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sin(mx)sin(nx), cos(mx)cos(nx), sin(mx)cos(nx) の0から2πまでの積分

準備

準備の準備

$$\begin{eqnarray} \cos{\left(\alpha+\beta\right)}&=&\href{https://shikitenkai.blogspot.com/2019/06/blog-post.html}{ \cos{\left(\alpha\right)}\cos{\left(\beta\right)}-\sin{\left(\alpha\right)}\sin{\left(\beta\right)} } \\\cos{\left(\alpha-\beta\right)}&=&\cos{\left(\alpha\right)}\cos{\left(\beta\right)}+\sin{\left(\alpha\right)}\sin{\left(\beta\right)} \\\sin{\left(\alpha+\beta\right)}&=&\href{https://shikitenkai.blogspot.com/2019/06/blog-post.html}{ \sin{\left(\alpha\right)}\cos{\left(\beta\right)}+\cos{\left(\alpha\right)}\sin{\left(\beta\right)} } \\\sin{\left(\alpha-\beta\right)}&=&\sin{\left(\alpha\right)}\cos{\left(\beta\right)}-\cos{\left(\alpha\right)}\sin{\left(\beta\right)} \end{eqnarray}$$

準備1

$$\begin{eqnarray} \\\cos{\left(\alpha-\beta\right)}-\cos{\left(\alpha+\beta\right)}&=&\cos{\left(\alpha\right)}\cos{\left(\beta\right)}+\sin{\left(\alpha\right)}\sin{\left(\beta\right)} -\left\{\cos{\left(\alpha\right)}\cos{\left(\beta\right)}-\sin{\left(\alpha\right)}\sin{\left(\beta\right)}\right\} \;\cdots\;準備の準備 \\&=&\cancel{\cos{\left(\alpha\right)}\cos{\left(\beta\right)}}+\sin{\left(\alpha\right)}\sin{\left(\beta\right)} \cancel{-\cos{\left(\alpha\right)}\cos{\left(\beta\right)}}+\sin{\left(\alpha\right)}\sin{\left(\beta\right)} \\&=&2\sin{\left(\alpha\right)}\sin{\left(\beta\right)} \\\sin{\left(\alpha\right)}\sin{\left(\beta\right)}&=&\frac{\cos{\left(\alpha-\beta\right)}-\cos{\left(\alpha+\beta\right)}}{2} \end{eqnarray}$$

準備2

$$\begin{eqnarray} \\\cos{\left(\alpha-\beta\right)}+\cos{\left(\alpha+\beta\right)}&=&\cos{\left(\alpha\right)}\cos{\left(\beta\right)}+\sin{\left(\alpha\right)}\sin{\left(\beta\right)} +\left\{\cos{\left(\alpha\right)}\cos{\left(\beta\right)}-\sin{\left(\alpha\right)}\sin{\left(\beta\right)}\right\} \;\cdots\;準備の準備 \\&=&\cos{\left(\alpha\right)}\cos{\left(\beta\right)}+\cancel{\sin{\left(\alpha\right)}\sin{\left(\beta\right)}} +\cos{\left(\alpha\right)}\cos{\left(\beta\right)}-\cancel{\sin{\left(\alpha\right)}\sin{\left(\beta\right)}} \\&=&2\cos{\left(\alpha\right)}\cos{\left(\beta\right)} \\\cos{\left(\alpha\right)}\cos{\left(\beta\right)}&=&\frac{\cos{\left(\alpha-\beta\right)}+\cos{\left(\alpha+\beta\right)}}{2} \end{eqnarray}$$

