Electronics Engineering  ·  Level 6
Electronics Engineering Mathematics I
Chapter 4: Perform coordinates geometry
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What you will be able to do

By the end of this chapter, you will be able to:

  • Convert polar equations to Cartesian equations correctly by applying the right concepts.
  • Convert Cartesian equations to polar equations accurately using the proper methods.
  • Plot graphs of polar equations correctly to visualize their shapes.
  • Determine normals and tangents using coordinate geometry accurately and confidently.

Mastering these skills will help you solve real-world engineering problems with precision and clarity, making your work in electronics engineering more effective and reliable.

Electronics engineering professionals in Kenya frequently encounter problems involving the analysis and representation of signals, fields, and circuit parameters in various coordinate systems. Polar coordinates provide a convenient way to describe points and curves that naturally depend on angles and distances from a reference point, especially in the design and analysis of antennas, waveguides, and control systems. This chapter develops the foundational concepts of polar coordinates and polar equations, equipping engineers with mathematical tools to model and visualize complex electronic phenomena in two dimensions.

4.1 Polar equations

Polar equations are fundamental in electronics engineering for describing curves and loci where the distance from a reference point varies with angle. This is essential in antenna radiation patterns, impedance loci on Smith charts, and phasor diagrams. The following subtopics introduce the polar coordinate system, define polar equations, and demonstrate how to represent curves with these equations.

4.1.1 Definition of polar coordinates

Polar coordinates specify a point in the plane by its distance from a fixed origin and the angle it makes with a fixed reference direction. This system is especially useful in electronics when dealing with circular symmetry or angular-dependent phenomena.

The polar coordinates \((r, \theta)\) relate to Cartesian coordinates \((x, y)\) by the formulas:

$$ x = r \cos \theta $$

$$ y = r \sin \theta $$

Conversely,

$$ r = \sqrt{x^2 + y^2} $$

$$ \theta = \tan^{-1} (\frac{y}{x}) $$

Worked Examples

Example 1: Find the Cartesian coordinates of a point with polar coordinates \(r = 5\,m\) and \(\theta = 60^\circ\).

Given: \(r = 5\,m\), \(\theta = 60^\circ\)

$$ x = r \cos \theta $$

$$ x = 5 \times \cos 60^\circ $$

$$ x = 5 \times 0.5 = 2.5\,m $$

$$ y = r \sin \theta $$

$$ y = 5 \times \sin 60^\circ $$

$$ y = 5 \times 0.866 = 4.33\,m $$

Answer: (2.5\,m, 4.33\,m)

Example 2: Convert the Cartesian point \((x, y) = (3\,m, 4\,m)\) to polar coordinates.

Given: \(x = 3\,m\), \(y = 4\,m\)

$$ r = \sqrt{x^2 + y^2} $$

$$ r = \sqrt{3^2 + 4^2} = \sqrt{9 + 16} = \sqrt{25} = 5\,m $$

$$ \theta = \tan^{-1} (\frac{y}{x}) $$

$$ \theta = \tan^{-1} (\frac{4}{3}) = 53.13^\circ $$

Answer: \(r = 5\,m, \theta = 53.13^\circ\)

Example 3: Find the polar coordinates of the point \((-3\,m, 3\,m)\).

Given: \(x = -3\,m\), \(y = 3\,m\)

$$ r = \sqrt{(-3)^2 + 3^2} = \sqrt{9 + 9} = \sqrt{18} = 4.24\,m $$

$$ \theta = \tan^{-1} (\frac{3}{-3}) = \tan^{-1}(-1) = -45^\circ $$

Since \(x < 0\) and \(y > 0\), \(\theta\) lies in the second quadrant:

$$ \theta = 180^\circ - 45^\circ = 135^\circ $$

Answer: \(r = 4.24\,m, \theta = 135^\circ\)

Example 4: Determine the Cartesian coordinates of a point with polar coordinates \(r = 10\,cm\), \(\theta = 210^\circ\).

Given: \(r = 10\,cm\), \(\theta = 210^\circ\)

$$ x = 10 \times \cos 210^\circ = 10 \times (-0.866) = -8.66\,cm $$

$$ y = 10 \times \sin 210^\circ = 10 \times (-0.5) = -5\,cm $$

Answer: (-8.66\,cm, -5\,cm)

Example 5: Convert Cartesian point \((x, y) = (-5\,m, -5\,m)\) to polar coordinates.

