| ²é¿´: 402 | »Ø¸´: 1 | |||
inmanyzhľ³æ (ÖøÃûдÊÖ)
|
[ÇóÖú]
ÇóÖú·ÒëÕâ¾ä»°¡£
|
|
ͨ¹ý͸¾µµÄ¼¤¹âÇ¿¶È(I0)Ö÷Òª·ÖΪÁ½²¿·Ö£¬Ò»²¿·Ö·øÉäÔÚ¾§ÌåÉÏ£¬¼´¹âÇ¿·øÉäÔÚ¾§ÌåÉϵÄÓÐЧ²¿·Ö£¬ÁíÒ»²¿·Ö±»·´Éä(Ieff)¡£ËûÃÇÖ®¼äµÄ¹ØÏµÊÇIeff +IR=I0¡£¸ù¾ÝÆØ¹âÄÜÁ¿Á÷µÄ¶¨Ò壬½Ó½ü¾§ÌåµÄÓÐÐ§ÆØ¹âÄÜÁ¿Á÷ÊÇEeff = Ieff ¦Ó=(1-R) ¡£ ¾äʽԽ¾«²ÊÔ½ºÃ£¬²»ÒªÖ±Ò룬Âé·³ÁË£¡£¡ |
» ²ÂÄãϲ»¶
±¾¿Æ211£¬293·ÖÇëÇóµ÷¼Á
ÒѾÓÐ6È˻ظ´
085600²ÄÁÏÓ뻯¹¤µ÷¼Á
ÒѾÓÐ25È˻ظ´
±¾9Ò»Ö¾Ô¸2 0854µÍ·Öר˶286Çóµ÷¼Á
ÒѾÓÐ4È˻ظ´
085600£¬320·ÖÇóµ÷¼Á
ÒѾÓÐ9È˻ظ´
316Çóµ÷¼Á
ÒѾÓÐ5È˻ظ´
0856µ÷¼Á
ÒѾÓÐ8È˻ظ´
278Çóµ÷¼Á
ÒѾÓÐ5È˻ظ´
0703Çóµ÷¼Á383·Ö
ÒѾÓÐ3È˻ظ´
400·ÖÇóµ÷¼Á
ÒѾÓÐ3È˻ظ´
085701Çóµ÷¼Á
ÒѾÓÐ5È˻ظ´

Î人һÐÄÒ»Òë
¾èÖú¹ó±ö (ÖøÃûдÊÖ)
- ·ÒëEPI: 502
- Ó¦Öú: 8 (Ó×¶ùÔ°)
- ½ð±Ò: 2283.1
- É¢½ð: 5914
- ºì»¨: 32
- Ìû×Ó: 1665
- ÔÚÏß: 321.9Сʱ
- ³æºÅ: 3587652
- ×¢²á: 2014-12-10
- ÐÔ±ð: GG
- רҵ: ¸ß·Ö×Ӻϳɻ¯Ñ§
¡¾´ð°¸¡¿Ó¦Öú»ØÌû
É̼ÒÒѾÖ÷¶¯ÉùÃ÷´Ë»ØÌû¿ÉÄܺ¬ÓÐÐû´«ÄÚÈÝ|
ͨ¹ý ͸¾µµÄ ¼¤¹âÇ¿¶È(I0) Ö÷Òª·Ö ΪÁ½²¿·Ö£¬Ò»²¿·Ö ·øÉäÔÚ ¾§ÌåÉÏ£¬¼´ ¹âÇ¿·øÉä ÔÚ¾§ÌåÉÏ µÄ ÓÐЧ²¿·Ö£¬ÁíÒ»²¿·Ö ±»·´Éä(Ieff)¡£ËûÃÇÖ®¼ä µÄ¹ØÏµ ÊÇIeff +IR=I0¡£¸ù¾Ý ÆØ¹â ÄÜÁ¿Á÷µÄ ¶¨Ò壬½Ó½ü ¾§ÌåµÄ ÓÐЧ ÆØ¹âÄÜÁ¿Á÷ ÊÇEeff = Ieff ¦Ó=(1-R) ¡£ There are two major parts of laser intensities (I0) travelling through optical lens. The first part of laser radiates onto crystals, also known as the effective part of radiation intensity that radiates on crystals; the other part is reflected laser (Ieff). The correlation between these two parts is Ieff +IR=I0. Based on the definition of exposed energy flux, we can know that the crystal-approaching effective exposed energy flux is Eeff = Ieff ¦Ó=(1-R). |
2Â¥2015-07-19 10:13:52














»Ø¸´´ËÂ¥
10