Warning: foreach() argument must be of type array|object, bool given in /var/www/html/web/app/themes/studypress-core-theme/template-parts/header/mobile-offcanvas.php on line 20

Follow the procedure illustrated in Example 4 to determine the indicated roots of the given complex number. $$ 1^{1 / 4} $$

Short Answer

Expert verified
Answer: The fourth roots of the complex number 1 are: 1. \(1(\cos(0) + i\sin(0))\). 2. \(1(\cos(\frac{1}{2}) + i\sin(\frac{1}{2}))\). 3. \(1(\cos(1) + i\sin(1))\). 4. \(1(\cos(\frac{3}{2}) + i\sin(\frac{3}{2}))\).

Step by step solution

01

Convert the given complex number to polar form

To find the roots, we first need to convert the given complex number to its polar form. The complex number is 1, which can be represented as \(1 + 0i\). In polar form, we represent a complex number as \(r(\cos(\theta) + i\sin(\theta))\), where \(r\) is the magnitude and \(\theta\) is the angle. The magnitude (r) can be calculated using the formula \(r =\sqrt{a^2 + b^2}\), where \(a\) and \(b\) are the real and imaginary parts of the complex number, respectively. In this case, \(a = 1\) and \(b = 0\). $$ r = \sqrt{1^2 + 0^2} = \sqrt{1} = 1 $$ The angle \((\theta)\) can be calculated using the formula \(\theta = \arctan(\frac{b}{a})\). In this case, since \(a = 1\) and \(b = 0\), the angle is: $$ \theta = \arctan(\frac{0}{1}) = 0 $$ So, the polar form of the given complex number is \(1(\cos(0) + i\sin(0))\).
02

Use De Moivre's theorem to find the fourth roots

According to De Moivre's theorem, to find the n-th root of a complex number in polar form, we should divide the angle \((\theta)\) by n and raise the magnitude \((r)\) to the power of \(\frac{1}{n}\). In this case, we want to find the fourth roots, so \(n = 4\). For each root, the angle will be: $$ \theta_k = \frac{(2k + 0)}{4} = \frac{2k}{4}, \qquad k = 0, 1, 2, 3 $$ Also, the magnitude of the roots will be: $$ r_k = (1)^{\frac{1}{4}} = 1 $$ Now we can find the fourth roots: 1. \(k = 0\): \(\theta_0 = \frac{2\cdot 0}{4} = 0\), so the root is \(1(\cos(0) + i\sin(0))\). 2. \(k = 1\): \(\theta_1 = \frac{2\cdot 1}{4} = \frac{1}{2}\), so the root is \(1(\cos(\frac{1}{2}) + i\sin(\frac{1}{2}))\). 3. \(k = 2\): \(\theta_2 = \frac{2\cdot 2}{4} = 1\), so the root is \(1(\cos(1) + i\sin(1))\). 4. \(k = 3\): \(\theta_3 = \frac{2\cdot 3}{4} = \frac{3}{2}\), so the root is \(1(\cos(\frac{3}{2}) + i\sin(\frac{3}{2}))\).
03

Writing the roots in rectangular form (optional)

If you need the roots in rectangular form (a + bi), you can use the trigonometric identities: $$ \cos(\frac{n\pi}{4}) = \frac{a}{\sqrt{1 + a^2}} $$ and $$ \sin(\frac{n\pi}{4}) = \frac{a\sqrt{1 - a^2}}{1+a^2}. $$ However, since the question doesn't specifically ask for the roots in rectangular form, we'll leave them in polar form. So, the fourth roots of the given complex number 1 are: 1. \(1(\cos(0) + i\sin(0))\). 2. \(1(\cos(\frac{1}{2}) + i\sin(\frac{1}{2}))\). 3. \(1(\cos(1) + i\sin(1))\). 4. \(1(\cos(\frac{3}{2}) + i\sin(\frac{3}{2}))\).

Unlock Step-by-Step Solutions & Ace Your Exams!

