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

Short Answer

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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 $$e^{j \pi} = -1 + 0i$$.

Step by step solution

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: $$ e^{j \pi} = -1 + 0i $$

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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

Consider the vibrating system described by the initial value problem $$ u^{\prime \prime}+u=3 \cos \omega t, \quad u(0)=1, \quad u^{\prime}(0)=1 $$ (a) Find the solution for \(\omega \neq 1\). (b) Plot the solution \(u(t)\) versus \(t\) for \(\omega=0.7, \omega=0.8,\) and \(\omega=0.9 .\) Compare the results with those of Problem \(18,\) that is, describe the effect of the nonzero initial conditions.

A spring is stretched \(10 \mathrm{cm}\) by a force of 3 newtons. A mass of \(2 \mathrm{kg}\) is hung from the spring and is also attached to a viscous damper that exerts a force of 3 newtons when the velocity of the mass is \(5 \mathrm{m} / \mathrm{sec}\). If the mass is pulled down \(5 \mathrm{cm}\) below its equilibrium position and given an initial downward velocity of \(10 \mathrm{cm} / \mathrm{sec},\) determine its position \(u\) at any time \(t\) Find the quasi frequency \(\mu\) and the ratio of \(\mu\) to the natural frequency of the corresponding undamped motion.

A mass weighing 16 lb stretches a spring 3 in. The mass is attached to a viscous damper with a damping constant of 2 Ib-sec/ft. If the mass is set in motion from its equilibrium position with a downward velocity of 3 in / sec, find its position \(u\) at any time \(t .\) Plot \(u\) versus \(t\). Determine when the mass first returns to its equilibrium. Also find the time \(\tau\) such that \(|u(t)|<0.01\) in. fir all \(t>\tau\)

A mass weighing 3 Ib stretches a spring 3 in. If the mass is pushed upward, contracting the spring a distance of 1 in, and then set in motion with a downward velocity of \(2 \mathrm{ft}\) sec, and if there is no damping, find the position \(u\) of the mass at any time \(t .\) Determine the frequency, period, amplitude, and phase of the motion.

In the absence of damping the motion of a spring-mass system satisfies the initial value problem $$ m u^{\prime \prime}+k u=0, \quad u(0)=a, \quad u^{\prime}(0)=b $$ (a) Show that the kinetic energy initially imparted to the mass is \(m b^{2} / 2\) and that the potential energy initially stored in the spring is \(k a^{2} / 2,\) so that initially the total energy in the system is \(\left(k a^{2}+m b^{2}\right) / 2\). (b) Solve the given initial value problem. (c) Using the solution in part (b), determine the total energy in the system at any time \(t .\) Your result should confirm the principle of conservation of energy for this system.

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