準備3

$$\begin{eqnarray} \cos{\left(2x\right)}&=&\cos{\left(x+x\right)} \\&=&\cos(x)\cos(x)-\sin(x)\sin(x)\;\cdots\;準備の準備 \\&=&\cos^2{\left(x\right)}-\sin^2(x) \\&=&(1-\sin^2(x))-\sin^2(x) \\&=&1-2\sin^2(x) \\\cos{\left(2x\right)}-1&=&-2\sin^2(x) \\1-\cos{\left(2x\right)}&=&2\sin^2(x) \\\sin^2(x)&=&\frac{1-\cos(2x)}{2}=\frac{1}{2}-\frac{\cos(2x)}{2} \end{eqnarray}$$

準備4

$$\begin{eqnarray} \cos{\left(2x\right)}&=&\cos{\left(x+x\right)} \\&=&\cos(x)\cos(x)-\sin(x)\sin(x)\;\cdots\;準備の準備 \\&=&\cos^2{\left(x\right)}-\sin^2(x) \\&=&\cos^2{\left(x\right)}-\left(1-\cos^2{\left(x\right)}\right) \\&=&2\cos^2(x)-1 \\\cos{\left(2x\right)}+1&=&2\cos^2(x) \\\cos^2(x)&=&\frac{1+\cos(2x)}{2}=\frac{1}{2}+\frac{\cos(2x)}{2} \end{eqnarray}$$

準備5

$$\begin{eqnarray} \\\sin{\left(\alpha-\beta\right)}+\sin{\left(\alpha+\beta\right)}&=& \sin{\left(\alpha\right)}\cos{\left(\beta\right)}-\cos{\left(\alpha\right)}\sin{\left(\beta\right)} +\left\{\sin{\left(\alpha\right)}\cos{\left(\beta\right)}+\cos{\left(\alpha\right)}\sin{\left(\beta\right)}\right\} \;\cdots\;準備の準備 \\&=&\sin{\left(\alpha\right)}\cos{\left(\beta\right)}\cancel{-\cos{\left(\alpha\right)}\sin{\left(\beta\right)}} +\sin{\left(\alpha\right)}\cos{\left(\beta\right)}\cancel{+\cos{\left(\alpha\right)}\sin{\left(\beta\right)}} \\&=&2\sin{\left(\alpha\right)}\cos{\left(\beta\right)} \\\sin{\left(\alpha\right)}\cos{\left(\beta\right)}&=&\frac{\sin{\left(\alpha-\beta\right)}+\sin{\left(\alpha+\beta\right)}}{2} \end{eqnarray}$$

準備6

$$\begin{eqnarray} \sin{\left(2x\right)}&=&\sin{\left(x+x\right)} \\&=&\sin{\left(x\right)}\cos{\left(x\right)}+\cos{\left(x\right)}\sin{\left(x\right)} \;\cdots\;準備の準備 \\&=&2\sin{\left(x\right)}\cos{\left(x\right)} \\\sin{\left(x\right)}\cos{\left(x\right)}&=&\frac{\sin{\left(2x\right)}}{2} \end{eqnarray}$$

\(\sin{\left(m\;x\right)}\sin{\left(n\;x\right)}\)

\(m,n\in\mathbb{N},m\ne n\)

$$\begin{eqnarray} &&\int_{0}^{2\pi}\sin{\left(m\;x\right)}\sin{\left(n\;x\right)}\mathrm{d}x\;\cdots\;m,n\in\mathbb{N},m\ne n \\&=&\int_{0}^{2\pi}\frac{1}{2}\left[ \cos{\left(mx-nx\right)} -\cos{\left(mx+nx\right)} \right]\mathrm{d}x\;\cdots\;準備1 \\&=&\int_{0}^{2\pi}\frac{1}{2}\left[ \cos{\left(\left(m-n\right)\;x\right)} -\cos{\left(\left(m+n\right)\;x\right)} \right]\mathrm{d}x \\&=&\frac{1}{2}\left[ \int_{0}^{2\pi}\cos{\left(\left(m-n\right)\;x\right)}\mathrm{d}x -\int_{0}^{2\pi}\cos{\left(\left(m+n\right)\;x\right)}\mathrm{d}x \right] \\&=&\frac{1}{2}\left[ \left[\frac{1}{m-n}\sin{\left(\left(m-n\right)\;x\right)}\right]_{0}^{2\pi} -\left[\frac{1}{m+n}\sin{\left(\left(m+n\right)\;x\right)}\right]_{0}^{2\pi} \right] \\&=&\frac{1}{2}\left[ \frac{1}{m-n} \left[\sin{\left(\left(m-n\right)\;2\pi\right)} - \sin{\left(\left(m-n\right)\;0\right)}\right] -\frac{1}{m+n} \left[\sin{\left(\left(m+n\right)\;2\pi\right)} - \sin{\left(\left(m+n\right)\;0\right)}\right] \right] \\&=&\frac{1}{2}\left[ \frac{1}{m-n}\left[0-0\right] -\frac{1}{m+n}\left[0-0\right] \right] \\&=&\frac{1}{2}\left[ \frac{0}{m-n} -\frac{0}{m+n} \right] \\&=&\frac{1}{2}\;0 \\&=&0 \end{eqnarray}$$