Given: \(x = -5\,m\), \(y = -5\,m\)

$$ r = \sqrt{(-5)^2 + (-5)^2} = \sqrt{25 + 25} = \sqrt{50} = 7.07\,m $$

$$ \theta = \tan^{-1} (\frac{-5}{-5}) = \tan^{-1}(1) = 45^\circ $$

Since both \(x\) and \(y\) are negative, the point lies in the third quadrant:

$$ \theta = 180^\circ + 45^\circ = 225^\circ $$

Answer: \(r = 7.07\,m, \theta = 225^\circ\)

4.1.2 Definition and examples of polar equations

Polar equations express the radius \(r\) as a function of the angle \(\theta\). These equations describe curves where the distance from the origin changes with direction, useful in electronics for representing wavefronts, antenna patterns, and impedance plots.

A general polar equation is:

$$ r = f(\theta) $$

Common examples include:

  • Circle: \(r = a\)
  • Rose curve: \(r = a \cos n\theta\) or \(r = a \sin n\theta\)
  • Spiral: \(r = a \theta\)
  • Cardioid: \(r = a (1 + \cos \theta)\)

Worked Examples

Example 1: Find the radius when \(\theta = 45^\circ\) for the polar equation \(r = 4\).

Given: \(r = 4\), \(\theta = 45^\circ\)

Since \(r\) is constant:

Answer: \(r = 4\)

Example 2: Calculate \(r\) for \(\theta = 60^\circ\) for the rose curve \(r = 5 \cos 2\theta\).

Given: \(r = 5 \cos 2\theta\), \(\theta = 60^\circ\)

$$ r = 5 \times \cos (2 \times 60^\circ) = 5 \times \cos 120^\circ = 5 \times (-0.5) = -2.5 $$

Since radius cannot be negative in standard form, the point lies in the opposite direction, meaning \(r = 2.5\) at \(\theta = 240^\circ\).

Answer: \(r = -2.5\) (equivalent to \(2.5\) at \(\theta = 240^\circ\))

Example 3: Find the radius for \(\theta = \pi\) radians in the spiral defined by \(r = 3 \theta\).

Given: \(r = 3 \theta\), \(\theta = \pi\)

$$ r = 3 \times \pi = 9.4248 $$

Answer: \(r = 9.4248\) units

Example 4: Determine \(r\) when \(\theta = 90^\circ\) for the cardioid \(r = 6 (1 + \cos \theta)\).

Given: \(r = 6 (1 + \cos \theta)\), \(\theta = 90^\circ\)

$$ r = 6 (1 + \cos 90^\circ) = 6 (1 + 0) = 6 $$

Answer: \(r = 6\)

Example 5: Compute \(r\) for \(\theta = 150^\circ\) in the equation \(r = 8 \sin 3\theta\).

Given: \(r = 8 \sin 3\theta\), \(\theta = 150^\circ\)

$$ r = 8 \times \sin (3 \times 150^\circ) = 8 \times \sin 450^\circ $$

Since \(\sin 450^\circ = \sin (450^\circ - 360^\circ) = \sin 90^\circ = 1\),

$$ r = 8 \times 1 = 8 $$

Answer: \(r = 8\)

4.1.3 Representing curves using polar equations

Representing curves with polar equations allows electronics engineers to visualize complex shapes like antenna lobes and impedance loci. Plotting \(r\) versus \(\theta\) for a range of angles reveals the curve's shape.

The process involves evaluating \(r = f(\theta)\) for values of \(\theta\) typically from \(0^\circ\) to \(360^\circ\), then plotting points \((r, \theta)\) in polar coordinates.

Worked Examples

Example 1: Plot points for the circle \(r = 3\) at \(\theta = 0^\circ, 90^\circ, 180^\circ, 270^\circ\).

