| ²é¿´: 1131 | »Ø¸´: 6 | |||
| µ±Ç°Ö÷ÌâÒѾ´æµµ¡£ | |||
[½»Á÷]
¡¾ÇóÖú¡¿ÈýÑõ»¯¶þÌúµÄ¾§Ìå½á¹¹ÇóÖú
|
|||
| ÇëÎÊÈýÑõ»¯¶þÌúÊÇʲôÀàÐ͵ľ§Ìå½á¹¹£¿Áí»¹ÓÐa-Ñõ»¯Ìú¡¢r-Ñõ»¯ÌúºÍÈýÑõ»¯¶þÌúµÄÇø±ðÊÇʲô£¿¸÷×Ô¾§Ìå½á¹¹ºÍÐÔÖÊÄÜ·ñÌṩһЩ¡£Ð»Ð» |
» ²ÂÄãϲ»¶
265Çóµ÷¼Á
ÒѾÓÐ9È˻ظ´
085600²ÄÁÏÓ뻯¹¤µ÷¼Á
ÒѾÓÐ20È˻ظ´
ר˶ 351 086100 Ò²ÊÇ¿¼µÄ²Ä¿Æ»ù ±¾¿ÆÒ²ÊDzÄÁÏ
ÒѾÓÐ6È˻ظ´
085600ר˶²ÄÁÏÓ뻯¹¤348·ÖÇóµ÷¼Á
ÒѾÓÐ10È˻ظ´
085600 295·ÖÇóµ÷¼Á
ÒѾÓÐ21È˻ظ´
285Çóµ÷¼Á
ÒѾÓÐ5È˻ظ´
Ò»Ö¾Ô¸°²»Õ´óѧ0817»¯Ñ§¹¤³ÌÓë¼¼Êõ£¬Çóµ÷¼Á
ÒѾÓÐ9È˻ظ´
Ò»Ö¾Ô¸0817»¯Ñ§¹¤³ÌÓë¼¼Êõ£¬Çóµ÷¼Á
ÒѾÓÐ8È˻ظ´
271·ÖÇóµ÷¼ÁѧУ
ÒѾÓÐ3È˻ظ´
ÉúÎïѧ308·ÖÇóµ÷¼Á£¨Ò»Ö¾Ô¸»ª¶«Ê¦´ó£©
ÒѾÓÐ7È˻ظ´
queji
Ìú³æ (ÕýʽдÊÖ)
- Ó¦Öú: 2 (Ó×¶ùÔ°)
- ½ð±Ò: 104.6
- ºì»¨: 4
- Ìû×Ó: 389
- ÔÚÏß: 76.2Сʱ
- ³æºÅ: 556482
- ×¢²á: 2008-05-11
- רҵ: ¼«¶ËÌõ¼þÏÂʹÓõĽðÊô²ÄÁÏ
¡ï
sunxinli(½ð±Ò+1,VIP+0):лл 11-17 15:17
sunxinli(½ð±Ò+1,VIP+0):лл 11-17 15:17
|
ferric oxide has Different forms: Alpha phase, Beta phase, Gamma phase, Epsilon phase, and amorphous phase. [ Last edited by queji on 2009-6-16 at 20:47 ] |
2Â¥2009-06-16 20:39:01
queji
Ìú³æ (ÕýʽдÊÖ)
- Ó¦Öú: 2 (Ó×¶ùÔ°)
- ½ð±Ò: 104.6
- ºì»¨: 4
- Ìû×Ó: 389
- ÔÚÏß: 76.2Сʱ
- ³æºÅ: 556482
- ×¢²á: 2008-05-11
- רҵ: ¼«¶ËÌõ¼þÏÂʹÓõĽðÊô²ÄÁÏ
¡ï
sunxinli(½ð±Ò+1,VIP+0):ÈÏÕæ 11-17 15:17
sunxinli(½ð±Ò+1,VIP+0):ÈÏÕæ 11-17 15:17
|
Alpha phase ¦Á-Fe2O3 has the rhombohedral, corundum (¦Á-Al2O3) structure and is the most common form. It occurs naturally as the mineral hematite which is mined as the main ore of iron. It is antiferromagnetic below ~260 K (Morin transition temperature), and weak ferromagnetic between 260 K and 950 K (Neel temperature).[1] It is easy to prepare using both thermal decomposition and precipitation in the liquid phase. Its magnetic properties are dependent on many factors, e.g. pressure, particle size, and magnetic field intensity. [ Last edited by queji on 2009-6-16 at 20:47 ] |
3Â¥2009-06-16 20:39:41
queji
Ìú³æ (ÕýʽдÊÖ)
- Ó¦Öú: 2 (Ó×¶ùÔ°)
- ½ð±Ò: 104.6
- ºì»¨: 4
- Ìû×Ó: 389
- ÔÚÏß: 76.2Сʱ
- ³æºÅ: 556482
- ×¢²á: 2008-05-11
- רҵ: ¼«¶ËÌõ¼þÏÂʹÓõĽðÊô²ÄÁÏ
