Show that one value of the expression
${{\left( \dfrac{1+\sin \dfrac{\pi }{8}+i\cos \dfrac{\pi }{8}}{1+\sin \dfrac{\pi }{8}-i\cos \dfrac{\pi }{8}} \right)}^{\dfrac{8}{3}}}$ is -1.
Answer
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Hint: Use Euler’s identity ${{e}^{i\theta }}=\cos \theta +i\sin \theta $and ${{i}^{2}}=-1$. Try converting the numerator and denominator in $\cos \theta +i\sin \theta $ form. Use the trigonometric identities $1+\cos \theta =2{{\cos }^{2}}\dfrac{\theta }{2}$ and $\sin \theta =2\sin \dfrac{\theta }{2}\cos \dfrac{\theta }{2}$.
Complete step-by-step answer:
Let \[L=\dfrac{1+\sin \dfrac{\pi }{8}+i\cos \dfrac{\pi }{8}}{1+\sin \dfrac{\pi }{8}-i\cos \dfrac{\pi }{8}}\]
Using $\sin x=\cos \left( \dfrac{\pi }{2}-x \right)$ and $\cos x=\sin \left( \dfrac{\pi }{2}-x \right)$ we get
\[L=\dfrac{1+\cos \dfrac{3\pi }{8}+i\sin \dfrac{3\pi }{8}}{1+\cos \dfrac{3\pi }{8}-i\sin \dfrac{3\pi }{8}}\]
Using $1+\cos \theta =2{{\cos }^{2}}\dfrac{\theta }{2}$ and $\sin \theta =2\sin \dfrac{\theta }{2}\cos \dfrac{\theta }{2}$ we get
$L=\dfrac{2{{\cos }^{2}}\dfrac{3\pi }{16}+2i\sin \dfrac{3\pi }{16}\cos \dfrac{3\pi }{16}}{2{{\cos }^{2}}\dfrac{3\pi }{16}-2i\sin \dfrac{3\pi }{16}\cos \dfrac{3\pi }{16}}$
Taking $2\cos \dfrac{3\pi }{16}$ common from numerator and denominator, we get
$L=\dfrac{2\cos \dfrac{3\pi }{16}\left( \cos \dfrac{3\pi }{16}+i\sin \dfrac{3\pi }{16} \right)}{2\cos \dfrac{3\pi }{16}\left( \cos \dfrac{3\pi }{16}-i\sin \dfrac{3\pi }{16} \right)}$
Simplifying we get
$\begin{align}
& L=\dfrac{{{e}^{i\dfrac{3\pi }{16}}}}{{{e}^{-i\dfrac{3\pi }{16}}}} \\
& ={{e}^{i\dfrac{3\pi }{16}+i\dfrac{3\pi }{16}}} \\
& ={{e}^{i\dfrac{6\pi }{16}}} \\
& ={{e}^{\dfrac{3\pi }{8}}} \\
\end{align}$
Hence ${{\left( \dfrac{1+\sin \dfrac{\pi }{8}+i\cos \dfrac{\pi }{8}}{1+\sin \dfrac{\pi }{8}-i\cos \dfrac{\pi }{8}} \right)}^{\dfrac{8}{3}}}={{L}^{\dfrac{8}{3}}}={{e}^{i\dfrac{3\pi }{8}\times \dfrac{8}{3}}}={{e}^{i\pi }}=\cos \pi +i\sin \pi =-1$
Hence, we have ${{\left( \dfrac{1+\sin \dfrac{\pi }{8}+i\cos \dfrac{\pi }{8}}{1+\sin \dfrac{\pi }{8}-i\cos \dfrac{\pi }{8}} \right)}^{\dfrac{8}{3}}}=-1$.
Note:
[1] Euler’s identity ${{e}^{i\theta }}=\cos \theta +i\sin \theta $
[2] Demovire’s identity ${{\left( \cos x+i\sin x \right)}^{n}}=\cos nx+i\sin nx$
[3] We can use identity $\dfrac{1+\cos x+i\sin x}{1+\cos x-i\sin x}=\cos x+i\sin x$ directly to solve the question. The derivation of the above formula will follow the same steps as done in the above solution.
[4] Complex numbers help in finding the values of $\cos nx$ and $\sin nx$ conveniently and easily.
[5] Every complex number can be written in the form of $r{{e}^{ix}}$ where r is called the modulus of the complex number and x is called the argument of the complex number.
[6] Complex numbers play a role of backbone in calculus and are used in many places.
[7] $\left| z \right|=r$ is the equation of circle centred at (0,0) and radius r in the argand plane.