\(m,n\in\mathbb{N},m= n\)

$$\begin{eqnarray} &&\int_{0}^{2\pi}\sin{\left(m\;x\right)}\sin{\left(n\;x\right)}\mathrm{d}x\;\cdots\;m,n\in\mathbb{N},m=n \\&=&\int_{0}^{2\pi}\sin{\left(m\;x\right)}\sin{\left(m\;x\right)}\mathrm{d}x \\&=&\int_{0}^{2\pi}\sin^2{\left(m\;x\right)}\mathrm{d}x \\&=&\frac{1}{m}\int_{0}^{2m\pi}\sin^2{\left(u\right)}\mathrm{d}u\;\cdots\;u=mx,\frac{\mathrm{d}u}{\mathrm{d}x}=m,\mathrm{d}x=\frac{1}{m}\mathrm{d}u \\&=&\frac{1}{m}\int_{0}^{2m\pi}\left[\frac{1}{2}-\frac{1}{2}\cos{\left(2u\right)}\right]\mathrm{d}u\;\cdots\;準備3 \\&=&\frac{1}{2m}\left[\int_{0}^{2m\pi}\mathrm{d}u-\int_{0}^{2m\pi}\cos{\left(2u\right)}\mathrm{d}u\right] \\&=&\frac{1}{2m}\left[\left[u\right]_{0}^{2m\pi}-\left[\frac{1}{2}\sin{\left(2u\right)}\right]_0^{2m\pi}\right] \\&=&\frac{1}{2m}\left[\left[2m\pi-0\right]-\left[\frac{1}{2}\sin{\left(2\cdot2m\pi\right)}-\frac{1}{2}\sin{\left(2\cdot0\right)}\right]\right] \\&=&\frac{1}{2m}\left[2m\pi-\left[0-0\right]\right] \\&=&\frac{1}{\cancel{2m}}\cancel{2m}\pi \\&=&\pi \end{eqnarray}$$

\(\cos{\left(m\;x\right)}\cos{\left(n\;x\right)}\)

\(m,n\in\mathbb{N},m\ne n\)

