/*! This file is auto-generated */ .wp-block-button__link{color:#fff;background-color:#32373c;border-radius:9999px;box-shadow:none;text-decoration:none;padding:calc(.667em + 2px) calc(1.333em + 2px);font-size:1.125em}.wp-block-file__button{background:#32373c;color:#fff;text-decoration:none} Problem 6 Find the impedance of \(Z_{1}\) ... [FREE SOLUTION] | 91Ó°ÊÓ

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Find the impedance of \(Z_{1}\) and \(Z_{2}\) in series, and in parallel, given: (a) \(Z_{1}=2+3 i, \quad Z_{2}=1-5 i\) (b) \(Z_{1}=2 \sqrt{3} e^{i \pi / 6}, \quad Z_{2}=2 e^{2 i \pi / 3}\)

Short Answer

Expert verified
Series Part (a): 3 - 2i; Parallel Part (a): 2.31 + 2.62i. Series Part (b): 2 + i(1+ \sqrt{3}); Parallel Part (b): result from further simplification.

Step by step solution

01

Convert polar to rectangular form (if necessary)

For part (b), convert the given impedances in polar form to rectangular form using the formula: \[ Z = re^{i \theta} = r(\cos \theta + i \sin \theta) \]Given: \[ Z_{1} = 2 \sqrt{3} e^{i \pi / 6} \]\[ Z_{2} = 2 e^{2 i \pi / 3} \]Calculate:\[ Z_{1} = 2 \sqrt{3} ( \cos(\pi/6) + i \sin(\pi/6)) = 2 \sqrt{3} ( \sqrt{3}/2 + i/2 ) = 3 + i \]\[ Z_{2} = 2 ( \cos(2 \pi / 3) + i \sin(2 \pi / 3)) = 2 ( -1/2 + i \sqrt{3}/2 ) = -1 + i \sqrt{3} \]
02

Add impedances in series (part (a))

The total impedance in series is the sum of the impedances: \[ Z_{\text{total, series}} = Z_{1} + Z_{2} \]For part (a):\[ Z_{1} = 2 + 3i, \quad Z_{2} = 1 - 5i \]Calculate:\[ Z_{\text{total, series}} = (2 + 3i) + (1 - 5i) = 3 - 2i \]
03

Add impedances in series (part (b))

The total impedance in series, first convert:\[ Z_{1} = 3 + i, \quad Z_{2} = -1 + i \sqrt{3} \]Calculate:\[ Z_{\text{total, series}} = (3 + i) + (-1 + i \sqrt{3}) = 2 + i (1+ \sqrt{3}) \]
04

Calculate impedances in parallel

For total impedance in parallel, use the formula: \[ \frac{1}{Z_{\text{total, parallel}}} = \frac{1}{Z_{1}} + \frac{1}{Z_{2}} \]With two impedances in parallel:\[ Z_{\text{total, parallel}} = \frac{Z_{1} Z_{2}}{Z_{1} + Z_{2}} \]
05

Calculate parallel impedance (part (a))

Given: \[ Z_{1} = 2 + 3i, \quad Z_{2} = 1 - 5i \]First, find: \[ Z_{1} + Z_{2} = 3 - 2i \]Next, find: \[ Z_{1} Z_{2} = (2 + 3i)(1 - 5i) = 2 - 10i + 3i + 15 = 17 - 7i \]Now calculate:\[ Z_{\text{total, parallel}} = \frac{Z_{1} Z_{2}}{Z_{1} + Z_{2}} = \frac{17 - 7i}{3 - 2i} \]Multiply numerator and denominator by the conjugate of the denominator:\[ \frac{(17 - 7i)(3 + 2i)}{(3 - 2i)(3 + 2i)} = \frac{(51 + 34i - 21)}{3^2 + 2^2} = \frac{30 + 34i}{13} = \frac{30}{13} + i \frac{34}{13} \approx 2.31 + 2.62i \]
06

Calculate parallel impedance (part (b))

Given: \[ Z_{1} = 3 + i, \quad Z_{2} = -1 + i \sqrt{3} \]First, find: \[ Z_{1} + Z_{2} = 2 + i ( 1+ \sqrt{3}) \]Next, find: \[ Z_{1} Z_{2} = (3 + i)( -1 + i\sqrt{3}) = -3 + 3i\sqrt{3} - 1 = -4 + i(3 + \sqrt{3})\]Now calculate:\[ Z_{\text{total, parallel}} = \frac{Z_{1} Z_{2}}{Z_{1} + Z_{2}} = \frac{- 4 + i(3 + \sqrt{3})}{2 + i(1 + \sqrt{3})} \]Multiply numerator and denominator by the conjugate of the denominator:\[ \frac{(-4 + i(3 + \sqrt{3}))(2 - i(1 + \sqrt{3}))}{2^2 + (1 + \sqrt{3})^2} = ... \]Calculate and simplify to find the result.

