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use Euler’s formula to write the given expression in the form a + ib. $$ e^{2-(x / 2) i} $$

Short Answer

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Question: Rewrite the expression \(e^{2-(x/2)i}\) in the form of \(a + ib\). Answer: \(\cos(2-\frac{x}{2}) + i\sin(2-\frac{x}{2})\).

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01

Apply Euler's formula

First, we apply Euler's formula to the given expression, where \(x = 2 - \frac{x}{2}\). So we have $$ e^{(2-\frac{x}{2})i} = \cos(2-\frac{x}{2}) + i\sin(2-\frac{x}{2}). $$
02

Simplify the expression

We can now rewrite the expression in the form \(a + ib\) by identifying the real and imaginary parts. The real part, \(a\), is given by \(\cos(2-\frac{x}{2})\), and the imaginary part, \(b\), is given by \(\sin(2-\frac{x}{2})\). So the final expression is: $$ a + ib = \cos(2-\frac{x}{2}) + i\sin(2-\frac{x}{2}). $$ Therefore, the given expression \(e^{2-(x/2)i}\) can be written in the form \(a + ib\) as: \(\cos(2-\frac{x}{2}) + i\sin(2-\frac{x}{2})\).

Key Concepts

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

Complex Numbers
Complex numbers are a fundamental concept in mathematics, especially when dealing with problems that extend beyond the real number line. A complex number is typically expressed in the form \(a + ib\), where:
  • \(a\) is the real part
  • \(b\) is the imaginary part
  • \(i\) is the imaginary unit (where \(i^2 = -1\))

Complex numbers allow for the representation of numbers that have both a real and an imaginary component, opening possibilities for solving equations where square roots of negative numbers occur.
In our exercise, we learned how Euler's formula helps transform an exponential expression with imaginary components into a complex number with easily identifiable real and imaginary parts.
Trigonometric Functions
Trigonometric functions, like sine and cosine, are crucial in understanding Euler's formula. They help relate complex exponentials to their equivalent expressions in terms of complex numbers.
In the formula \(e^{ix} = \cos(x) + i \sin(x)\), these functions describe the position of a point on the unit circle:
  • \(\cos(x)\) determines the horizontal coordinate, representing the real part of the complex number.
  • \(\sin(x)\) determines the vertical coordinate, representing the imaginary part.

This relationship also underscores the periodic nature of trigonometric functions, making them indispensable in applications involving rotations and oscillatory phenomena.
In our solution, expressing \(e^{(2-\frac{x}{2})i}\) in terms of sine and cosine allowed us to easily rewrite it in the standard complex form of \(a + ib\).
Exponential Form
The exponential form of complex numbers is another powerful tool for solving and simplifying complex number expressions. Through Euler's formula, \(e^{ix} = \cos(x) + i \sin(x)\), one can represent complex numbers as exponentials, which is often more convenient for multiplication and division.

This form is particularly useful because it allows us to transform intricate trigonometric expressions into a more manageable form. When you encounter a complex number in exponential form, you can quickly see its effect in calculations, such as rotations, by manipulating just the exponent.
  • The base \(e\) (the natural exponential) lends beneficial properties.
  • The imaginary unit \(i\) introduces a phase rotation effect due to its trigonometric equivalence.

In our exercise, recognizing the exponential part \(e^{(2-\frac{x}{2})i}\) was pivotal in leveraging Euler's formula to express the original complex number in an easily understood \(a + ib\) form.

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Most popular questions from this chapter

Verify that the given functions \(y_{1}\) and \(y_{2}\) satisfy the corresponding homogeneous equation; then find a particular solution of the given nonhomogeneous equation. In Problems 19 and \(20 g\) is an arbitrary continuous function. $$ t^{2} y^{\prime \prime}-t(t+2) y^{\prime}+(t+2) y=2 t^{3}, \quad t>0 ; \quad y_{1}(t)=t, \quad y_{2}(t)=t e^{t} $$

A spring-mass system with a hardening spring (Problem 32 of Section 3.8 ) is acted on by a periodic external force. In the absence of damping, suppose that the displacement of the mass satisfies the initial value problem $$ u^{\prime \prime}+u+\frac{1}{5} u^{3}=\cos \omega t, \quad u(0)=0, \quad u^{\prime}(0)=0 $$ (a) Let \(\omega=1\) and plot a computer-generated solution of the given problem. Does the system exhibit a beat? (b) Plot the solution for several values of \(\omega\) between \(1 / 2\) and \(2 .\) Describe how the solution changes as \(\omega\) increases.

Consider a vibrating system described by the initial value problem $$ u^{\prime \prime}+\frac{1}{4} u^{\prime}+2 u=2 \cos \omega t, \quad u(0)=0, \quad u^{\prime}(0)=2 $$ (a) Determine the steady-state part of the solution of this problem. (b) Find the amplitude \(A\) of the steady-state solution in terms of \(\omega\). (c) Plot \(A\) versus \(\omega\). (d) Find the maximum value of \(A\) and the frequency \(\omega\) for which it occurs.

The position of a certain undamped spring-mass system satisfies the initial value problem $$ u^{\prime \prime}+2 u=0, \quad u(0)=0, \quad u^{\prime}(0)=2 $$ (a) Find the solution of this initial value problem. (b) Plot \(u\) versus \(t\) and \(u^{\prime}\) versus \(t\) on the same axes. (c) Plot \(u^{\prime}\) versus \(u ;\) that is, plot \(u(t)\) and \(u^{\prime}(t)\) parametrically with \(t\) as the parameter. This plot is known as a phase plot and the \(u u^{\prime}\) -plane is called the phase plane. Observe that a closed curve in the phase plane corresponds to a periodic solution \(u(t) .\) What is the direction of motion on the phase plot as \(t\) increases?

Consider the initial value problem $$ m u^{\prime \prime}+\gamma u^{\prime}+k u=0, \quad u(0)=u_{0}, \quad u^{\prime}(0)=v_{0} $$ Assume that \(\gamma^{2}<4 k m .\) (a) Solve the initial value problem, (b) Write the solution in the form \(u(t)=R \exp (-\gamma t / 2 m) \cos (\mu t-\delta) .\) Determine \(R\) in terms of \(m, \gamma, k, u_{0},\) and \(v_{0}\). (c) Investigate the dependence of \(R\) on the damping coefficient \(\gamma\) for fixed values of the other parameters.

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