$$\begin{eqnarray} &&\int_{0}^{2\pi}\cos{\left(m\;x\right)}\cos{\left(n\;x\right)}\mathrm{d}x\;\cdots\;m,n\in\mathbb{N},m\ne n \\&=&\int_{0}^{2\pi}\frac{1}{2}\left[ \cos{\left(mx-nx\right)} +\cos{\left(mx+nx\right)} \right]\mathrm{d}x\;\cdots\;準備2 \\&=&\int_{0}^{2\pi}\frac{1}{2}\left[ \cos{\left(\left(m-n\right)\;x\right)} +\cos{\left(\left(m+n\right)\;x\right)} \right]\mathrm{d}x \\&=&\frac{1}{2}\left[ \int_{0}^{2\pi}\cos{\left(\left(m-n\right)\;x\right)}\mathrm{d}x +\int_{0}^{2\pi}\cos{\left(\left(m+n\right)\;x\right)}\mathrm{d}x \right] \\&=&\frac{1}{2}\left[ \left[\frac{1}{m-n}\sin{\left(\left(m-n\right)\;x\right)}\right]_{0}^{2\pi} +\left[\frac{1}{m+n}\sin{\left(\left(m+n\right)\;x\right)}\right]_{0}^{2\pi} \right] \\&=&\frac{1}{2}\left[ \frac{1}{m-n} \left[\sin{\left(\left(m-n\right)\;2\pi\right)} - \sin{\left(\left(m-n\right)\;0\right)}\right] +\frac{1}{m+n} \left[\sin{\left(\left(m+n\right)\;2\pi\right)} - \sin{\left(\left(m+n\right)\;0\right)}\right] \right] \\&=&\frac{1}{2}\left[ \frac{1}{m-n}\left[0-0\right] +\frac{1}{m+n}\left[0-0\right] \right] \\&=&\frac{1}{2}\left[ \frac{0}{m-n} +\frac{0}{m+n} \right] \\&=&\frac{1}{2}\;0 \\&=&0 \end{eqnarray}$$

\(m,n\in\mathbb{N},m= n\)

$$\begin{eqnarray} &&\int_{0}^{2\pi}\cos{\left(m\;x\right)}\cos{\left(n\;x\right)}\mathrm{d}x\;\cdots\;m,n\in\mathbb{N},m=n \\&=&\int_{0}^{2\pi}\cos{\left(m\;x\right)}\cos{\left(m\;x\right)}\mathrm{d}x \\&=&\int_{0}^{2\pi}\cos^2{\left(m\;x\right)}\mathrm{d}x \\&=&\frac{1}{m}\int_{0}^{2m\pi}\cos^2{\left(u\right)}\mathrm{d}u\;\cdots\;u=mx,\frac{\mathrm{d}u}{\mathrm{d}x}=m,\mathrm{d}x=\frac{1}{m}\mathrm{d}u \\&=&\frac{1}{m}\int_{0}^{2m\pi}\left[\frac{1}{2}+\frac{1}{2}\cos{\left(2u\right)}\right]\mathrm{d}u\;\cdots\;準備4 \\&=&\frac{1}{2m}\left[\int_{0}^{2m\pi}\mathrm{d}u+\int_{0}^{2m\pi}\cos{\left(2u\right)}\mathrm{d}u\right] \\&=&\frac{1}{2m}\left[\left[u\right]_{0}^{2m\pi}+\left[\frac{1}{2}\sin{\left(2u\right)}\right]_0^{2m\pi}\right] \\&=&\frac{1}{2m}\left[\left[2m\pi-0\right]+\left[\frac{1}{2}\sin{\left(2\cdot2m\pi\right)}-\frac{1}{2}\sin{\left(2\cdot0\right)}\right]\right] \\&=&\frac{1}{2m}\left[2m\pi+\left[0-0\right]\right] \\&=&\frac{1}{\cancel{2m}}\cancel{2m}\pi \\&=&\pi \end{eqnarray}$$

\(\sin{\left(m\;x\right)}\cos{\left(n\;x\right)}\)

\(m,n\in\mathbb{N},m\ne n\)

