µÚÒ»Ìâ

ÏÖÔÚÖ¤Ã÷£¬ DÊÇ BC µÄÖе㡣 ×öƽÐÐËıßÐεĵڶþÌõ¶Ô½ÇÏßAC¡£ µÚÒ»Ìõ¶Ô½ÇÏßÊÇÈý½ÇÐÎABC AC ±ßµÄÖÐÏß¡£ Èç¹ûD²»ÊÇ BC µÄÖе㣬 ×öÈý½ÇÐÎABC BC ±ßµÄÖÐÏߣ¬¼´Í¼ÖкìÏß¡£Ôò AC ±ßµÄÖÐÏß½«ºìÏ߽سÉÉÏϳ¤¶È±ÈΪ 2:1 µÄÁ½²¿·Ö¡£ µ« AC ±ßµÄÖÐÏßͬʱ°ÑAD Ò²½Ø³ÉÉÏϳ¤¶È±ÈΪ 2:1 µÄÁ½²¿·Ö¡£ÕâÑùÁ½¸ö½»µãµÄÁ¬ÏßÓ¦µ±Æ½ÐÐÓڵױߡ£ ÕâÊDz»¿ÉÄܵġ£ËùÒÔDÊÇ BC µÄÖе㡣
Èý½ÇÐÎABD µÄÃæ»ýÊÇÆ½ÐÐËıßÐ뵀 1/4, 96.
µÚ¶þÌâ

ÑÓ³¤ BD ½» CO ÓÚ E¡£ Òò½ÇCBD ÊÇÖ±½Ç£¬ CE ÊÇÔ²µÄÖ±¾¶¡£ ËùÒÔCD = DE£¬\[ \angle{OCD} = \angle{OED} = \frac{1}{2}\angle{CDB} = \frac{\pi}{8}¡£\]Éè \( r = \)Ô²°ë¾¶£¬ Ôò \[ a = r - r\tan \frac{\pi}{8}= r( 1 - \frac{\sin \frac{\pi}{4}}{1 + \cos \frac{\pi}{4}})\] ËùÒÔ£¬ \[r = a(1 + \frac{\sqrt{2}}{2} ) \]¶øËùÇóÈý½ÇÐÎÃæ»ýΪ \[ \frac{1}{2}r(r-a) = a^2 \frac{1}{2}(1 + \frac{\sqrt{2}}{2} )\frac{\sqrt{2}}{2}= \frac{1}{4}a^2(2 + \sqrt{2})\]

ÏÖÔÚÖ¤Ã÷£¬ DÊÇ BC µÄÖе㡣 ×öƽÐÐËıßÐεĵڶþÌõ¶Ô½ÇÏßAC¡£ µÚÒ»Ìõ¶Ô½ÇÏßÊÇÈý½ÇÐÎABC AC ±ßµÄÖÐÏß¡£ Èç¹ûD²»ÊÇ BC µÄÖе㣬 ×öÈý½ÇÐÎABC BC ±ßµÄÖÐÏߣ¬¼´Í¼ÖкìÏß¡£Ôò AC ±ßµÄÖÐÏß½«ºìÏ߽سÉÉÏϳ¤¶È±ÈΪ 2:1 µÄÁ½²¿·Ö¡£ µ« AC ±ßµÄÖÐÏßͬʱ°ÑAD Ò²½Ø³ÉÉÏϳ¤¶È±ÈΪ 2:1 µÄÁ½²¿·Ö¡£ÕâÑùÁ½¸ö½»µãµÄÁ¬ÏßÓ¦µ±Æ½ÐÐÓڵױߡ£ ÕâÊDz»¿ÉÄܵġ£ËùÒÔDÊÇ BC µÄÖе㡣
Èý½ÇÐÎABD µÄÃæ»ýÊÇÆ½ÐÐËıßÐ뵀 1/4, 96.
µÚ¶þÌâ

ÑÓ³¤ BD ½» CO ÓÚ E¡£ Òò½ÇCBD ÊÇÖ±½Ç£¬ CE ÊÇÔ²µÄÖ±¾¶¡£ ËùÒÔCD = DE£¬\[ \angle{OCD} = \angle{OED} = \frac{1}{2}\angle{CDB} = \frac{\pi}{8}¡£\]Éè \( r = \)Ô²°ë¾¶£¬ Ôò \[ a = r - r\tan \frac{\pi}{8}= r( 1 - \frac{\sin \frac{\pi}{4}}{1 + \cos \frac{\pi}{4}})\] ËùÒÔ£¬ \[r = a(1 + \frac{\sqrt{2}}{2} ) \]¶øËùÇóÈý½ÇÐÎÃæ»ýΪ \[ \frac{1}{2}r(r-a) = a^2 \frac{1}{2}(1 + \frac{\sqrt{2}}{2} )\frac{\sqrt{2}}{2}= \frac{1}{4}a^2(2 + \sqrt{2})\]
���à¼Ê±ï¿½ï¿½: 2023-06-17 15:57:58


[¶ÀÆÀ] 