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use Euler’s formula to write the given expression in the form a + ib. $$ e^{j \pi} $$

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**Question:** Use Euler's formula to convert the given expression $$e^{j \pi}$$ into the form $$a + ib$$. **Answer:** Using Euler's formula, we find that $$e^{j \pi} = -1 + 0i$$.

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01

Apply Euler's Formula to the given expression

According to Euler's formula, we have $$e^{jx} = \cos(x) + j\sin(x)$$. We are given the expression $$e^{j \pi}$$. So, we just need to substitute $$x = \pi$$ into the formula: $$ e^{j \pi} = \cos(\pi) + j\sin(\pi) $$
02

Simplify the trigonometric expressions

Now, we need to evaluate the sine and cosine parts of the expression. Recall that: $$ \cos(\pi) = -1 $$ And: $$ \sin(\pi) = 0 $$ Now, substituting these values back into the expression we get: $$ e^{j \pi} = -1 + j(0) $$
03

Finalize the expression in the form a + ib

Since the sine part is zero, the expression becomes: $$ e^{j \pi} = -1 $$ So, in the form $$a + ib$$, we have $$a = -1$$ and $$b = 0$$. The final expression is: $$ e^{j \pi} = -1 + 0i $$

Key Concepts

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

Complex Numbers
Complex numbers are fundamental components of advanced mathematics, especially useful when dealing with phenomena that have two interrelated elements. Each complex number can be expressed in the form of \( a + ib \), where \('a'\) and \('b'\) are real numbers, and \('i'\) is the imaginary unit defined by its property that \('i^2 = -1'\).

When dealing with complex numbers, the real part, \( a \), and the imaginary part, \( ib \), describe different dimensions of a 2D space. This numerical system extends our traditional understanding of the 1D number line to include not just positions along a line (real numbers), but positions on a plane (real and imaginary numbers). In the example \( e^{j \theta} \), the polar form of complex numbers is used where \( j \), like \( i \), represents the square root of -1, and \( \theta \) is the angle in radians formed with the positive real axis.

Understanding the nature of complex numbers is essential for interpreting and solving equations that describe oscillatory motion, waves, and many aspects of electrical engineering, as well as quantum mechanics.
Trigonometric Functions
Trigonometric functions are a crucial tool in connecting angles to ratios of side lengths in right-angled triangles. They have far-reaching applications beyond geometry, into various fields including physics, engineering, and even music theory. The most commonly known trigonometric functions are sine \( (\sin) \), cosine \( (\cos) \) and tangent \((\tan)\).

These functions also define relationships on the unit circle, where the angle \( \theta \) specifies a point on the circumference. The cosine of \( \theta \) then represents the x-coordinate (horizontal) and the sine of \( \theta \) the y-coordinate (vertical) of that point. When analyzing the expression \( e^{j \theta} \), Euler's formula elegantly links complex exponentials to trigonometric functions by equating \( e^{j \theta} = \cos(\theta) + j\sin(\theta) \).

By grasping the fundamentals of trigonometric functions and their application to the unit circle, one can easily transition to understanding more complex mathematical concepts, including Fourier analysis, signal processing, and the behavior of oscillatory systems.
Exponential Functions
Exponential functions are characterized by their rate of growth or decay, which remains proportional to the value of the function itself. The most recognizable base of an exponential function is Euler's number, denoted as \( e \), approximately equal to 2.71828. This irrational and transcendental number has unique properties that make it naturally suited for describing growth processes, compound interest, and complex numbers in the form of \('e^{ix}'\).

In Euler's formula, the representation \( e^{jx} \), where \( x \) is a real number, directly correlates to oscillations when mapped onto a graph because it forms a circle in the complex plane, mirroring the circular nature of trigonometric functions. This relationship between exponential and trigonometric functions becomes especially significant in understanding waveforms and harmonic motion, often employed in electrical engineering and physics.

Learning about exponential functions with basis \( e \) not only provides insights into natural growth and continuous compounding but also equips learners with the knowledge to reconcile real-valued exponential growth with the oscillatory behavior that occurs in complex-valued functions.

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Most popular questions from this chapter

In the spring-mass system of Problem \(31,\) suppose that the spring force is not given by Hooke's law but instead satisfies the relation $$ F_{s}=-\left(k u+\epsilon u^{3}\right) $$ where \(k>0\) and \(\epsilon\) is small but may be of either sign. The spring is called a hardening spring if \(\epsilon>0\) and a softening spring if \(\epsilon<0 .\) Why are these terms appropriate? (a) Show that the displacement \(u(t)\) of the mass from its equilibrium position satisfies the differential equation $$ m u^{\prime \prime}+\gamma u^{\prime}+k u+\epsilon u^{3}=0 $$ Suppose that the initial conditions are $$ u(0)=0, \quad u^{\prime}(0)=1 $$ In the remainder of this problem assume that \(m=1, k=1,\) and \(\gamma=0\). (b) Find \(u(t)\) when \(\epsilon=0\) and also determine the amplitude and period of the motion. (c) Let \(\epsilon=0.1 .\) Plot (a numerical approximation to) the solution. Does the motion appear to be periodic? Estimate the amplitude and period. (d) Repeat part (c) for \(\epsilon=0.2\) and \(\epsilon=0.3\) (e) Plot your estimated values of the amplitude \(A\) and the period \(T\) versus \(\epsilon\). Describe the way in which \(A\) and \(T\), respectively, depend on \(\epsilon\). (f) Repeat parts (c), (d), and (e) for negative values of \(\epsilon .\)

Use the method of Problem 32 to solve the given differential $$ y^{\prime \prime}+2 y^{\prime}+y=2 e^{-t} \quad(\text { see Problem } 6) $$

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?

The differential equation $$ x y^{\prime \prime}-(x+N) y^{\prime}+N y=0 $$ where \(N\) is a nonnegative integer, has been discussed by several authors. 6 One reason it is interesting is that it has an exponential solution and a polynomial solution. (a) Verify that one solution is \(y_{1}(x)=e^{x}\). (b) Show that a second solution has the form \(y_{2}(x)=c e^{x} \int x^{N} e^{-x} d x\). Calculate \(y_{2 (x)\) for \(N=1\) and \(N=2 ;\) convince yourself that, with \(c=-1 / N !\) $$ y_{2}(x)=1+\frac{x}{1 !}+\frac{x^{2}}{2 !}+\cdots+\frac{x^{N}}{N !} $$ Note that \(y_{2}(x)\) is exactly the first \(N+1\) terms in the Taylor series about \(x=0\) for \(e^{x},\) that is, for \(y_{1}(x) .\)

Find the general solution of the given differential equation. $$ u^{n}+\omega_{0}^{2} u=\cos \omega t, \quad \omega^{2} \neq \omega_{0}^{2} $$

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