A Real Exploration of Euler's Imaginary I: Isomorphism And
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												Section 2.6 Cylindrical and Spherical Coordinates
Section 2.6 Cylindrical and Spherical Coordinates A) Review on the Polar Coordinates The polar coordinate system consists of the origin O,the rotating ray or half line from O with unit tick. A point P in the plane can be uniquely described by its distance to the origin r = dist (P, O) and the angle µ, 0 µ < 2¼ : · Y P(x,y) r θ O X We call (r, µ) the polar coordinate of P. Suppose that P has Cartesian (stan- dard rectangular) coordinate (x, y) .Then the relation between two coordinate systems is displayed through the following conversion formula: x = r cos µ Polar Coord. to Cartesian Coord.: y = r sin µ ½ r = x2 + y2 Cartesian Coord. to Polar Coord.: y tan µ = ( p x 0 µ < ¼ if y > 0, 2¼ µ < ¼ if y 0. · · · Note that function tan µ has period ¼, and the principal value for inverse tangent function is ¼ y ¼ < arctan < . ¡ 2 x 2 1 So the angle should be determined by y arctan , if x > 0 xy 8 arctan + ¼, if x < 0 µ = > ¼ x > > , if x = 0, y > 0 < 2 ¼ , if x = 0, y < 0 > ¡ 2 > > Example 6.1. Fin:>d (a) Cartesian Coord. of P whose Polar Coord. is ¼ 2, , and (b) Polar Coord. of Q whose Cartesian Coord. is ( 1, 1) . 3 ¡ ¡ ³ So´l. (a) ¼ x = 2 cos = 1, 3 ¼ y = 2 sin = p3. 3 (b) r = p1 + 1 = p2 1 ¼ ¼ 5¼ tan µ = ¡ = 1 = µ = or µ = + ¼ = . 1 ) 4 4 4 ¡ 5¼ Since ( 1, 1) is in the third quadrant, we choose µ = so ¡ ¡ 4 5¼ p2, is Polar Coord. - 
												
												About the Phasor Pathways in Analogical Amplitude Modulations
About the Phasor Pathways in Analogical Amplitude Modulations H.M. de Oliveira1, F.D. Nunes1 ABSTRACT Phasor diagrams have long been used in Physics and Engineering. In telecommunications, this is particularly useful to clarify how the modulations work. This paper addresses rotating phasor pathways derived from different standard Amplitude Modulation Systems (e.g. A3E, H3E, J3E, C3F). A cornucopia of algebraic curves is then derived assuming a single tone or a double tone modulation signal. The ratio of the frequency of the tone modulator (fm) and carrier frequency (fc) is considered in two distinct cases, namely: fm/fc<1 and fm/fc 1. The geometric figures are some sort of Lissajours figures. Different shapes appear looking like epicycloids (including cardioids), rhodonea curves, Lemniscates, folium of Descartes or Lamé curves. The role played by the modulation index is elucidated in each case. Keyterms: Phasor diagram, AM, VSB, Circular harmonics, algebraic curves, geometric figures. 1. Introduction Classical analogical modulations are a nearly exhausted subject, a century after its introduction. The first approach to the subject typically relies on the case of transmission of a single tone (for the sake of simplicity) and establishes the corresponding phasor diagram. This furnishes a straightforward interpretation, which is quite valuable, especially with regard to illustrating the effects of the modulation index, overmodulation effects, and afterward, distinctions between AM and NBFM. Often this presentation is rather naïf. Nice applets do exist to help the understanding of the phasor diagram [1- 4]. However ... Without further target, unpretentiously, we start a deeper investigating the dynamic phasor diagram with the aim of building applets or animations that illustrates the temporal variation of the magnitude of the amplitude modulated phasor. - 
												
												Correspondence Between Phasor Transforms and Frequency Response Function in Rlc Circuits
CORRESPONDENCE BETWEEN PHASOR TRANSFORMS AND FREQUENCY RESPONSE FUNCTION IN RLC CIRCUITS Hassan Mohamed Abdelalim Abdalla Polytechnic Department of Engineering and Architecture, University of Studies of Udine, 33100 Udine, Italy. E-mail: [email protected] Abstract: The analysis of RLC circuits is usually made by considering phasor transforms of sinusoidal signals (characterized by constant amplitude, period and phase) that allow the calculation of the AC steady state of RLC circuits by solving simple algebraic equations. In this paper I try to show that phasor representation of RLC circuits is analogue to consider the frequency response function (commonly designated by FRF) of the total impedance of the circuit. In this way I derive accurate expressions for the resonance and anti-resonance frequencies and their corresponding values of impedances of the parallel and series RLC circuits respectively, notwithstanding the presence of damping effects. Keywords: Laplace transforms, phasors, Frequency response function, RLC circuits. 1. Introduction and mathematical background RLC circuits have many applications as oscillator circuits described by a second-order differential equation. The three circuit elements, resistor R, inductor L and capacitor C can be combined in different manners. All three elements in series or in parallel are the simplest and most straightforward to analyze. RLC circuits are analyzed mathematically in the phasor domain instead of solving differential equations in the time domain. Generally, a time-dependent sinusoidal function is expressed in the following way è [1]: () (1.1) where is the amplitude, is the angular frequency and is the initial phase of . () = sin ( + ) The medium value of is given by: () () (1.2) 1 2 = |()| = where is the period of the sinusoidal function . - 
												