  • Full Textbook Solutions

    Get detailed explanations and key concepts

  • Unlimited Al creation

    Al flashcards, explanations, exams and more...

  • Ads-free access

    To over 500 millions flashcards

  • Money-back guarantee

    We refund you if you fail your exam.

Over 30 million students worldwide already upgrade their learning with Vaia!

Key Concepts

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

Polar Form
To understand complex numbers fully, it's important to know how to convert them into polar form. A complex number like 1 can be expressed as 1 + 0i in its basic rectangular form. In polar terms, it's represented as \( r(\cos(\theta) + i\sin(\theta)) \). Here, \( r \) is the magnitude and \( \theta \) is the angle (often called the argument).
The magnitude \( r \) is found using the formula \( r = \sqrt{a^2 + b^2} \), where \( a \) is the real part, and \( b \) is the imaginary part of the number.
For the number 1, since \( a = 1 \) and \( b = 0 \), we get \( r = \sqrt{1^2 + 0^2} = 1 \).
The angle \( \theta \) is calculated as \( \theta = \arctan(\frac{b}{a}) \). Here, that means \( \theta = \arctan(\frac{0}{1}) = 0 \).
  • The polar form of 1 is thus \( 1(\cos(0) + i\sin(0)) \).
This shows how a number in geometric form gives intuitive insight into its size and direction.
De Moivre's Theorem
De Moivre's theorem is a powerful tool that simplifies many operations on complex numbers when they are in polar form. It's used to find powers and roots of complex numbers.
According to this theorem, if you have a complex number in the form of \( r(\cos(\theta) + i\sin(\theta)) \), its \( n \)-th root is determined by:
  • New magnitude: \( r^{1/n} \)
  • New angles: \( \frac{\theta + 2k\pi}{n} \), where \( k \) is an integer.
The theorem works because of the periodic nature of trigonometric functions, making it possible to rotate the angle sufficiently to get all necessary roots.
In our example, we find the fourth roots of 1 by dividing the angle by 4 while maintaining a magnitude of 1. We compute four roots by substituting \( k = 0, 1, 2, 3 \).
Fourth Roots
To understand the fourth roots of a complex number, such as 1, one can use both geometric and algebraic perspectives. The fourth roots, viewed geometrically, are points evenly spaced on a circle in the complex plane.
For a complex number of magnitude 1 like in this example, every root has a magnitude of \( 1^{1/4} = 1 \).
What varies is the angle: we compute four distinct angles by using \( \theta_k = \frac{2k\pi}{4} \) for \( k = 0, 1, 2, 3 \).
  • \( k = 0 \) gives angle \( 0 \). Root is \( 1(\cos(0) + i\sin(0)) \).
  • \( k = 1 \) gives angle \( \frac{\pi}{2} \). Root is \( 1(\cos(\frac{\pi}{2}) + i\sin(\frac{\pi}{2})) \).
  • \( k = 2 \) gives angle \( \pi \). Root is \( 1(\cos(\pi) + i\sin(\pi)) \).
  • \( k = 3 \) gives angle \( \frac{3\pi}{2} \). Root is \( 1(\cos(\frac{3\pi}{2}) + i\sin(\frac{3\pi}{2})) \).
These angles demonstrate the calculation of roots in their pure polar form.
Rectangular Form
Complex numbers are often represented in what's called rectangular form, which is \( a + bi \). To shift from polar to rectangular form, we apply trigonometric functions to get the Cartesian coordinates \( a \) and \( b \).
For a complex number \( r(\cos(\theta) + i\sin(\theta)) \), we find it in rectangular form by calculating:
  • \( a = r\cos(\theta) \)
  • \( b = r\sin(\theta) \)
This converts each point in polar coordinates into a point on the complex plane.
For instance, the polar root \( 1(\cos(\frac{\pi}{2}) + i\sin(\frac{\pi}{2})) \) translates to \( 0 + i \cdot 1 \), or just \( i \) in rectangular form.
This process helps in visualizing and performing arithmetic on complex roots.