[8] Complex numbers are used in Calculus e.g. Cauchy residue theorem (Theorem for complex integrals) is used to evaluate some difficult real integrals.
[9] Multiplication by $i$ is equivalent to a rotation of $90{}^\circ $ in the argand plane.
[10] A complex number can be thought of as a vector in the Argand plane. This is why complex numbers follow a similar algebra as vector algebra.
[11] Complex numbers are used in AC circuit analysis etc in physics.
Complete step-by-step answer:
Let \[L=\dfrac{1+\sin \dfrac{\pi }{8}+i\cos \dfrac{\pi }{8}}{1+\sin \dfrac{\pi }{8}-i\cos \dfrac{\pi }{8}}\]
Using $\sin x=\cos \left( \dfrac{\pi }{2}-x \right)$ and $\cos x=\sin \left( \dfrac{\pi }{2}-x \right)$ we get
\[L=\dfrac{1+\cos \dfrac{3\pi }{8}+i\sin \dfrac{3\pi }{8}}{1+\cos \dfrac{3\pi }{8}-i\sin \dfrac{3\pi }{8}}\]
Using $1+\cos \theta =2{{\cos }^{2}}\dfrac{\theta }{2}$ and $\sin \theta =2\sin \dfrac{\theta }{2}\cos \dfrac{\theta }{2}$ we get
$L=\dfrac{2{{\cos }^{2}}\dfrac{3\pi }{16}+2i\sin \dfrac{3\pi }{16}\cos \dfrac{3\pi }{16}}{2{{\cos }^{2}}\dfrac{3\pi }{16}-2i\sin \dfrac{3\pi }{16}\cos \dfrac{3\pi }{16}}$
Taking $2\cos \dfrac{3\pi }{16}$ common from numerator and denominator, we get
$L=\dfrac{2\cos \dfrac{3\pi }{16}\left( \cos \dfrac{3\pi }{16}+i\sin \dfrac{3\pi }{16} \right)}{2\cos \dfrac{3\pi }{16}\left( \cos \dfrac{3\pi }{16}-i\sin \dfrac{3\pi }{16} \right)}$
Simplifying we get
$\begin{align}
& L=\dfrac{{{e}^{i\dfrac{3\pi }{16}}}}{{{e}^{-i\dfrac{3\pi }{16}}}} \\
& ={{e}^{i\dfrac{3\pi }{16}+i\dfrac{3\pi }{16}}} \\
& ={{e}^{i\dfrac{6\pi }{16}}} \\
& ={{e}^{\dfrac{3\pi }{8}}} \\
\end{align}$
Hence ${{\left( \dfrac{1+\sin \dfrac{\pi }{8}+i\cos \dfrac{\pi }{8}}{1+\sin \dfrac{\pi }{8}-i\cos \dfrac{\pi }{8}} \right)}^{\dfrac{8}{3}}}={{L}^{\dfrac{8}{3}}}={{e}^{i\dfrac{3\pi }{8}\times \dfrac{8}{3}}}={{e}^{i\pi }}=\cos \pi +i\sin \pi =-1$
Hence, we have ${{\left( \dfrac{1+\sin \dfrac{\pi }{8}+i\cos \dfrac{\pi }{8}}{1+\sin \dfrac{\pi }{8}-i\cos \dfrac{\pi }{8}} \right)}^{\dfrac{8}{3}}}=-1$.
Note:
[1] Euler’s identity ${{e}^{i\theta }}=\cos \theta +i\sin \theta $
[2] Demovire’s identity ${{\left( \cos x+i\sin x \right)}^{n}}=\cos nx+i\sin nx$
[3] We can use identity $\dfrac{1+\cos x+i\sin x}{1+\cos x-i\sin x}=\cos x+i\sin x$ directly to solve the question. The derivation of the above formula will follow the same steps as done in the above solution.
[4] Complex numbers help in finding the values of $\cos nx$ and $\sin nx$ conveniently and easily.
[5] Every complex number can be written in the form of $r{{e}^{ix}}$ where r is called the modulus of the complex number and x is called the argument of the complex number.
[6] Complex numbers play a role of backbone in calculus and are used in many places.
[7] $\left| z \right|=r$ is the equation of circle centred at (0,0) and radius r in the argand plane.
[8] Complex numbers are used in Calculus e.g. Cauchy residue theorem (Theorem for complex integrals) is used to evaluate some difficult real integrals.
[9] Multiplication by $i$ is equivalent to a rotation of $90{}^\circ $ in the argand plane.
[10] A complex number can be thought of as a vector in the Argand plane. This is why complex numbers follow a similar algebra as vector algebra.
[11] Complex numbers are used in AC circuit analysis etc in physics.
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