												Designing Patterns with Polar Equations Using Maple
Designing Patterns with Polar Equations using Maple Somasundaram Velummylum Claflin University Department of Mathematics and Computer Science 400 Magnolia St Orangeburg, South Carolina 29115 U.S.A [email protected] The Cartesian coordinates and polar coordinates can be used to identify a point in two dimensions. The polar coordinate system has a fixed point O called the origin or pole and a directed half –line called the polar axis with end point O. A point P on the plane can be described by the polar coordinates ( r, θ ), where r is the radial distance from the origin and θ is the angle made by OP with the polar axis. Several important types of graphs have equations that are simpler in polar form than in rectangular form. For example, the polar equation of a circle having radius a and centered at the origin is simply r = a. In other words , polar coordinate system is useful in describing two dimensional regions that may be difficult to describe using Cartesian coordinates. For example, graphing the circle x 2 + y 2 = a 2 in Cartesian coordinates requires two functions, one for the upper half and one for the lower half. In polar coordinate system, the same circle has the very simple representation r = a. Maple can be used to create patterns in two dimensions using polar coordinate system. When we try to analyze two dimensional patterns mathematically it will be helpful if we can draw a set of patterns in different colors using the help of technology. To investigate and compare some patterns we will go through some examples of cardioids and rose curves that are drawn using Maple. - 
												
												Complex Numbers and Phasor Technique
RaoApp-Av3.qxd 12/18/03 5:44 PM Page 779 APPENDIX A Complex Numbers and Phasor Technique In this appendix, we discuss a mathematical technique known as the phasor technique, pertinent to operations involving sinusoidally time-varying quanti- ties.The technique simplifies the solution of a differential equation in which the steady-state response for a sinusoidally time-varying excitation is to be deter- mined, by reducing the differential equation to an algebraic equation involving phasors. A phasor is a complex number or a complex variable. We first review complex numbers and associated operations. A complex number has two parts: a real part and an imaginary part. Imag- inary numbers are square roots of negative real numbers. To introduce the con- cept of an imaginary number, we define 2-1 = j (A.1a) or ;j 2 =-1 (A.1b) 1 2 Thus, j5 is the positive square root of -25, -j10 is the negative square root of -100, and so on.A complex number is written in the form a + jb, where a is the real part and b is the imaginary part. Examples are 3 + j4 -4 + j1 -2 - j2 2 - j3 A complex number is represented graphically in a complex plane by using Rectangular two orthogonal axes, corresponding to the real and imaginary parts, as shown in form Fig.A.1, in which are plotted the numbers just listed. Since the set of orthogonal axes resembles the rectangular coordinate axes, the representation a + jb is 1 2 known as the rectangular form. 779 RaoApp-Av3.qxd 12/18/03 5:44 PM Page 780 780 Appendix A Complex Numbers and Phasor Technique Imaginary (3 ϩ j4) 4 (Ϫ4 ϩ j1) 1 Ϫ2 2 Ϫ 4 0 3 Real Ϫ2 (Ϫ2 Ϫj2) Ϫ3 Ϫ FIGURE A.1 (2 j3) Graphical representation of complex numbers in rectangular form. - 
												
												Polar Coordinates and Calculus.Wxp
Polar Coordinates and Calculus Recall that in the Polar coordinate system the coordinates ) represent <ß the directed distance from the pole to the point and the directed angle, counterclockwise from the polar axis to the segment from the pole to the point. A polar function would be of the form: ) . < œ 0 To find the slope of the tangent line of a polar graph we will parameterize the equation. ) ( Assume is a differentiable function of ) ) <œ0 0 ¾Bœ<cos))) œ0 cos and Cœ< sin ))) œ0 sin . .C .C .) Recall also that œ .B .B .) 1Þ Find the derivative of < œ # sin ) Remember that horizontal tangent lines occur when and that vertical tangent lines occur when page 1 2 Find the HTL and VTL for cos ) and sketch the graph. Þ < œ # " page 2 Recall our formula for the derivative of a function in polar coordinates. Since Bœ<cos))) œ0 cos and Cœ< sin ))) œ0 sin , we can conclude .C .C .) that œ.B œ .B .) Solutions obtained by setting < œ ! gives equations of tangent lines through the pole. 3Þ Find the equations of the tangent line(s) through the pole if <œ#sin #Þ) page 3 To find the arc length of a polar curve, you have two options. 1) You can use the parametrization of the polar curve: cos))) cos and sin ))) sin Bœ< œ0 Cœ< œ0 then use the arc length formula for parametric curves: " w # w # 'α ÈÐBÐ) ÑÑ ÐCÐ ) ÑÑ . ) or, 2) You can use an alternative formula for arc length in polar form: " <# Ð.< Ñ # . - 
												
