こんにちは。いろいろ勉強して覚えたことです。忘備録として書いておきます。意外と覚えやすい証明方法ですので, ご参考にしてください。
斜辺ABの長さが1の直角三角形AEBがあり, それが図のように台形ABCDにちょうど収まっているとする。点Eは辺CD上にある。また, ,
,
とする。
このとき,









ここで, 図のように, 点Aから下底へ垂線AFを引くと, 直角三角形ABFができる。このとき,




これより,


が得られる。








が得られる。
最後に,




これまでの証明を利用すると,


右辺の分子分母を


以上より,

このような感じで加法定理が証明できる。
案外覚えやすいので, 覚えられるなら覚えておいた方がいいと思う。
加法定理