ÊÀÉÏ×îΰ´óµÄÊ®¸ö¹«Ê½£¬Ñ¦¶¨ÚÌ·½³ÌÅÅÃûµÚÁù£¬ÖÊÄÜ·½³ÌÅÅÃûµÚÎå
Ó¢¹ú¿ÆÑ§ÆÚ¿¯¡¶ÎïÀíÊÀ½ç¡·ÔøÈöÁÕßͶƱÆÀÑ¡ÁË¡°×îΰ´óµÄ¹«Ê½¡±£¬×îÖÕ°ñÉÏÓÐÃûµÄÊ®¸ö¹«Ê½¼ÈÓÐÎÞÈ˲»ÖªµÄ1+1=2£¬ÓÖÓÐÖøÃûµÄE=mc2£»¼ÈÓмòµ¥µÄ-Ô²Öܹ«Ê½£¬ÓÖÓи´ÔÓµÄÅ·À¹«Ê½¡¡
"J|y {;mn2R@Z0´ÓʲôʱºòÆðÎÒÃÇ¿ªÊ¼Ñá¶ñÊýѧ£¿ÕâЩ¶«Î÷Ô±¾Èç´ËÃÀÀö£¬Èç´Ë¾«Ãî¡£Õâ¸öµØÇòÉÏÓжàÉÙΰ´óµÄÖÇ»ÛÔøºÄ¾¡Ò»Éú£¬²Å×îÖÕдÏÂÒ»¸öµÈºÅ¡£Ã¿µ±Äã½â²»¿ª·½³ÌµÄʱºò£¬²»·Á»»Ò»¸ö½Ç¶ÈÏ룬ÔÝÇÒ·Å϶ÔÀí¿ÆµÄÑá¶ñºÍ¶Ô¿¼ÊÔµÄÍ´ºÞ¡£ÒòΪÄãÕýÔÚ¼ûÖ¤µÄ£¬ÊÇ¿ÆÑ§µÄÃÀÀöÓëÈËÀàµÄ×ðÑÏ¡£ÂÛÎÄÍø
mqYg2]r^p^Il G&Q
z,Y'eOj^}!Y0
No.10 Ô²µÄÖܳ¤¹«Ê½£¨The Length of the Circumference of a Circle£©ÂÛÎÄÍøqp4Pxd4Y e#K
ÂÛÎÄÍø'a1JI5y,w7G{I'p#vÂÛÎÄÍøR_~0Yn ^
,{/d9F8S%yS0 ÂÛÎÄÍø3ewv| Du-pe8H(v
Õ⹫ʽÔôÅ£±ÆÁË£¬³õÖÐѧµ½ÏÖÔÚ¡£Ä¿Ç°£¬ÈËÀàÒѾÄܵõ½Ô²ÖÜÂʵÄ2061ÒÚλ¾«¶È¡£»¹ÊÇͦÎÞÁĵġ£ÏÖ´ú¿Æ¼¼ÁìÓòʹÓõÄ-Ô²ÖÜÂÊÖµ£¬ÓÐÊ®¼¸Î»ÒѾ×ã¹»ÁË¡£Èç¹ûÓÃ35λ¾«¶ÈµÄ-Ô²ÖÜÂÊÖµ£¬À´¼ÆËãÒ»¸öÄܰÑÌ«Ñôϵ°üÆðÀ´µÄÒ»¸öÔ²µÄÖܳ¤£¬Îó²î»¹²»µ½ÖÊ×ÓÖ±¾¶µÄ°ÙÍò·ÖÖ®Ò»¡£ÏÖÔÚµÄÈ˼ÆËãÔ²ÖÜÂÊ£¬¶àÊýÊÇΪÁËÑéÖ¤¼ÆËã»úµÄ¼ÆËãÄÜÁ¦£¬»¹ÓоÍÊÇΪÁËÐËȤ¡£ÂÛÎÄÍø#X.f%h;S ZpQ(q7f C
ÂÛÎÄÍø4kXzW:C8Z3wk[0X/F7TÂÛÎÄÍø_Fe2e@tuZ
No.9 ¸µÁ¢Ò¶±ä»»£¨The Fourier Transform£©
*^H Sb#T{0%|5h t_7nYW0
$n&Ww [%ZS7OV p0ÂÛÎÄÍø%eY^
Av3@W#d
/s6[[3R2G H0
C7cY] @z O0Õâ¸öͦרҵµÄ£¬Ò»°ãÈËÍêÈ«²»Ã÷°×¡£²»¶à×÷½âÊÍ¡£¼òÒªµØËµÃ»ÓÐÕâ¸öʽ×ÓûÓнñÌìµÄµç×Ó¼ÆËã»ú£¬ËùÒÔÄãÄÜÔÚÕâÀïÉÏÍø³ýÁ˸Ðлµ³¸ÐлÕþ¸®»¹Òª¸ÐлÕâ¸öÍêÈ«¿´²»¶®µÄʽ×Ó¡£ÁíÍ⸵Á¢Ò¶ËäÈ»ÐÕ¸µ£¬µ«ÊÇ·¨¹úÈË¡£ÂÛÎÄÍø"HTk/dl4g
ÂÛÎÄÍømQ(\A.f|;q?L IU s{4Y0
No.8 µÂ²¼ÂÞÒâ·½³Ì×飨The de Broglie Relations£©
0b#PT ex1kk0ÂÛÎÄÍø-N,bJ"f:ojd;U TÂÛÎÄÍøtHOVYR1Y!uZ(G+|
%l'D:s:K\,d|v8I0