Given: \(r = 3\), \(\theta = 0^\circ, 90^\circ, 180^\circ, 270^\circ\)

\(\theta\) \(r\)
3
90° 3
180° 3
270° 3

Convert to Cartesian:

At \(\theta=0^\circ\),

$$ x = 3 \cos 0^\circ = 3 $$

$$ y = 3 \sin 0^\circ = 0 $$

At \(\theta=90^\circ\),

$$ x = 3 \cos 90^\circ = 0 $$

$$ y = 3 \sin 90^\circ = 3 $$

At \(\theta=180^\circ\),

$$ x = 3 \cos 180^\circ = -3 $$

$$ y = 3 \sin 180^\circ = 0 $$

At \(\theta=270^\circ\),

$$ x = 3 \cos 270^\circ = 0 $$

$$ y = 3 \sin 270^\circ = -3 $$

Answer: Points lie on a circle of radius 3 centered at origin.

Example 2: Calculate and plot \(r\) for \(\theta = 0^\circ, 45^\circ, 90^\circ, 135^\circ, 180^\circ\) for \(r = 4 \cos \theta\).

Given: \(r = 4 \cos \theta\)

At \(\theta=0^\circ\),

$$ r = 4 \times \cos 0^\circ = 4 \times 1 = 4 $$

At \(\theta=45^\circ\),

$$ r = 4 \times \cos 45^\circ = 4 \times 0.707 = 2.828 $$

At \(\theta=90^\circ\),

$$ r = 4 \times \cos 90^\circ = 0 $$

At \(\theta=135^\circ\),

$$ r = 4 \times \cos 135^\circ = 4 \times (-0.707) = -2.828 $$

At \(\theta=180^\circ\),

$$ r = 4 \times \cos 180^\circ = 4 \times (-1) = -4 $$

Answer: Values indicate a limaçon curve with points on both sides of the origin.

Example 3: For \(r = 2 + 3 \sin \theta\), find \(r\) at \(\theta = 30^\circ, 90^\circ, 150^\circ, 210^\circ, 270^\circ\).

Given: \(r = 2 + 3 \sin \theta\)

At \(\theta=30^\circ\),

$$ r = 2 + 3 \times \sin 30^\circ = 2 + 3 \times 0.5 = 3.5 $$

At \(\theta=90^\circ\),

$$ r = 2 + 3 \times \sin 90^\circ = 2 + 3 \times 1 = 5 $$

At \(\theta=150^\circ\),

$$ r = 2 + 3 \times \sin 150^\circ = 2 + 3 \times 0.5 = 3.5 $$

At \(\theta=210^\circ\),

$$ r = 2 + 3 \times \sin 210^\circ = 2 + 3 \times (-0.5) = 0.5 $$

At \(\theta=270^\circ\),

$$ r = 2 + 3 \times \sin 270^\circ = 2 + 3 \times (-1) = -1 $$

Answer: The curve extends into negative radius, indicating points in the opposite direction for \(\theta=270^\circ\).

Example 4: Evaluate \(r\) for \(\theta = 0^\circ, 60^\circ, 120^\circ, 180^\circ, 240^\circ, 300^\circ\) in the rose curve \(r = 5 \sin 3\theta\).

Given: \(r = 5 \sin 3\theta\)

At \(\theta=0^\circ\),

$$ r = 5 \times \sin 0^\circ = 0 $$

At \(\theta=60^\circ\),

$$ r = 5 \times \sin 180^\circ = 0 $$

At \(\theta=120^\circ\),

$$ r = 5 \times \sin 360^\circ = 0 $$

At \(\theta=180^\circ\),

$$ r = 5 \times \sin 540^\circ = 5 \times \sin 180^\circ = 0 $$

At \(\theta=240^\circ\),

$$ r = 5 \times \sin 720^\circ = 0 $$

At \(\theta=300^\circ\),

$$ r = 5 \times \sin 900^\circ = 5 \times \sin 180^\circ = 0 $$

Answer: All points at these multiples are zero radius, showing petal tips of the rose curve.

Example 5: For the spiral \(r = 2 \theta\), calculate \(r\) for \(\theta = 0, \frac{\pi}{2}, \pi, \frac{3\pi}{2}, 2\pi\).

Given: \(r = 2 \theta\)

At \(\theta=0\),

$$ r = 2 \times 0 = 0 $$

At \(\theta = \frac{\pi}{2} = 1.5708\),

$$ r = 2 \times 1.5708 = 3.1416 $$

At \(\theta = \pi = 3.1416\),

$$ r = 2 \times 3.1416 = 6.2832 $$

At \(\theta = \frac{3\pi}{2} = 4.7124\),

$$ r = 2 \times 4.7124 = 9.4248 $$

At \(\theta = 2\pi = 6.2832\),

$$ r = 2 \times 6.2832 = 12.5664 $$

Answer: Radius increases linearly with angle, forming an Archimedean spiral.

