第1章 1.16

(1)

y=ex+2e−xy = e^x + 2e^{-x}

y′=ex−2e−xy′′=ex+2e−xy' = e^x - 2e^{-x} \qquad y'' = e^x + 2e^{-x}

y′=0y'=0 のとき ex−2e−x=0e^x - 2e^{-x} = 0 ex=2e−xe^x = 2e^{-x} log⁡ex=log⁡2e−x=log⁡2+log⁡e−x\log e^x = \log 2e^{-x} = \log 2 + \log e^{-x}

x=log⁡2−x∴x=12log⁡2x = \log 2 - x \qquad \therefore x = \frac{1}{2}\log 2

x=12log⁡2x = \dfrac{1}{2}\log 2 のとき y′′=e12log⁡2+2e−12log⁡2>0y'' = e^{\frac{1}{2}\log 2} + 2e^{-\frac{1}{2}\log 2} > 0 (極小)

これから x=12log⁡2x = \dfrac{1}{2}\log 2 のとき極小値

y=e12log⁡2+2e−12log⁡2=elog⁡2+2elog⁡12=2+22=22y = e^{\frac{1}{2}\log 2} + 2e^{-\frac{1}{2}\log 2} = e^{\log\sqrt{2}} + 2e^{\log\frac{1}{\sqrt{2}}} = \sqrt{2} + \frac{2}{\sqrt{2}} = 2\sqrt{2}

(2)

y=e−xsin⁡x(0≤x≤2π)y = e^{-x}\sin x \qquad (0 \le x \le 2\pi)

y′=−e−xsin⁡x+e−xcos⁡xy′′=−(−e−xsin⁡x+e−xcos⁡x)−e−xcos⁡x+e−x(−sin⁡x)=−2e−xcos⁡xy' = -e^{-x}\sin x + e^{-x}\cos x \qquad y'' = -(-e^{-x}\sin x + e^{-x}\cos x) - e^{-x}\cos x + e^{-x}(-\sin x) = -2e^{-x}\cos x

y′=0y'=0 のとき −e−xsin⁡x+e−xcos⁡x=0-e^{-x}\sin x + e^{-x}\cos x = 0 −e−x(sin⁡x−cos⁡x)=0-e^{-x}(\sin x - \cos x) = 0 ∴x=π4,54π\therefore x = \dfrac{\pi}{4}, \dfrac{5}{4}\pi

x=π4x = \dfrac{\pi}{4} のとき y′′=−2e−π4⋅cos⁡π4=−2e−π4<0y'' = -2e^{-\frac{\pi}{4}} \cdot \cos\dfrac{\pi}{4} = -\sqrt{2}e^{-\frac{\pi}{4}} < 0 (極大)

x=54πx = \dfrac{5}{4}\pi のとき y′′=−2e−54πcos⁡54π=2e−54π>0y'' = -2e^{-\frac{5}{4}\pi} \cos\dfrac{5}{4}\pi = \sqrt{2}e^{-\frac{5}{4}\pi} > 0 (極小)

これから

x=π4x = \dfrac{\pi}{4} のとき極大値 y=12e−π4y = \dfrac{1}{\sqrt{2}}e^{-\frac{\pi}{4}} x=54πx = \dfrac{5}{4}\pi のとき極小値 y=−12e−54πy = -\dfrac{1}{\sqrt{2}}e^{-\frac{5}{4}\pi}

(3)

y=2sin⁡x+cos⁡2x(0≤x≤2π)y = 2\sin x + \cos^2 x \qquad (0 \le x \le 2\pi)

y′=2cos⁡x−2cos⁡x⋅sin⁡xy′′=−2sin⁡x+2sin⁡x⋅sin⁡x−2cos⁡x⋅cos⁡xy' = 2\cos x - 2\cos x \cdot \sin x \qquad\qquad y'' = -2\sin x + 2\sin x \cdot \sin x - 2\cos x \cdot \cos x

y′=0y'=0 のとき 2cos⁡x−2cos⁡x⋅sin⁡x=02\cos x - 2\cos x \cdot \sin x = 0 2cos⁡x(1−sin⁡x)=02\cos x(1-\sin x)=0 cos⁡x=0, sin⁡x=1\cos x=0,\ \sin x=1

∴ x=π2, 32π\therefore\ x = \frac{\pi}{2},\ \frac{3}{2}\pi

x=π2x=\dfrac{\pi}{2} のとき y′′=−2sin⁡π2+2sin⁡2π2−2cos⁡2π2=−2+2=0y'' = -2\sin\dfrac{\pi}{2}+2\sin^2\dfrac{\pi}{2}-2\cos^2\dfrac{\pi}{2} = -2+2=0

x=32πx=\dfrac{3}{2}\pi のとき y′′=−2sin⁡32π+2sin⁡232π−2cos⁡232π=2+2=4>0y'' = -2\sin\dfrac{3}{2}\pi+2\sin^2\dfrac{3}{2}\pi-2\cos^2\dfrac{3}{2}\pi = 2+2=4>0 (極小)

これから

x=π2x=\dfrac{\pi}{2} のとき極大値 y=2y=2 x=32πx=\dfrac{3}{2}\pi のとき極小値 y=−2y=-2

解説: r31bn1z