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Follow the procedure illustrated in Example 4 to determine the indicated roots of the given complex number. $$ [2(\cos \pi / 3+i \sin \pi / 3)]^{1 / 2} $$

Short Answer

Expert verified
Question: Calculate the square root of the complex number \(2(\cos \pi / 3+i \sin \pi / 3)\). Answer: The square roots of the given complex number are \(\sqrt[\frac{1}{2}]{2} (\cos \frac{2\pi}{3} + i \sin \frac{2\pi}{3})\) and \(\sqrt[\frac{1}{2}]{2} (\cos \frac{4\pi}{3} + i \sin \frac{4\pi}{3})\).

Step by step solution

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01

Identify r, θ, and n

First, let's identify the values for \(r\), \(\theta\), and \(n\) in our complex number. From the given complex number, we have: \(r = 2\) \(\theta = \pi/3\) \(n = 1/2\)
02

Use De Moivre's Theorem formula

We will now apply De Moivre's theorem with the established values. For \(k = 0\): $$ \sqrt[\frac{1}{2}]{2} (\cos \frac{\pi / 3 + 2(0)\pi}{1 / 2} + i \sin \frac{\pi / 3 + 2(0)\pi}{1 / 2}) $$ For \(k = 1\): $$ \sqrt[\frac{1}{2}]{2} (\cos \frac{\pi / 3 + 2(1)\pi}{1 / 2} + i \sin \frac{\pi / 3 + 2(1)\pi}{1 / 2}) $$
03

Calculate the roots

Now we will find the two roots. Root 1 (k=0): $$ \sqrt[\frac{1}{2}]{2} (\cos \frac{2\pi}{3} + i \sin \frac{2\pi}{3}) $$ Root 2 (k=1): $$ \sqrt[\frac{1}{2}]{2} (\cos \frac{4\pi}{3} + i \sin \frac{4\pi}{3}) $$
04

Write the final answer

The two roots of the given complex number are: Root 1: $$ \sqrt[\frac{1}{2}]{2} (\cos \frac{2\pi}{3} + i \sin \frac{2\pi}{3}) $$ Root 2: $$ \sqrt[\frac{1}{2}]{2} (\cos \frac{4\pi}{3} + i \sin \frac{4\pi}{3}) $$

Key Concepts

These are the key concepts you need to understand to accurately answer the question.

De Moivre's Theorem
De Moivre's Theorem elegantly connects complex numbers and trigonometry by providing a formula for raising complex numbers to integer and fractional powers. The theorem is expressed as:
\[ (r(\cos \theta + i \sin \theta))^n = r^n (\cos(n\theta) + i \sin(n\theta)) \]
where:
  • r is the modulus of the complex number
  • θ is the argument, or angle
  • n is the exponent
By using De Moivre's theorem, one can easily compute powers and roots of complex numbers when they are expressed in polar form. In the case of fractional powers, such as determining roots, the theorem requires calculating each possible value of k, where k represents each distinct root. It simplifies the otherwise complex operations through trigonometric functions.
Complex Roots
Finding complex roots refers to the process of discovering multiple values that satisfy an equation involving a complex number, usually when dealing with powers and roots. For example, finding the square roots of a complex number involves finding two different solutions, which may not only have real components but also imaginary ones.

When applying De Moivre's Theorem to find complex roots, you'll deal with the parameter k in a cyclic fashion. For a root of order \( n \), you'll explore solutions for \( k = 0, 1, 2, ..., n-1 \). Each results yields a different angle and thus a distinct root. This cyclical nature reflects the periodicity of trigonometric functions in the complex plane, offering a complete set of roots, which in the context of square roots, typically results in two solutions, as shown in the exercise.
Polar Form
Polar form is an alternative way to express complex numbers. Instead of using the typical Cartesian coordinates \( x + yi \), we use a magnitude and an angle, represented as \( r(\cos \theta + i \sin \theta) \), which can also be simplified as \( r \text{cis} \theta \).