$$\begin{eqnarray} &&\int_{0}^{2\pi}\sin{\left(m\;x\right)}\cos{\left(n\;x\right)}\mathrm{d}x\;\cdots\;m,n\in\mathbb{N},m\ne n \\&=&\int_{0}^{2\pi}\frac{1}{2}\left[ \sin{\left(mx-nx\right)} +\sin{\left(mx+nx\right)} \right]\mathrm{d}x\;\cdots\;準備5 \\&=&\int_{0}^{2\pi}\frac{1}{2}\left[ \sin{\left((m-n)x\right)} +\sin{\left((m+n)x\right)} \right]\mathrm{d}x \\&=&\frac{1}{2}\left[ \int_{0}^{2\pi}\sin{\left((m-n)x\right)}\mathrm{d}x +\int_{0}^{2\pi}\sin{\left((m+n)x\right)}\mathrm{d}x \right] \\&=&\frac{1}{2}\left[ \left[ \frac{-1}{m-n} \cos{\left((m-n)x\right)} \right]_{0}^{2\pi} +\left[ \frac{-1}{m+n} \cos{\left((m+n)x\right)} \right]_{0}^{2\pi} \right] \\&=&\frac{1}{2}\left[ \frac{-1}{m-n}\left[ \cos{\left((m-n)2\pi\right)}-\cos{\left((m-n)0\right)} \right] +\frac{-1}{m+n}\left[ \cos{\left((m-n)2\pi\right)}-\cos{\left((m-n)0\right)} \right] \right] \\&=&\frac{1}{2}\left[ \frac{-1}{m-n}\left[1-1\right] +\frac{-1}{m+n}\left[1-1\right] \right] \\&=&\frac{1}{2}\left[ \frac{-1}{m-n}0 +\frac{-1}{m+n}0 \right] \\&=&\frac{1}{2}\left[ 0 +0 \right] \\&=&\frac{1}{2}0 \\&=&0 \end{eqnarray}$$

\(m,n\in\mathbb{N},m= n\)

$$\begin{eqnarray} &&\int_{0}^{2\pi}\sin{\left(m\;x\right)}\cos{\left(n\;x\right)}\mathrm{d}x\;\cdots\;m,n\in\mathbb{N},m= n \\&=&\int_{0}^{2\pi}\sin{\left(m\;x\right)}\cos{\left(m\;x\right)}\mathrm{d}x \\&=&\int_{0}^{2\pi}\frac{1}{2}\sin{\left(2m\;x\right)}\mathrm{d}x\;\cdots\;準備6 \\&=&\frac{1}{2}\int_{0}^{4m\pi}\frac{1}{2m}\sin{\left(u\right)}\mathrm{d}u\;\cdots\;u=2mx,\;\frac{\mathrm{d}u}{\mathrm{d}x}=2m,\;\mathrm{d}x=\frac{1}{2m}\mathrm{d}u \\&=&\frac{1}{4m}\left[-\cos{\left(u\right)}\right]_{0}^{4m\pi} \\&=&\frac{1}{4m}\left[-\cos{\left(4m\pi\right)}-\left(-\cos{\left(0\right)}\right)\right] \\&=&\frac{1}{4m}\left[-1-\left(-1\right)\right] \\&=&\frac{1}{4m}\left[-1+1\right] \\&=&\frac{1}{4m}0 \\&=&0 \end{eqnarray}$$

まとめ

$$\begin{eqnarray} m,n\in\mathbb{N} \\\int_{0}^{2\pi}\sin{\left(m\;x\right)}\sin{\left(n\;x\right)}\mathrm{d}x&=& \begin{cases} \pi\;\cdots\;m=n \\0\;\cdots\;m\ne n \end{cases} \\\int_{0}^{2\pi}\cos{\left(m\;x\right)}\cos{\left(n\;x\right)}\mathrm{d}x&=& \begin{cases} \pi\;\cdots\;m=n \\0\;\cdots\;m\ne n \end{cases} \\\int_{0}^{2\pi}\sin{\left(m\;x\right)}\cos{\left(n\;x\right)}\mathrm{d}x&=&0 \end{eqnarray}$$

単位円の半分に収まる(?)正方形の面積は有理数(一辺の長さは無理数(sin(arctan(2))=2/√5))

点\(C\)の位置

$$\begin{eqnarray} &&C(\overline{OF},\overline{CF}) \\&=&C(\cos{(\theta)},\sin{(\theta)}) \end{eqnarray}$$