QZAtH0Õâ¸ö¶«Î÷Ҳͦţ±ÆµÄ£¬¸ßÖÐÎïÀíѧµ½¹âѧµÄ»°ºÜ¶à¸ÅÄî¸úËüÊÇÔ¶Çס£¼òÒªµØËµµÂ²¼ÂÞÒâÕâÈ˾õµÃµç×Ó²»½öÊÇÒ»¸öÁ£×Ó£¬Ò²ÊÇÒ»ÖÖ²¨£¬Ëü»¹ÓÐ ¡°²¨³¤¡±¡£ÓÚÊǸ㰡¸ã¾ÍÓÐÁËÕâ¸öÎïÖʲ¨·½³Ì£¬±í´ïÁ˲¨³¤¡¢ÄÜÁ¿µÈµÈÖ®¼äµÄ¹ØÏµ¡£Í¬Ê±Ëû»ñµÃÁË1929Äêŵ±´¶ûÎïÀíѧ½±¡£
*^Ca_ c7ct0ÂÛÎÄÍø+WBuZhfSrp3AH^/FjffU$}0
No.7 1+1=2ÂÛÎÄÍø-r^RI-k
Õâ¸ö¹«Ê½²»ÐèÒªÃû³Æ£¬²»ÐèÒª·Ò룬²»ÐèÒª½âÊÍ¡£ÂÛÎÄÍø#^*@}P0]O X DQ
0} Q@ p h4P*u0 ÂÛÎÄÍøeAjNV;MF7h#k
No.6 Ѧ¶¨ÚÌ·½³Ì£¨The Schrödinger Equation£©ÂÛÎÄÍøJKda[
7Jv:~^Xw%gF0
tv*W`$z&rn@m0 ÂÛÎÄÍø(Y:X LL&wv*f GA0fE
Ò²ÊÇÒ»°ãÈËÍêÈ«²»Ã÷°×µÄ¡£Òò´ËÎÒժ¼¹Ù·½ÆÀ¼Û£º¡°Ñ¦¶¨ÚÌ·½³ÌÊÇÊÀ½çÔ×ÓÎïÀíѧÎÄÏ×ÖÐÓ¦ÓÃ×î¹ã·º¡¢Ó°Ïì×î´óµÄ¹«Ê½¡£¡±ÓÉÓÚ¶ÔÁ¿×ÓÁ¦Ñ§µÄ½Ü³ö¹±Ï×£¬Ñ¦¶¨ÚÌ»ñµÃ1933Äêŵ±´¶ûÎïÀí½±¡£ÂÛÎÄÍø!os:tkQL!_G TD
ÁíÍâѦ¶¨ÚÌËäÈ»ÐÕѦ£¬µ«ÊǰµØÀûÈË¡£
]S"XJ Y d(?4x:MJ0
o;i0k0RAR*K/T0No.5 ÖÊÄÜ·½³Ì£¨Mass¨Cenergy Equivalence£©ÂÛÎÄÍø[#qvBHuD9~X#Km
ÂÛÎÄÍøW1O3N p|ÂÛÎÄÍø8E/e.\^}'QaU
bo*xr'`2F0 ÂÛÎÄÍøaJwEJX
ºÃÏñ´ÓÀ´Ã»ÓÐÒ»¸ö¿ÆÑ§½çµÄ¹«Ê½ÓÐÈç´Ë¹ã·ºµÄÒâÒå¡£ÔÚÎïÀíѧ¡°Ææ¼£Äꡱ1905Ä꣬ÓÉÒ»¸ö½Ð×ö°®Òò˹̹µÄÄêÇáÈËÌá³ö¡£Í¬ÄêËû»¹·¢±íÁË¡¶ÂÛ¶¯ÌåµÄµç¶¯Á¦Ñ§¡·¡ª¡ªË׳ÆÏÁÒåÏà¶ÔÂÛ¡£ÂÛÎÄÍøTJQzk4@;sLN-X a
Õâ¸ö¹«Ê½¸æËßÎÒÃÇ£¬°®Òò˹̹ÊÇÅ£±ÆµÄ£¬ÄÜÁ¿ºÍÖÊÁ¿ÊÇ¿ÉÒÔ»¥»»µÄ¡£¸±²úÆ·£ºÔ×Óµ¯¡£ÂÛÎÄÍø7qRWv5tSF
ÂÛÎÄÍø }N"q h8CrZ1^:XÂÛÎÄÍø3pI0T jS!p0\n&A4q6U
No.4 ¹´¹É¶¨Àí/±Ï´ï¸çÀ˹¶¨Àí£¨Pythagorean Theorem£©
xR2P:Hx/t0ÂÛÎÄÍø9rzB6TJpÂÛÎÄÍø&doj#R~,D9E+P3\
ÂÛÎÄÍøWx#i'X ~u9X'}
IP!DR,J}h b,v0
$|%Qsuv0×öÊýѧ²»¿ÉÄÜûÓõ½¹ý°É£¬²»¶à½²ÁË¡£ÂÛÎÄÍø9?@$\P$c,j*e e
4uJXym6Rr0
4F9p3Z{4vP$W}0No.3 Å£¶ÙµÚ¶þ¶¨ÂÉ£¨Newton's Second Law of Motion£©
otw(W"o:|d2c0ÂÛÎÄÍøX2LWj J,SÂÛÎÄÍø9p/^x3Zi{6N6y,N`