												Lesson 1: Representation of Ac Voltages and Currents1
1/22/2016 Lesson 1: Phasors and Complex Arithmetic ET 332b Ac Motors, Generators and Power Systems lesson1_et332b.pptx 1 Learning Objectives After this presentation you will be able to: Write time equations that represent sinusoidal voltages and currents found in power systems. Explain the difference between peak and RMS electrical quantities. Write phasor representations of sinusoidal time equations. Perform calculations using both polar and rectangular forms of complex numbers. lesson1_et332b.pptx 2 1 1/22/2016 Ac Analysis Techniques Time function representation of ac signals Time functions give representation of sign instantaneous values v(t) Vmax sin(t v ) Voltage drops e(t) Emax sin(t e ) Source voltages Currents i(t) Imax sin(t i ) Where Vmax = maximum ( peak) value of voltage Emax = maximum (peak) value of source voltage Imax = maximum (peak) value of current v, e, i = phase shift of voltage or current = frequency in rad/sec Note: =2pf lesson1_et332b.pptx 3 Ac Signal Representations Ac power system calculations use effective values of time waveforms (RMS values) Therefore: V E I V max E max I max RMS 2 RMS 2 RMS 2 1 Where 0.707 2 So RMS quantities can be expressed as: VRMS 0.707Vmax ERMS 0.707Emax IRMS 0.707Imax lesson1_et332b.pptx 4 2 1/22/2016 Ac Signal Representations Ac power systems calculations use phasors to represent time functions Phasor use complex numbers to represent the important information from the time functions (magnitude and phase angle) in vector form. Phasor Notation I I V VRMS RMS or or I I V VRMS RMS Where: VRMS, IRMS = RMS magnitude of voltages and currents = phase shift in degrees for voltages and currents lesson1_et332b.pptx 5 Ac Signal Representations Time to phasor conversion examples, Note all signal must be the same frequency Time function-voltage Find RMS magnitude v(t) 170sin(377t 30 ) VRMS 0.707170 120.2 V Phasor V 120.230 V Time function-current Find RMS magnitude i(t) 25sin(377t 20 ) IRMS 0.70725 17.7 A Phasor I 17.7 20 A Phase shift can be given in either radians or degrees. - 
												
												Classical Mechanics Lecture Notes POLAR COORDINATES
PHYS 419: Classical Mechanics Lecture Notes POLAR COORDINATES A vector in two dimensions can be written in Cartesian coordinates as r = xx^ + yy^ (1) where x^ and y^ are unit vectors in the direction of Cartesian axes and x and y are the components of the vector, see also the ¯gure. It is often convenient to use coordinate systems other than the Cartesian system, in particular we will often use polar coordinates. These coordinates are speci¯ed by r = jrj and the angle Á between r and x^, see the ¯gure. The relations between the polar and Cartesian coordinates are very simple: x = r cos Á y = r sin Á and p y r = x2 + y2 Á = arctan : x The unit vectors of polar coordinate system are denoted by r^ and Á^. The former one is de¯ned accordingly as r r^ = (2) r Since r = r cos Á x^ + r sin Á y^; r^ = cos Á x^ + sin Á y^: The simplest way to de¯ne Á^ is to require it to be orthogonal to r^, i.e., to have r^ ¢ Á^ = 0. This gives the condition cos ÁÁx + sin ÁÁy = 0: 1 The simplest solution is Áx = ¡ sin Á and Áy = cos Á or a solution with signs reversed. This gives Á^ = ¡ sin Á x^ + cos Á y^: This vector has unit length Á^ ¢ Á^ = sin2 Á + cos2 Á = 1: The unit vectors are marked on the ¯gure. With our choice of sign, Á^ points in the direc- tion of increasing angle Á. Notice that r^ and Á^ are drawn from the position of the point considered. - 
												