角\(\theta\)との関係

$$\begin{eqnarray} \frac{\overline{CF}}{\overline{OF}}&=&2\;\cdots\;正方形となるため \\&=&\frac{\sin{(\theta)}}{\cos{(\theta)}} \\&=&\tan{(\theta)} \\\tan^{-1}{(2)}&=&\theta \end{eqnarray}$$

線分\(OF\)の長さ

$$\begin{eqnarray} \overline{OF}&=&\cos{\left(\tan^{-1}{\left(2\right)}\right)} \\&=&\frac{1}{\sqrt{\tan(\tan^{-1}{(2)})^2+1}} \\&&\;\cdots\;\cos{(\theta)}=\frac{1}{\sqrt{\tan^2{\left(\theta\right)}+1}} \\&=&\frac{1}{\sqrt{2^2+1}} \\&=&\frac{1}{\sqrt{5}} \end{eqnarray}$$

線分\(CF\)の長さ

$$\begin{eqnarray} \overline{CF} \\&=&\sin{(\theta)} \\&=&2\cos{(\theta)} \\&=&2\frac{1}{\sqrt{5}} \\&=&\frac{2}{\sqrt{5}} \end{eqnarray}$$

面積\(A_1\)

$$\begin{eqnarray} A_1&=&\overline{CF}^2 \\&=&\left(\frac{2}{\sqrt{5}} \right)^2 \\&=&\frac{2^2}{\left(\sqrt{5}\right)^2} \\&=&\frac{4}{5}\;(=0.8) \end{eqnarray}$$

1/(1+x^2)の[0, t]での定積分がarctan(t)となる話


中心を点\(P\)に持つ円と直線\(g\)との交点\(Q\)を求める.

\(x\)座標を求める. $$\begin{eqnarray} x^2+\left(y+1\right)^2&=&1 \\x^2+\left(\color{red}{\frac{x}{t}-1}\color{black}{}+1\right)^2&=&1\;\cdots\;g:y=\frac{x}{t}-1を代入 \\x^2+\left(\frac{x}{t}\right)^2&=&1 \\x^2\left(1+\frac{1}{t^2}\right)&=&1 \\x^2\left(\frac{t^2+1}{t^2}\right)&=&1 \\x^2&=&\frac{t^2}{t^2+1} \\x&=&\sqrt{\frac{t^2}{t^2+1}}\;\cdots\;x\ge0 \\&=&\frac{t}{\sqrt{t^2+1}} \end{eqnarray}$$ \(y\)座標は\(g\)を用いて求める. $$\begin{eqnarray} y&=&\frac{x}{t}-1 \\&=&\frac{\frac{t}{\sqrt{t^2+1}}}{t}-1 \\&=&\frac{1}{\sqrt{t^2+1}}-1 \end{eqnarray}$$

面積\(A_1\)(=四角形\(ABCO\))を求める.

$$\begin{eqnarray} A_1&=&\overline{OA}\cdot\overline{AB}\;\cdots\;長方形の面積 \\&=&t\cdot\frac{1}{2}\frac{1}{1+t^2} \\&=&\frac{t}{2\left(1+t^2\right)} \end{eqnarray}$$

面積\(A_2\)(=凾数\(f\)と線分\(\overline{CB}\)及び\(y\)軸で囲まれる領域(図の\(x\lt0\)の領域の着色は間違い))を求める.

