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

Short Answer

Expert verified
Answer: The polar and exponential form for the complex number -i is 1e^(i(3π/2)).

Step by step solution

01

Find the magnitude (R)

Using the polar representation of complex numbers, R is the magnitude of the complex number. For the complex number, which is given as \(-i\), we can write it as \(0-1i.\) Now, use the formula \(R=\sqrt{a^2+b^2}\) where a is the real part, and b is the imaginary part. In our case, a = 0 and b = -1. So, $$R=\sqrt{(0)^2+(-1)^2} = \sqrt{0+1} = \sqrt{1} =1.$$
02

Find the angle (θ)

To find the angle (θ), we can use the formula \(\theta=\tan^{-1}\frac{b}{a}\), where a is the real part and b is the imaginary part. Keep in mind that we need to consider which quadrant the complex number lies in. Since our complex number is \(-i\), it is in the third quadrant (negative real axis and negative imaginary axis). In our case, a = 0 and b = -1. So, $$\theta=\tan^{-1}\frac{-1}{0}.$$ Since the division by zero is undefined and we know that the complex number is on the negative imaginary axis, we can determine that $$\theta=\frac{3\pi}{2}$$ using the knowledge of the coordinates system and trigonometry.
03

Write the complex number in the desired form

Now that we have the magnitude (R) and the angle (θ), we can write the complex number in the required form: $$R(\cos\theta+\( \)i\sin\theta)=R e^{i\theta}.$$ For our case, R = 1 and θ = \(\frac{3\pi}{2}\). So, $$1(\cos\frac{3\pi}{2} + i\sin\frac{3\pi}{2}) = 1e^{i\frac{3\pi}{2}}.$$ Thus, the desired form for the complex number \(-i\) is: $$-i = 1e^{i\frac{3\pi}{2}}.$$

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Most popular questions from this chapter

verify that the given functions are solutions of the differential equation, and determine their Wronskian. $$ y^{\mathrm{iv}}+y^{\prime \prime}=0 ; \quad 1, \quad t, \quad \cos t, \quad \sin t $$

Find the solution of the given initial value problem. Then plot a graph of the solution. \(y^{\mathrm{iv}}+2 y^{\prime \prime}+y=3 t+4, \quad y(0)=y^{\prime}(0)=0, \quad y^{\prime \prime}(0)=y^{\prime \prime \prime}(0)=1\)

In this problem we show how to generalize Theorem 3.3 .2 (Abel's theorem) to higher order equations. We first outline the procedure for the third order equation $$ y^{\prime \prime \prime}+p_{1}(t) y^{\prime \prime}+p_{2}(t) y^{\prime}+p_{3}(t) y=0 $$ Let \(y_{1}, y_{2},\) and \(y_{3}\) be solutions of this equation on an interval \(I\) (a) If \(W=W\left(y_{1}, y_{2}, y_{3}\right),\) show that $$ W^{\prime}=\left|\begin{array}{ccc}{y_{1}} & {y_{2}} & {y_{3}} \\\ {y_{1}^{\prime}} & {y_{2}^{\prime}} & {y_{3}^{\prime}} \\ {y_{1}^{\prime \prime \prime}} & {y_{2}^{\prime \prime \prime}} & {y_{3}^{\prime \prime \prime}}\end{array}\right| $$ Hint: The derivative of a 3 -by-3 determinant is the sum of three 3 -by-3 determinants obtained by differentiating the first, second, and third rows, respectively. (b) Substitute for \(y_{1}^{\prime \prime \prime}, y_{2}^{\prime \prime \prime},\) and \(y_{3}^{\prime \prime \prime}\) from the differential equation; multiply the first row by \(p_{3},\) the second row by \(p_{2},\) and add these to the last row to obtain $$ W^{\prime}=-p_{1}(t) W $$ (c) Show that $$ W\left(y_{1}, y_{2}, y_{3}\right)(t)=c \exp \left[-\int p_{1}(t) d t\right] $$ It follows that \(W\) is either always zero or nowhere zero on \(I .\) (d) Generalize this argument to the \(n\) th order equation $$ y^{(n)}+p_{1}(t) y^{(n-1)}+\cdots+p_{n}(t) y=0 $$ with solutions \(y_{1}, \ldots, y_{n} .\) That is, establish Abel's formula, $$ W\left(y_{1}, \ldots, y_{n}\right)(l)=c \exp \left[-\int p_{1}(t) d t\right] $$ for this case.

Use Abel’s formula (Problem 20) to find the Wronskian of a fundamental set of solutions of the given differential equation. $$ y^{\mathrm{iv}}+y=0 $$

Find the solution of the given initial value problem. Then plot a graph of the solution. \(y^{\prime \prime \prime}-3 y^{\prime \prime}+2 y^{\prime}=t+e^{t}, \quad y(0)=1, \quad y^{\prime}(0)=-\frac{1}{4}, \quad y^{\prime \prime}(0)=-\frac{3}{2}\)

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