Practice Questions

  1. Convert the polar coordinates \(r = 7\,m\), \(\theta = 120^\circ\) to Cartesian coordinates. (5 marks)
  2. For the polar equation \(r = 6 \sin 2\theta\), calculate \(r\) at \(\theta = 30^\circ, 60^\circ, 90^\circ\). (6 marks)
  3. Find the polar coordinates of the Cartesian point \((-4\,m, 4\,m)\). (5 marks)
  4. Evaluate \(r\) for \(\theta = 0^\circ, 90^\circ, 180^\circ, 270^\circ\) in the cardioid \(r = 5 (1 + \cos \theta)\). (6 marks)
  5. For the spiral \(r = 4 \theta\), compute \(r\) at \(\theta = \frac{\pi}{4}, \frac{\pi}{2}, \pi\). (6 marks)
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🔒4.2 Cartesian equation

The Cartesian coordinate system is fundamental in electronics engineering for representing spatial relationships, signal paths, and component placements on circuit boards. Kenyan electronics engineers use Cartesian coordinates to model circuits, analyze signal…

🔒4.3 Graphs of polar equations

In electronics engineering, polar coordinates provide an efficient way to represent signals, antenna patterns, and impedance characteristics that depend on angle and magnitude. Understanding how to plot and analyze polar equations enhances the ability to visua…

🔒4.4 Normal and Tangents

In electronics engineering, precise understanding of curves and their properties is essential when analysing signal waveforms, designing antenna arrays, and modelling semiconductor junctions. Tangents and normals to curves provide critical information on insta…

🔒4.5 Loci

Loci are fundamental in electronics engineering mathematics, especially when dealing with signal paths, antenna positioning, and circuit layouts. Understanding loci enables engineers to determine the set of points that satisfy given geometric conditions, criti…

Chapter Summary

This chapter explored the fundamentals of coordinate geometry, beginning with polar coordinates and their equations, highlighting how curves can be represented using polar forms. It then contrasted this with Cartesian coordinates, defining points and equations in the Cartesian plane, and demonstrated the relationship and conversion methods between Cartesian and polar systems. The chapter further detailed the process of plotting polar equations, emphasizing the use of symmetry and periodicity to analyze key features such as intercepts and extrema, with practical applications in engineering. The concepts of tangents and normals to curves were examined next, including methods to find their slopes and equations in both Cartesian and polar contexts. Finally, the chapter introduced the concept of loci, explaining their definitions and importance, especially in relation to circles, and showed how loci are applied in engineering problems such as robotic arm movement and mechanical system optimization. Throughout, the integration of theoretical understanding with practical engineering applications was emphasized to enrich problem-solving skills.

Self-Assessment

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Written Assessment

  1. Find the polar coordinates \((r, \theta)\) of the point with Cartesian coordinates \((3, 3\sqrt{3})\) relevant to positioning an antenna on a communication tower. (3 marks)

  2. Given the polar equation \(r = 4 \cos \theta\), calculate the Cartesian coordinates of the point where \(\theta = \frac{\pi}{3}\) radians, representing the position of a sensor on a rotating arm. (3 marks)

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Chapter Examination Questions

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SECTION A (40 Marks) - Answer ALL Questions

  1. A sensor in a KPLC substation has its position described by the polar coordinates \(r = 5\) m and \(\theta = 60^\circ\). Convert these coordinates to Cartesian form. (4 marks)
  2. Given the polar equation \(r = 3 + 2 \cos \theta\), find the value of \(r\) when \(\theta = 90^\circ\). (4 marks)
🔒18 more in this section.
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Am I competent?

At the start of this chapter we promised you would be able to:

  • Convert polar equations to Cartesian equations correctly by applying the right concepts.
  • Convert Cartesian equations to polar equations accurately using the proper methods.
  • Plot graphs of polar equations correctly to visualize their shapes.
  • Determine normals and tangents using coordinate geometry accurately and confidently.

Tick each one you can genuinely do.

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