¡ï
sunxinli(½ð±Ò+1,VIP+0):ÈÏÕæ 11-17 15:17
sunxinli(½ð±Ò+1,VIP+0):ÈÏÕæ 11-17 15:17
|
Beta phase Cubic face centered, metastable, at temperatures above 500 ¡ãC converts to alpha phase. It can be prepared by reduction of hematite by carbon, pyrolysis of iron(III) chloride solution, or thermal decomposition of iron(III) sulfate. |
4Â¥2009-06-16 20:40:58
queji
Ìú³æ (ÕýʽдÊÖ)
- Ó¦Öú: 2 (Ó×¶ùÔ°)
- ½ð±Ò: 104.6
- ºì»¨: 4
- Ìû×Ó: 389
- ÔÚÏß: 76.2Сʱ
- ³æºÅ: 556482
- ×¢²á: 2008-05-11
- רҵ: ¼«¶ËÌõ¼þÏÂʹÓõĽðÊô²ÄÁÏ
¡ï
sunxinli(½ð±Ò+1,VIP+0):ÈÏÕæ 11-17 15:17
sunxinli(½ð±Ò+1,VIP+0):ÈÏÕæ 11-17 15:17
|
Gamma phase Cubic, metastable, converts to the alpha phase at high temperatures. Occurs naturally as the mineral maghemite. Ferrimagnetic. Ultrafine particles smaller than 10 nanometers are superparamagnetic. Can be prepared by thermal dehydratation of gamma iron(III) oxide-hydroxide, careful oxidation of iron(II,III) oxide. The ultrafine particles can be prepared by thermal decomposition of iron(III) oxalate. |
5Â¥2009-06-16 20:41:29
queji
Ìú³æ (ÕýʽдÊÖ)
- Ó¦Öú: 2 (Ó×¶ùÔ°)
- ½ð±Ò: 104.6
- ºì»¨: 4
- Ìû×Ó: 389
- ÔÚÏß: 76.2Сʱ
- ³æºÅ: 556482
- ×¢²á: 2008-05-11
- רҵ: ¼«¶ËÌõ¼þÏÂʹÓõĽðÊô²ÄÁÏ
¡ï
sunxinli(½ð±Ò+1,VIP+0):ÈÏÕæ 11-17 15:17
sunxinli(½ð±Ò+1,VIP+0):ÈÏÕæ 11-17 15:17
|
Epsilon phase Rhombic, shows properties intermediate between alpha and gamma. So far has not been prepared in pure form; it is always mixed with the alpha phase or gamma phases. Material with a high proportion of epsilon phase can be prepared by thermal transformation of the gamma phase. The epsilon phase is metastable, transforming to the alpha phase at between 500 and 750 ¡ãC. Can also be prepared by oxidation of iron in an electric arc or by sol-gel precipitation from iron(III) nitrate. |
6Â¥2009-06-16 20:42:22
queji
Ìú³æ (ÕýʽдÊÖ)
- Ó¦Öú: 2 (Ó×¶ùÔ°)
- ½ð±Ò: 104.6
- ºì»¨: 4
- Ìû×Ó: 389
- ÔÚÏß: 76.2Сʱ
- ³æºÅ: 556482
- ×¢²á: 2008-05-11
- רҵ: ¼«¶ËÌõ¼þÏÂʹÓõĽðÊô²ÄÁÏ
7Â¥2009-06-16 20:45:24














»Ø¸´´ËÂ¥