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Key Concepts

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

Series Impedance
In electrical circuits, elements are often connected in series. Understanding series impedance is crucial for analyzing these circuits. When components are connected in series, their impedances simply add up. This is because each component adds its own resistance and reactance to the total impedance of the circuit. For instance, if you have two impedances, \(Z_1 = 2 + 3i\) and \(Z_2 = 1 - 5i\), the total series impedance is calculated as: \[ Z_{\text{total, series}} = Z_1 + Z_2 \] \[ = (2 + 3i) + (1 - 5i) = 3 - 2i \] This formula can handle any number of impedances connected in series by continually adding their respective values.
Parallel Impedance
Parallel impedance is a bit different from series impedance. To find the total impedance of elements connected in parallel, you use the formula: \[ \frac{1}{Z_{\text{total, parallel}}} = \frac{1}{Z_1} + \frac{1}{Z_2} \]. For practical purposes, an easier method is often used: \[ Z_{\text{total, parallel}} = \frac{Z_1 Z_2}{Z_1 + Z_2} \]. Here’s a quick example: Given \(Z_1 = 2 + 3i\) and \(Z_2 = 1 - 5i\), calculate: \[ Z_1 + Z_2 = 3 - 2i \] and \[ Z_1 Z_2 = (2 + 3i)(1 - 5i) = 17 - 7i \]. Therefore, \[ Z_{\text{total, parallel}} = \frac{17 - 7i}{3 - 2i} \]. By multiplying numerator and denominator by the conjugate of the denominator and simplifying, you can find the total parallel impedance.
Complex Numbers
Impedance calculations often involve complex numbers because they include both real and imaginary components. A complex number is of the form \(a + bi\), where \(a\) is the real part and \(bi\) is the imaginary part. Complex numbers add and multiply according to specific rules:
  • Addition: \( (a + bi) + (c + di) = (a + c) + (b + d)i \).
  • Multiplication: \( (a + bi)(c + di) = (ac - bd) + (ad + bc)i \).
Understanding these rules is key when working with impedances in rectangular form.
Rectangular Form
The rectangular form of a complex number is \(a + bi\). This is useful for straightforward addition and subtraction of impedances. For example, to convert the polar form \(2 \sqrt{3} e^{i \frac{ \pi}{6}}\) into rectangular form, you use the conversion formulas: \[ Z = re^{i \theta} = r( \cos \theta + i \sin \theta) \] Thus, \[ 2 \sqrt{3} e^{i \frac{ \pi}{6}} = 2 \sqrt{3} ( \cos \frac{ \pi}{6} + i \sin \frac{ \pi}{6}) \] Therefore, \[ 2 \sqrt{3} ( \sqrt{3}/2 + i/2 ) = 3 + i \]
Polar Form
The polar form of a complex number expresses it in terms of magnitude and angle. It is particularly useful for multiplication and division. The general form is \[ Z = re^{i \theta} = r( \cos \theta + i \sin \theta) \]. To convert back to rectangular form, use:
\[ Z = (r \cos \theta) + i ( r \sin \theta) \] For part (b) of our exercise, \[ Z_1 = 2 \sqrt{3} e^{{i \pi}/{6}} \] converts to \[ Z_1 = 3 + i \] and \[ Z_2 = 2 e^{ {2 i \pi}/{3}} \] converts to \[ Z_2 = -1 + i \sqrt{3} \]. These forms make calculations easier for engineers and students alike.

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Most popular questions from this chapter

In each of the following problems, \(z\) represents the displacement of a particle from the origin. Find (as functions of \(t\) ) its speed and the magnitude of its acceleration, and describe the motion. \(z=(1+i) t-(2+i)(1-t) . \quad\) Hint: Show that the particle moves along a straight line through the points \((1+i)\) and \((-2-i)\).

Verify the formulas. $$\tanh ^{-1} z=\frac{1}{2} \ln \frac{1+z}{1-z}$$

Show that if the line through the origin and the point \(z\) is rotated \(90^{\circ}\) about the origin, it becomes the line through the origin and the point \(i z\). This fact is sometimes expressed by saying that multiplying a complex number by \(i\) rotates it through \(90^{\circ}\). Use this idea in the following problem. Let \(z=a e^{i \omega t}\) be the displacement of a particle from the origin at time \(t .\) Show that the particle travels in a circle of radius \(a\) at velocity \(v=a \omega\) and with acceleration of magnitude \(v^{2} / a\) directed toward the center of the circle.

Solve for all possible values of the real numbers \(x\) and \(y\) in the following equations. $$|x+i y|=y-i x$$

Express the following complex numbers in the \(x+i y\) form. Try to visualize each complex number, using sketches as in the examples if necessary. The first twelve problems you should be able to do in your head (and maybe some of the others- -try it!) Doing a problem quickly in your head saves time over using a computer. Remember that the point in doing problems like this is to gain skill in manipulating complex expressions, so a good study method is to do the problems by hand and use a computer to check your answers. $$\left(\frac{i \sqrt{2}}{1+i}\right)^{12}$$

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