/cm3 ＞ |
D50 (μm) |
D50 (μm) |
ml | ≥% | ＜% | ＜% | ||
| FA3 | 99.5 | 0.1 | 0.03 | 0.08 | 0.1 | 3.96 | >0.85 | ~2.8 | 2.1-2.7 | ＜17 | ≥95 | 0.5 | / | 1. High temperature calcination 2. Deep grinding & Good flowability 3. Reasonable particle size distribution 4. Good thermo conductivity |
1. It can be used to thermal conductive materials 2. It suitable for ceramic coatings etc. |
| FA4 | 99.5 | 0.05 | 0.03 | 0.08 | 0.1 | 3.96 | >0.85 | ~4 | 3.6-4.5 | 13-15 | ≥95 | 0.5 | 0.02 | 1. High temperture clacination 2. Deep grinding 3. Reasonable grain size & crystal shape distribution 4. Good flowability & Good thermo conductivity |
|
| FA5 | 99.5 | 0.05 | 0.03 | 0.10 | 0.1 | 3.96 | >0.85 | ~6 | 5.5-6 | ≤14 | ≥95 | 0.5 | 0.1 | 1. High temperature calcination 2. Deep grinding 3. Larger crystal paticle 4. Reasonable paricle distribution 5. High apparent density 6. Good flowability & good themo conductivity |
|
| FA10 | 99.5 | 0.05 | 0.03 | 0.10 | 0.1 | 3.96 | >0.85 | ~10 | 8-10 | / | ≥95 | 1 | 0.1 | 1. Large crystal particle 2. Reasonable particle size distribution 3. High apparent density 4. Excellent flowability 5. Excellent thermo conductivity |
|
| FA15 | 99.5 | 0.05 | 0.03 | 0.10 | 0.1 | 3.96 | >0.85 | ~13 | 10-13 | / | ≥95 | 1 | 0.1 | 1. Special production process 2. Large crystal particle 3. Good flowability 4. Good thermoconductivity |
|
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By Margaret from Croatia - 2017.10.27 12:12
Sales manager is very enthusiastic and professional, gave us a great concessions and product quality is very good,thank you very much!
By Ada from Australia - 2018.12.28 15:18
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