ÌâÄ¿ÄÚÈÝ
8£®Ä³ÊµÑéС×éÀûÓÃͼ¼×ËùʾµÄ×°ÖÃ̽¾¿Ð¡³µ×öÔȱäËÙÖ±ÏßÔ˶¯µÄ¹æÂÉ£®¢ÙÏÂÁÐ×ö·¨ÖжÔÓÚÌá¸ßʵÑé½á¹û¾«¶ÈÓÐÀûµÄÊÇCD
A£®Ñ¡Óþ¡¿ÉÄܹ⻬µÄľ°å
B£®Ñ¡ÓÃÖÊÁ¿¾¡Á¿Ð¡Ò»Ð©µÄíÀÂëͰ
C£®¿ªÊ¼Ê±ÈÃС³µ¾¡¿ÉÄܽӽü´òµã¼ÆÊ±Æ÷
D£®Ï¸Éþ±£³ÖÓëľ°åƽÐÐ
¢ÚͼÒÒΪ¸ÃС×éµÃµ½µÄÒ»ÌõÖ½´ø£¬ÏàÁÚÁ½¸ö¼ÆÊýµã¼ä»¹ÓÐËĸöµãδ»³ö£¬¸ù¾Ý¼ºÖªÊý¾Ý¿É¼ÆËã³öС³µÔ˶¯µÄ¼ÓËÙ¶Èa=1.0m/s2 £¨½á¹û±£ÁôÁ½Î»ÓÐЧÊý×Ö£©£»
¢ÛÈôʵÑéÖвÉÓõĽ»Á÷µçƵÂʵÍÓÚ50Hz£¬Ôò¼ÆËã½á¹ûÓëʵֵÏà±ÈÆ«´ó£¨Ìî¡°Æ«´ó¡±¡°Æ«Ð¡¡±¡°²»±ä¡±£©£®
·ÖÎö ¢Ù¸ù¾ÝʵÑéµÄÔÀíÒÔ¼°²Ù×÷ÖеÄ×¢ÒâÊÂÏîÈ·¶¨ÕýÈ·µÄ²Ù×÷²½Ö裮
¢Ú¸ù¾ÝÁ¬ÐøÏàµÈʱ¼äÄÚµÄÎ»ÒÆÖ®²îÊÇÒ»ºãÁ¿£¬ÔËÓÃÖð²î·¨Çó³öС³µÔ˶¯µÄ¼ÓËÙ¶È£®
¢Û¸ù¾ÝÖÜÆÚµÄ²âÁ¿Îó²î£¬½áºÏ¡÷x=aT2È·¶¨¼ÓËٶȵIJâÁ¿Îó²î£®
½â´ð ½â£º¢ÙA¡¢Ì½¾¿Ð¡³µÔȱäËÙÖ±ÏßÔ˶¯µÄ¹æÂÉ£¬Ä¾°åÊÇ·ñ¹â»¬¶ÔʵÑéûÓÐÓ°Ï죬¹ÊA´íÎó£®
B¡¢ÎªÁ˱ãÓÚ²âÁ¿£¬Ê¹µÃµã¼£¼äµÄ¾àÀëÊʵ±´óһЩ£¬Ñ¡ÓÃÖÊÁ¿´óһЩµÄíÀÂëͰ£¬¹ÊB´íÎó£®
C¡¢ÊµÑéʱ£¬Ð¡³µÓ¦¾¡¿ÉÄÜ¿¿½ü´òµã¼ÆÊ±Æ÷£¬¹ÊCÕýÈ·£®
D¡¢Ï¸ÏßÓ¦±£³ÖÓëľ°åƽÐУ¬¹ÊDÕýÈ·£®
¹ÊÑ¡£ºCD£®
¢Ú¸ù¾Ý¡÷x=aT2£¬ÔËÓÃÖð²î·¨µÃ£ºa=$\frac{{x}_{CE}-{x}_{AC}}{4{T}^{2}}=\frac{£¨8.21+9.69-6.20-7.70£©¡Á1{0}^{-2}}{4¡Á0.01}$=1.0m/s2£®
¢ÛÈôʵÑéÖвÉÓõĽ»Á÷µçƵÂʵÍÓÚ50Hz£¬ÔòÖÜÆÚµÄ²âÁ¿Öµ±Èʵ¼ÊֵƫС£¬¸ù¾Ý$a=\frac{¡÷x}{{T}^{2}}$Öª£¬¼ÓËٶȵIJâÁ¿ÖµÆ«´ó£®
