| ²é¿´: 1370 | »Ø¸´: 7 | |||
| µ±Ç°Ö÷ÌâÒѾ´æµµ¡£ | |||
| µ±Ç°Ö»ÏÔʾÂú×ãÖ¸¶¨Ìõ¼þµÄ»ØÌû£¬µã»÷ÕâÀï²é¿´±¾»°ÌâµÄËùÓлØÌû | |||
ZANCAIгæ (ÖøÃûдÊÖ)
|
[½»Á÷]
ÇëÎÊʲôÊdz¬Ë³´ÅÐÔ°¡¡£
|
||
| ÎÒ¿´ÎÄÏ×˵ÄÉÃ×ËÄÑõ»¯ÈýÌúÓг¬Ë³´ÅÐÔ£¬Ê²Ã´Êdz¬Ë³´ÅÐÔ°¡£¬ÓëÎÒÃÇͨ³£´ÅÌúµÄ´ÅÐÔÓÐÇø±ðÂð£¬ÆÕͨµÄËÄÑõ»¯ÈýÌú¾ÍûÓг¬Ë³´ÅÐÔÂ𣬳¬Ë³´ÅÐÔÓÐʲôӦÓÃÂð£¿Ð»Ð»¡£ |
» ²ÂÄãϲ»¶
ѧԺ¹Ù·½Èº-ԺʿÍŶÓÕÐÉú-ѧÉú×ÔÓɶȸß-ÅàÑøÄ£Ê½³ÉÊìÒÑÓÐ10ÓàÃûѧÉú¸°985º£ÍâÉîÔì
ÒѾÓÐ0È˻ظ´
Î人·ÄÖ¯´óѧ»¯¹¤Ñ§Ôº¹Ù·½Èº-ԺʿÍŶÓÕÐÉú-ѧÉú×ÔÓɶȸß-10ÓàÃûѧÉú¸°985º£ÍâÉîÔì
ÒѾÓÐ0È˻ظ´
ÎÞ»ú»¯Ñ§ÂÛÎÄÈóÉ«/·ÒëÔõôÊÕ·Ñ?
ÒѾÓÐ143È˻ظ´
Äϲýº½¿Õ´óѧ½¯»ª÷ë½ÌÊÚ¿ÎÌâ×éÕÐÊÕ»¯Ñ§¡¢»·¾³¡¢Ì¼´ï·å̼Öкͼ°Ïà¹Ø×¨ÒµË¶Ê¿ÐÅÏ¢
ÒѾÓÐ0È˻ظ´
ºþ±±Ê¦·¶´óѧ¸´ÊÔµ÷¼Á
ÒѾÓÐ0È˻ظ´
Î人·ÄÖ¯´óѧ_»¯¹¤Ñ§Ôº¹Ù·½µ÷¼ÁȺ-ԺʿÍŶÓÕÐÉú-ѧÉú×ÔÓɶȸß-ÿ½ì·¢Õ¹ºÃ
ÒѾÓÐ0È˻ظ´
ºÓ±±´óѧ²ÄÁÏÓ뻯¹¤×¨ÒµÑо¿Éú£¨×¨Ë¶£©ÕÐÊÕµ÷¼ÁÉú
ÒѾÓÐ0È˻ظ´
ºÓ±±´óѧÎÞ»ú»¯Ñ§×¨ÒµÕÐÊÕµ÷¼ÁÉú
ÒѾÓÐ0È˻ظ´
¼ÃÄÏ´óѧ¹ú¼ÒÓÅÇà¿ÎÌâ×é 2026 µ÷¼ÁÕÐÉúÀ´À²
ÒѾÓÐ0È˻ظ´
Î人·ÄÖ¯´óѧ_»¯Ñ§Ôº¹Ù·½µ÷¼ÁȺ-ԺʿÍŶÓÕÐÉú-ѧÉú×ÔÓɶȸ߷¢Õ¹ºÃ-»¶Ó¸÷λͬѧ
ÒѾÓÐ0È˻ظ´
» ±¾Ö÷ÌâÏà¹ØÉ̼ÒÍÆ¼ö: (ÎÒÒ²ÒªÔÚÕâÀïÍÆ¹ã)
ZANCAI
гæ (ÖøÃûдÊÖ)
- Ó¦Öú: 5 (Ó×¶ùÔ°)
- ½ð±Ò: 53.4
- É¢½ð: 654
- ºì»¨: 5
- Ìû×Ó: 1943
- ÔÚÏß: 841.7Сʱ
- ³æºÅ: 398036
- ×¢²á: 2007-06-10
- רҵ: ÂÌÉ«Óлú»¯Ñ§
3Â¥2008-03-10 13:14:47
FePt
ľ³æ (ÕýʽдÊÖ)
- Ó¦Öú: 0 (Ó×¶ùÔ°)
- ½ð±Ò: 1851
- É¢½ð: 25
- Ìû×Ó: 717
- ÔÚÏß: 284.8Сʱ
- ³æºÅ: 502966
- ×¢²á: 2008-02-15
- רҵ: µç¹¤²ÄÁÏÌØÐÔ¼°ÆäÓ¦ÓÃ
¡ï
jackchen145(½ð±Ò+1,VIP+0):ллӦÖú!»¶Ó³£À´ÄÉÃ×°æ
jackchen145(½ð±Ò+1,VIP+0):ллӦÖú!»¶Ó³£À´ÄÉÃ×°æ
|
Õâ¸ö½âÊÍÆðÀ´Ì«·Ñ¾¢£¬ÒÔÏÂÊÇWikipediaµÄ½âÊÍ£¬¿´ÁËÒ»±é£¬´ó¸ÅÄÜ˵Çå³þ Superparamagnetism From Wikipedia, the free encyclopedia Jump to: navigation, search Superparamagnetism is a phenomenon by which magnetic materials may exhibit a behavior similar to paramagnetism even when at temperatures below the Curie or the N¨¦el temperature. This is a small length-scale phenomenon, where the energy required to change the direction of the magnetic moment of a particle is comparable to the ambient thermal energy. At this point, the rate at which the particles will randomly reverse direction becomes significant. Normally, coupling forces in ferromagnetic materials cause the magnetic moments of neighboring atoms to align, resulting in very large internal magnetic fields. This is what distinguishes ferromagnetic materials from paramagnetic materials. At temperatures above the Curie temperature (or the Neel temperature for antiferromagnetic materials), the thermal energy is sufficient to overcome the coupling forces, causing the atomic magnetic moments to fluctuate randomly. Because there is no