One App. One Place for Learning.

All the tools & learning materials you need for study success - in one app.

Get started for free

Most popular questions from this chapter

We consider another way of arriving at the proper form of \(Y(t)\) for use in the method of undetermined coefficients. The procedure is based on the observation that exponential, polynomial, or sinusoidal terms (or sums and products of such terms) can be viewed as solutions of certain linear homogeneous differential equations with constant coefficients. It is convenient to use the symbol \(D\) for \(d / d t\). Then, for example, \(e^{-t}\) is a solution of \((D+1) y=0 ;\) the differential operator \(D+1\) is said to annihilate, or to be an annihilator of, \(e^{-t}\). Similarly, \(D^{2}+4\) is an annihilator of \(\sin 2 t\) or \(\cos 2 t,\) \((D-3)^{2}=D^{2}-6 D+9\) is an annihilator of \(e^{3 t}\) or \(t e^{3 t},\) and so forth. Show that linear differential operators with constant coefficients obey the commutative law, that is, $$ (D-a)(D-b) f=(D-b)(D-a) f $$ for any twice differentiable function \(f\) and any constants \(a\) and \(b .\) The result extends at once to any finite number of factors.

Find the general solution of the given differential equation. $$ 12 y^{\mathrm{iv}}+31 y^{\prime \prime \prime}+75 y^{\prime \prime}+37 y^{\prime}+5 y=0 $$

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

Find the general solution of the given differential equation. $$ y^{\mathrm{vi}}-y^{\prime \prime}=0 $$

Consider the spring-mass system, shown in Figure \(4.2 .4,\) consisting of two unit masses suspended from springs with spring constants 3 and \(2,\) respectively. Assume that there is no damping in the system. (a) Show that the displacements \(u_{1}\) and \(u_{2}\) of the masses from their respective equilibrium positions satisfy the equations $$ u_{1}^{\prime \prime}+5 u_{1}=2 u_{2}, \quad u_{2}^{\prime \prime}+2 u_{2}=2 u_{1} $$ (b) Solve the first of Eqs. (i) for \(u_{2}\) and substitute into the second equation, thereby obtaining the following fourth order equation for \(u_{1}:\) $$ u_{1}^{\mathrm{iv}}+7 u_{1}^{\prime \prime}+6 u_{1}=0 $$ Find the general solution of Eq. (ii). (c) Suppose that the initial conditions are $$ u_{1}(0)=1, \quad u_{1}^{\prime}(0)=0, \quad u_{2}(0)=2, \quad u_{2}^{\prime}(0)=0 $$ Use the first of Eqs. (i) and the initial conditions (iii) to obtain values for \(u_{1}^{\prime \prime}(0)\) and \(u_{1}^{\prime \prime \prime}(0)\) Then show that the solution of Eq. (ii) that satisfies the four initial conditions on \(u_{1}\) is \(u_{1}(t)=\cos t .\) Show that the corresponding solution \(u_{2}\) is \(u_{2}(t)=2 \cos t .\) (d) Now suppose that the initial conditions are $$ u_{1}(0)=-2, \quad u_{1}^{\prime}(0)=0, \quad u_{2}(0)=1, \quad u_{2}^{\prime}(0)=0 $$ Proceed as in part (c) to show that the corresponding solutions are \(u_{1}(t)=-2 \cos \sqrt{6} t\) and \(u_{2}(t)=\cos \sqrt{6} t\) (e) Observe that the solutions obtained in parts (c) and (d) describe two distinct modes of vibration. In the first, the frequency of the motion is \(1,\) and the two masses move in phase, both moving up or down together. The second motion has frequency \(\sqrt{6}\), and the masses move out of phase with each other, one moving down while the other is moving up and vice versa. For other initial conditions, the motion of the masses is a combination of these two modes.

See all solutions

Recommended explanations on Math Textbooks

View all explanations

What do you think about this solution?

We value your feedback to improve our textbook solutions.

Study anywhere. Anytime. Across all devices.

Sign-up for free