¹Ê´ð°¸Îª£º¢ÙCD£»¢Ú1.0£»¢ÛÆ«´ó£®
µãÆÀ ½â¾ö±¾ÌâµÄ¹Ø¼üÖªµÀʵÑéµÄÔÀíÒÔ¼°²Ù×÷ÖеÄ×¢ÒâÊÂÏî£¬ÕÆÎÕÖ½´øµÄ´¦Àí·½·¨£¬»áͨ¹ýÖ½´øÇó½â˲ʱËٶȺͼÓËÙ¶È£®
| A£® | $\frac{\sqrt{3}}{3}$mg | B£® | mg | C£® | $\sqrt{3}$mg | D£® | $\frac{1}{2}$mg |
| A£® | Ò»¶¨ÖÊÁ¿ÆøÌåѹǿ²»±äζÈÉý¸ßʱ£¬ÎüÊÕµÄÈÈÁ¿Ò»¶¨´óÓÚÄÚÄܵÄÔö¼Ó | |
| B£® | ¿ÉÀûÓø߿Ƽ¼ÊֶΣ¬½«Á÷É¢µÄÄÚÄÜÈ«²¿ÊÕ¼¯¼ÓÒÔÀûÓ㬶ø²»ÒýÆðÆäËû±ä»¯ | |
| C£® | ¸ß¿ÕÖеıù¾§ÔÚ¿ÕÆøÖÐÏÂÂä±ä³ÉÓêµÎʱ£¬ÄÚÄÜÔö¼ÓÁË | |
| D£® | µ±·Ö×Ó¼äµÄÏ໥×÷ÓÃÁ¦ÎªÒýÁ¦Ê±£¬Æä·Ö×Ó¼äûÓгâÁ¦ | |
| E£® | ²¼ÀÊÔ˶¯²¢²»ÊÇ·Ö×ÓµÄÎÞ¹æÔòÔ˶¯£¬ÊÇÒºÌå·Ö×ÓÎÞ¹æÔòÔ˶¯µÄ·´Ó³ |
| A£® | îѵÄÒݳö¹¦Îª6.67¡Á10-19J | |
| B£® | îѵļ«ÏÞÆµÂÊΪ1.0¡Á1015Hz | |
| C£® | ¹âµç×ÓµÄ×î´ó³õ¶¯ÄÜΪ1.0¡Á10-18J | |
| D£® | Óò»Í¬ÆµÂʵĵ¥É«¹âÕÕÉä½ðÊôîѱíÃæ£¬Èô¶¼ÄÜ·¢Éú¹âµçЧӦ£¬ÔòÆä×î´ó³õ¶¯Äܲ¢²»Ïàͬ | |
| E£® | ¹âµç×ÓµÄ×î´ó³õ¶¯ÄÜÓëÈëÉä¹âµÄƵÂʳÉÕý±È |
| A£® | a¡¢bÏßËÙ¶ÈÖ®±ÈΪ3£º2 | B£® | a¡¢b½ÇËÙ¶ÈÖ®±ÈΪ2$\sqrt{2}$£º3$\sqrt{3}$ | ||
| C£® | a¡¢bÖÜÆÚÖ®±ÈΪ2$\sqrt{2}$£º3$\sqrt{3}$ | D£® | a¡¢bÏòÐļÓËÙ¶ÈÖ®±ÈΪ4£º9 |
| A£® | $\frac{s}{{v}_{0}}$ | B£® | $\sqrt{\frac{2h}{g}}$ | C£® | $\frac{{v}_{1}}{g}$ | D£® | $\frac{\sqrt{{{v}_{1}}^{2}-{{v}_{0}}^{2}}}{g}$ |