												Waveguide Propagation
NTNU Institutt for elektronikk og telekommunikasjon Januar 2006 Waveguide propagation Helge Engan Contents 1 Introduction ........................................................................................................................ 2 2 Propagation in waveguides, general relations .................................................................... 2 2.1 TEM waves ................................................................................................................ 7 2.2 TE waves .................................................................................................................... 9 2.3 TM waves ................................................................................................................. 14 3 TE modes in metallic waveguides ................................................................................... 14 3.1 TE modes in a parallel-plate waveguide .................................................................. 14 3.1.1 Mathematical analysis ...................................................................................... 15 3.1.2 Physical interpretation ..................................................................................... 17 3.1.3 Velocities ......................................................................................................... 19 3.1.4 Fields ................................................................................................................ 21 3.2 TE modes in rectangular waveguides ..................................................................... - 
												
												Chapter 16 Waves I
Chapter 16 Waves I In this chapter we will start the discussion on wave phenomena. We will study the following topics: Types of waves Amplitude, phase, frequency, period, propagation speed of a wave Mechanical waves propagating along a stretched string Wave equation Principle of superposition of waves Wave interference Standing waves, resonance (16 – 1) A wave is defined as a disturbance that is self-sustained and propagates in space with a constant speed Waves can be classified in the following three categories: 1. Mechanical waves. These involve motions that are governed by Newton’s laws and can exist only within a material medium such as air, water, rock, etc. Common examples are: sound waves, seismic waves, etc. 2. Electromagnetic waves. These waves involve propagating disturbances in the electric and magnetic field governed by Maxwell’s equations. They do not require a material medium in which to propagate but they travel through vacuum. Common examples are: radio waves of all types, visible, infra-red, and ultra- violet light, x-rays, gamma rays. All electromagnetic waves propagate in vacuum with the same speed c = 300,000 km/s 3. Matter waves. All microscopic particles such as electrons, protons, neutrons, atoms etc have a wave associated with them governed by Schroedinger’s equation. (16 – 2) Transverse and Longitudinal waves (16 – 3) Waves can be divided into the following two categories depending on the orientation of the disturbance with r respect to the wave propagation velocity v. If the disturbance associated with a particular wave is perpendicular to the wave propagation velocity, this wave is called "transverse ". - 
												
												Section 6.7 Polar Coordinates 113
Section 6.7 Polar Coordinates 113 Course Number Section 6.7 Polar Coordinates Instructor Objective: In this lesson you learned how to plot points in the polar coordinate system and write equations in polar form. Date I. Introduction (Pages 476-477) What you should learn How to plot points in the To form the polar coordinate system in the plane, fix a point O, polar coordinate system called the pole or origin , and construct from O an initial ray called the polar axis . Then each point P in the plane can be assigned polar coordinates as follows: 1) r = directed distance from O to P 2) q = directed angle, counterclockwise from polar axis to the segment from O to P In the polar coordinate system, points do not have a unique representation. For instance, the point (r, q) can be represented as (r, q ± 2np) or (- r, q ± (2n + 1)p) , where n is any integer. Moreover, the pole is represented by (0, q), where q is any angle . Example 1: Plot the point (r, q) = (- 2, 11p/4) on the polar py/2 coordinate system. p x0 3p/2 Example 2: Find another polar representation of the point (4, p/6). Answers will vary. One such point is (- 4, 7p/6). Larson/Hostetler Trigonometry, Sixth Edition Student Success Organizer IAE Copyright © Houghton Mifflin Company. All rights reserved. 114 Chapter 6 Topics in Analytic Geometry II. Coordinate Conversion (Pages 477-478) What you should learn How to convert points The polar coordinates (r, q) are related to the rectangular from rectangular to polar coordinates (x, y) as follows . - 
												
												1.7 Cylindrical and Spherical Coordinates
56 CHAPTER 1. VECTORS AND THE GEOMETRY OF SPACE 1.7 Cylindrical and Spherical Coordinates 1.7.1 Review: Polar Coordinates The polar coordinate system is a two-dimensional coordinate system in which the position of each point on the plane is determined by an angle and a distance. The distance is usually denoted r and the angle is usually denoted . Thus, in this coordinate system, the position of a point will be given by the ordered pair (r, ). These are called the polar coordinates These two quantities r and , are determined as follows. First, we need some reference points. You may recall that in the Cartesian coordinate system, everything was measured with respect to the coordinate axes. In the polar coordinate system, everything is measured with respect a fixed point called the pole and an axis called the polar axis. The is the equivalent of the origin in the Cartesian coordinate system. The polar axis corresponds to the positive x-axis. Given a point P in the plane, we draw a line from the pole to P . The distance from the pole to P is r, the angle, measured counterclockwise, by which the polar axis has to be rotated in order to go through P is . The polar coordinates of P are then (r, ). Figure 1.7.1 shows two points and their representation in the polar coordinate system. Remark 79 Let us make several remarks. 1. Recall that a positive value of means that we are moving counterclock- wise. But can also be negative. A negative value of means that the polar axis is rotated clockwise to intersect with P .