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»ó´ë¼ºÀÌ·Ð (Theory of Relativity)

1. °¥¸±·¹¿ÀÀÇ »ó´ë¼ºÀÌ·Ð

Galileo Galilei
(1564-1642)
°¥¸±·¹¿ÀÀÇ »ó´ë·Ð¿¡ ´ëÇÑ °¡¼³
¡°Any two observers moving at constant speed and direction with respect to one another will obtain the same results for all mechanical experiments.¡±
¡°¼­·Î ÀÏÁ¤ÇÑ ¼Óµµ·Î ¿òÁ÷ÀÌ´Â µÎ °üÂûÀÚ´Â ¸ðµç ¿ªÇÐÀû ½ÇÇè¿¡ ´ëÇØ µ¿ÀÏÇÑ °á°ú¸¦ ¾ò°Ô µÈ´Ù.¡±
¼Óµµ´Â Àý´ëÀûÀÎ ¾çÀÌ ¾Æ´Ï´Ù.
¼­·Î¿¡ ´ëÇØ ÀÏÁ¤ÇÑ ¼Óµµ·Î ¿òÁ÷ÀÌ´Â µÎ ÁÂÇ¥°è (°ü¼º°è)¿¡¼­
¹°¸® ¹ýÄ¢Àº µ¿ÀÏÇÏ´Ù.
°¥¸±·¹¿À »ó´ë·Ð¿¡¼­ ¼Óµµ °¡¹ý
°üÃøÀÚµéÀÌ ÃøÁ¤ÇÑ µ¹ÀÇ ¼Óµµ
°¥¸±·¹ÀÌ º¯È¯(Galilean Transformation)
O, O¡¯ : µÎ °üÂûÀÚ
ºñÀ¯:
ÇÑ Çö»ó :
Çѱ¹¾î ¡°»¡°£ Àå¹Ì¡±
¿µ¾î ¡°the red rose¡±
°¥¸±·¹ÀÌ º¯È¯
¹ø¿ª ±ÔÄ¢ : °¥¸±·¹ÀÌ º¯È¯

2. Einstein ÀÇ Æ¯¼ö»ó´ë¼ºÀÌ·Ð (Special Relativity)

NewtonÀÇ ¿îµ¿¹ýÄ¢Àº ¼­·Î ±ÕÀÏÇÑ ¿îµ¿À» ÇÏ´Â µÎ °üÃøÀÚ¿¡°Ô µ¿ÀÏ.
Maxwell ÀüÀÚ±âÇÐ ¹ýÄ¢Àº ±×·± µÎ °üÃøÀÚ¿¡¡¦(»ý·«)

1) ·ÎÄÏÀÌ Áö±¸·ÎºÎÅÍ ¸Ö¾îÁö´Â ¸Ö¾îÁö´Â °æ¿ì :



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