In this context:
  • r is known as the modulus or absolute value of the complex number, denoting its distance from the origin in the complex plane.
  • \(\theta\) is the argument, representing the direction measured as the angle from the positive real axis.
Using polar form allows for more intuitive operations on complex numbers, like multiplication and finding roots. This is particularly useful in trigonometric functions due to their cyclical nature.
Trigonometric Form
The trigonometric form of a complex number is a direct expression involving sines and cosines to reflect its position in the complex plane. It's closely linked to the polar form and is given by \( r(\cos \theta + i \sin \theta) \).

This form highlights:
  • Cosine \(\cos \theta\) denotes the horizontal component, or the real part, of the complex number.
  • Sine \(\sin \theta\) expresses the vertical component, or the imaginary part.
The trigonometric form provides a natural connection to various applications in fields such as physics and engineering, where oscillations and rotations are frequent. It simplifies computation with complex numbers, making it especially beneficial for applying identities and theorems like De Moivre's.

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Most popular questions from this chapter

The purpose of this problem is to show that if \(W\left(y_{1}, \ldots, y_{n}\right)\left(t_{0}\right) \neq 0\) for some \(t_{0}\) in an interval \(I,\) then \(y_{1}, \ldots, y_{n}\) are linearly independent on \(I,\) and if they are linearly independent and solutions of $$ L(y]=y^{(n)}+p_{1}(t) y^{(n-1)}+\cdots+p_{n}(t) y=0 $$ on \(I,\) then \(W\left(y_{1}, \ldots, y_{n}\right)\) is nowhere zero in \(I .\) (a) Suppose that \(W\left(y_{1}, \ldots, y_{n}\right)\left(t_{0}\right) \neq 0,\) and suppose that $$ c_{1} y_{1}(t)+\cdots+c_{n} y_{n}(t)=0 $$ for all \(t\) in \(I\). By writing the equations corresponding to the first \(n-1\) derivatives of Fa. (ii) at \(t_{0}\), show that \(c_{1}=\cdots=c_{n}=0 .\) Therefore, \(y_{1}, \ldots, y_{n}\) are linearly independent. (b) Suppose that \(y_{1}, \ldots, y_{n}\) are linearly independent solutions of Eq. (i). If \(W\left(y_{1}, \ldots, y_{n}\right)\left(t_{0}\right)=0\) for some \(t_{0},\) show that there is a nonzero solution of Eq. (i) satisfying the initial conditions $$ y\left(t_{0}\right)=y^{\prime}\left(t_{0}\right)=\cdots=y^{(n-1)}\left(t_{0}\right)=0 $$ since \(y=0\) is a solution of this initial value problem, the uniqueness part of Theorem 4. 1. I yields a contradiction. Thus \(W\) is never zero.

Determine the general solution of the given differential equation. \(y^{\mathrm{iv}}-4 y^{\prime \prime}=t^{2}+e^{t}\)

Find the general solution of the given differential equation. $$ y^{\mathrm{iv}}+6 y^{\prime \prime \prime}+17 y^{\prime \prime}+22 y^{\prime}+14 y=0 $$

Consider the nonhomogeneous \(n\) th order linear differential equation $$ a_{0} y^{(n)}+a_{1} y^{(n-1)}+\cdots+a_{n} y=g(t) $$ where \(a_{0}, \ldots, a_{n}\) are constants. Verify that if \(g(t)\) is of the form $$ e^{\alpha t}\left(b_{0} t^{m}+\cdots+b_{m}\right) $$ then the substitution \(y=e^{\alpha t} u(t)\) reduces the preceding equation to the form $$ k_{0} u^{(n)}+k_{1} u^{(n-1)}+\cdots+k_{n} u=b_{0} t^{m}+\cdots+b_{m} $$ where \(k_{0}, \ldots, k_{n}\) are constants. Determine \(k_{0}\) and \(k_{n}\) in terms of the \(a^{\prime}\) 's and \(\alpha .\) Thus the problem of determining a particular solution of the original equation is reduced to the simpler problem of determining a particular solution of an equation with constant coefficients and a polynomial for the nonhomogeneous term.

Express the given complex number in the form \(R(\cos \theta+\) \(i \sin \theta)=R e^{i \theta}\) $$ \sqrt{3}-i $$

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