longer any magnetic order, the internal magnetic field no longer exists and the material exhibits paramagnetic behavior. If the material is non-homogeneous, one can observe a mixture of ferromagnetic and paramagnetic clusters of atoms at the same temperature, the superparamagnetic stage. The idea of superparamagnetism is used in SuperParamagnetic Clustering algorithm (SPC) as well as in its extension global SPC. Superparamagnetism occurs when the material is composed of very small crystallites (1¨C10 nm). In this case even when the temperature is below the Curie or Neel temperature (and hence the thermal energy is not sufficient to overcome the coupling forces between neighboring atoms), the thermal energy is sufficient to change the direction of magnetization of the entire crystallite. The resulting fluctuations in the direction of magnetization cause the magnetic field to average to zero. Thus the material behaves in a manner similar to paramagnetism, except that instead of each individual atom being independently influenced by an external magnetic field, the magnetic moment of the entire crystallite tends to align with the magnetic field. The energy required to change the direction of magnetization of a crystallite is called the crystalline anisotropy energy and depends both on the material properties and the crystallite size. As the crystallite size decreases, so does the crystalline anisotropy energy, resulting in a decrease in the temperature at which the material becomes superparamagnetic. The rate at which particles will lose their direction is governed by the Neel-Arrhenius equation. In particular, it is a function of the exponential of the grain volume. |
2Â¥2008-03-10 11:35:42
our360
ľ³æ (СÓÐÃûÆø)
С±ø
- Ó¦Öú: 0 (Ó×¶ùÔ°)
- ½ð±Ò: 5004.7
- Ìû×Ó: 247
- ÔÚÏß: 81.8Сʱ
- ³æºÅ: 484559
- ×¢²á: 2007-12-27
- ÐÔ±ð: GG
- רҵ: ÎÞ»úÄÉÃ×»¯Ñ§
¡ï
jackchen145(½ð±Ò+1,VIP+0):ллӦÖú!»¶Ó³£À´ÄÉÃ×°æ
jackchen145(½ð±Ò+1,VIP+0):ллӦÖú!»¶Ó³£À´ÄÉÃ×°æ
| µ±ÄÉÃ×Á£×ÓСµ½Ò»¶¨³ß´çµÄʱºò£¬±ÈÈçËÄÑõ»¯ÈýÌúÁ£×Ó´óСΪʮ¼¸¶þÊ®ÄÉÃ×»òÕ߸üС£¬Ã¿Ò»¸öÄÉÃ×Á£×Ó¶¼Ï൱ÓÚÒ»¸öСµÄ´Å³ë¡£µ±ÎÞÍâ¼Ó´Å³¡£¬Á£×Ó£¨´Å³ë£©ÅÅÁÐÎÞÐò£¬±íÏÖΪ˳´Å¡£µ±Ê©¼Ó´Å³¡£¬Á£×Ó°´´Å³¡ÅÅÁУ¬ÏÔʾ³öÌú´Å£¨µ«±È¿éÌåÈõ£©¡£Õâ¾ÍÊÇÎÒÃdz£ËµµÄ³¬Ë³´ÅÁË¡£¶ø¿éÌåÔò²»»á£¬¿ÉÒÔ×Ô¼ºÏëÏóһϡ£ |

4Â¥2008-03-10 15:14:03
ÏëÖªµÀ ÄãµÄ²ÄÁÏÊÇ·ñÓÐÒþÉíÐÔÄÜô£¿
|
µç´Å²ÎÊýºÍ·´ÉäÂʲâÊÔ£¨2¡«18GHz£©£¬¿ÉÌṩÊý¾ÝºÍÇúÏߣ¬¼Û¸ñ¸ù¾ÝÊýÁ¿¶ø¶¨£¨ Ò»°ãΪ200ÔªÕû¸öƵ¶Î£©¡£ ÕÅÏÈÉú zschenkai@163.com 13681011903 q19572435 |
5Â¥2008-03-10 21:10:18














»Ø¸´´ËÂ¥