$$\begin{eqnarray} 2y&=&\frac{1}{1+x^2} \\1+x^2&=&\frac{1}{2y} \\x^2&=&\frac{1}{2y}-1 \\x^2&=&\frac{1}{2y}-1 \\&=&\frac{1-2y}{2y} \\x&=&\sqrt{\frac{1-2y}{2y}} \end{eqnarray}$$ $$\begin{eqnarray} A_2&=&\int_{\frac{1}{2\left(1+t^2\right)}}^{\frac{1}{2}} x\mathrm{d}y \\&=&\int_{\frac{1}{2\left(1+t^2\right)}}^{\frac{1}{2}} \sqrt{\frac{1-2y}{2y}} \mathrm{d}y \\&=&\int_{\sqrt{\frac{1}{\left(1+t^2\right)}}-1}^{0} \sqrt{\frac{1-\left(u+1\right)^2}{\cancel{2y}}}\cancel{\sqrt{2y}}\mathrm{d}u \\&&\;\cdots\;u=\sqrt{2y}-1,\;\frac{\mathrm{d}u}{\mathrm{d}y} =\frac{1}{2}\frac{1}{\sqrt{2y}}\cdot2=\frac{1}{\sqrt{2y}},\;\mathrm{d}y=\sqrt{2y}\mathrm{d}u \\&&\;\cdots\;\frac{1}{2}\rightarrow\sqrt{2\cdot \frac{1}{2}}-1=0 \\&&\;\cdots\;\frac{1}{2\left(1+t^2\right)}\rightarrow\sqrt{2\cdot \frac{1}{2\left(1+t^2\right)}}-1 =\frac{1}{\sqrt{1+t^2}}-1 \\&=&\int_{\frac{1}{\sqrt{1+t^2}}-1}^{0} \sqrt{1-\left(u+1\right)^2}\mathrm{d}u \end{eqnarray}$$

面積\(B_1\)(=三角形\(PQR\))を求める.

$$\begin{eqnarray} B_1&=&\frac{1}{2}\overline{QR}\cdot\overline{PR}\;\cdots\;三角形の面積 \\&=&\frac{1}{2}\cdot\frac{t}{\sqrt{t^2+1}}\cdot\left\{1+\left(\frac{1}{\sqrt{t^2+1}}-1\right)\right\} \\&=&\frac{1}{2}\cdot\frac{t}{\sqrt{t^2+1}}\cdot\frac{1}{\sqrt{t^2+1}} \\&=&\frac{t}{2\left(1+t^2\right)} \end{eqnarray}$$

面積\(B_2\)(=円\(x^2+(y-1)^2=1\)と線分\(\overline{QR}\)及び\(y\)軸で囲まれる領域)を求める.

$$\begin{eqnarray} x^2+\left(y+1\right)^2&=&1 \\x^2&=&1-\left(y+1\right)^2 \\x&=&\sqrt{1-\left(y+1\right)^2} \end{eqnarray}$$ $$\begin{eqnarray} B_2&=&\int_{\frac{1}{\sqrt{t^2+1}}-1}^{0} x \mathrm{d}y \\&=&\int_{\frac{1}{\sqrt{t^2+1}}-1}^{0} \sqrt{1-\left(y+1\right)^2} \mathrm{d}y \end{eqnarray}$$

扇PQRの面積を求める.

$$\begin{eqnarray} 扇PQR&=&半径1の面積\cdot比率=\left(1\cdot1\cdot\pi\right)\cdot\frac{\theta}{2\pi} &=&\frac{\theta}{2} \end{eqnarray}$$

\(\theta\)と\(t\)の関係式を求める.

$$\begin{eqnarray} \tan{\left(\theta\right)}&=&\frac{t-0}{0-(-1)}=\frac{t}{1}=t \\\tan^{-1}{\left(t\right)}&=&\theta \end{eqnarray}$$

扇PQRの面積を介して.

$$\begin{eqnarray} 扇PQR&=&\frac{\theta}{2} \\&=&\frac{\tan^{-1}\left(t\right)}{2} \\&=&B_1+B_2 \\&=&A_1+A_2\;\cdots\;B_1=A_1,\;B_2=A_2 \\&=&\int_0^t \frac{1}{2}\frac{1}{1+x^2}\mathrm{d}x =凾数fの区間[0,t]における定積分 \end{eqnarray}$$ $$\begin{eqnarray} \int_0^t \frac{1}{1+x^2}\mathrm{d}x&=&\tan^{-1}\left(t\right) \end{eqnarray}$$