第3章 3.19

(1)

f=ex(x=1)f = e^x \qquad (x = 1)

f′=exx=1のときf′=ef' = e^x \qquad x = 1 のとき \qquad f' = e

f′′=exx=1のときf′′=ef'' = e^x \qquad x = 1 のとき \qquad f'' = e

これから

f≅e+e(x−1)+e2(x−1)2f \cong e + e(x-1) + \frac{e}{2}(x-1)^2

(2)

f=log⁡x(x=e)f = \log x \qquad (x = e)

f′=1xx=eのときf′=1ef' = \dfrac{1}{x} \qquad x = e のとき \qquad f' = \dfrac{1}{e}

f′′=−1x2x=eのときf′′=−1e2f'' = -\dfrac{1}{x^2} \qquad x = e のとき \qquad f'' = -\dfrac{1}{e^2}

これから

f≅1+1e(x−e)−12e2(x−e)2f \cong 1 + \frac{1}{e}(x-e) - \frac{1}{2e^2}(x-e)^2

(3)

f=sin⁡x(x=π)f = \sin x \qquad (x = \pi)

f′=cos⁡xx=πのときf′=−1f' = \cos x \qquad x = \pi のとき \qquad f' = -1

f′′=−sin⁡xx=πのときf′′=0f'' = -\sin x \qquad x = \pi のとき \qquad f'' = 0

f′′′=−cos⁡xx=πのときf′′′=1f''' = -\cos x \qquad x = \pi のとき \qquad f''' = 1

f(4)=sin⁡xx=πのときf(4)=0f^{(4)} = \sin x \qquad x = \pi のとき \qquad f^{(4)} = 0

f(5)=cos⁡xx=πのときf(5)=−1f^{(5)} = \cos x \qquad x = \pi のとき \qquad f^{(5)} = -1

これから

f≅−(x−π)+13!(x−π)3−15!(x−π)5=−(x−π)+16(x−π)3−1120(x−π)5f \cong -(x-\pi) + \frac{1}{3!}(x-\pi)^3 - \frac{1}{5!}(x-\pi)^5 = -(x-\pi) + \frac{1}{6}(x-\pi)^3 - \frac{1}{120}(x-\pi)^5

(4)

f=cos⁡x(x=π4)f = \cos x \qquad \left(x = \frac{\pi}{4}\right)

f′=−sin⁡xx=π4のときf′=−12f' = -\sin x \qquad x = \frac{\pi}{4}\text{のとき} \qquad f' = -\frac{1}{\sqrt{2}}

f′′=−cos⁡xx=π4のときf′=−12f'' = -\cos x \qquad x = \frac{\pi}{4}\text{のとき} \qquad f' = -\frac{1}{\sqrt{2}}

これから

f≅12−12(x−π4)−122(x−π4)2f \cong \frac{1}{\sqrt{2}} - \frac{1}{\sqrt{2}}\left(x - \frac{\pi}{4}\right) - \frac{1}{2\sqrt{2}}\left(x - \frac{\pi}{4}\right)^2

解説: r31bn1z