12.4 Polar Form of a Complex Number

  • Polar Form r( cos θ +  j sin θ) Expressing Numbers in Polar Form

In this section, we use the fact that a complex number can be represented by a vector to write complex numbers in another form. This form has advantages when multiplying and dividing complex numbers, and we will discuss these operations later in this chapter.

In the complex plane, by drawing a vector from the origin to the point that represents the number x + yj ,  an angle θ in standard position is formed. The point x + yj is r units from the origin. In fact, we can find any point in the complex plane by knowing the angle θ and the value of r. The equations relating x, y, r, and θ are similar to those developed for vectors in Chapter 9. Referring to Fig. 12.9, we see that

Position vector of length r goes to x plus y j at counterclockwise angle theta. Horizontal length is x = r times cosine of theta, and vertical length is y = r times sine of theta.

Fig. 12.9

x = rcos θy = rsin θ
(12.7)
r2 = x2 + y2tanθ = yx
(12.8)

Substituting Eq. (12.7) into the rectangular form x + yj of a complex number, we have x + yj = rcos θ + j(rsin θ) ,  or

x + yj = r(cos θ + jsin θ)
(12.9)

The right side of Eq. (12.9) is called the polar form (sometimes the trigonometric form). The length r is the absolute value, or the modulus, and θ is the argument of the complex number. Equations (12.7)–(12.9) define the polar form of a complex number.

EXAMPLE 1 Representing a number in polar form

Represent the complex number 3 + 4j graphically and give its polar form.

From the rectangular form 3 + 4j ,  we see that x = 3 and y = 4. Using Eqs. (12.8), we have

r = 32 + 42 = 5θ = tan − 143 = 53.1 ° 

Thus, the polar form is 5(cos 53.1 °  + jsin 53.1 ° ) .  See Fig. 12.10.

A position vector of length r = 5 goes to 3 plus 4 j at (3, 4) at counterclockwise angle 53.1 degrees.

Fig. 12.10

In Example 1, in expressing the polar form as 5(cos 53.1 °  + jsin 53.1 ° ) ,  we rounded the angle to the nearest 0.1 ° , as it is not possible to express the result exactly in degrees. In dealing with nonexact numbers, we will express angle to the nearest 0.1 ° . Other results that cannot be written exactly will be expressed to three significant digits, unless a different accuracy is given in the problem. Of course, in applied situations, most numbers are approximate, as they are derived through measurement.

Another convenient and widely used notation for the polar form is r ∠ θ_  .  We must remember in using this form that it represents a complex number and is simply a shorthand way of writing r(cos θ + jsin θ) .  Therefore,

r ∠ θ_  = r(cos θ + jsin θ)
(12.10)

EXAMPLE 2 Polar form r ∠ θ_ 

  1. 3(cos 40 °  + jsin 40 ° ) = 3 ∠ 40 ° _ 

  2. 6.26(cos 217.3 °  + jsin 217.3 ° ) = 6.26 ∠ 217.3 ° _ 

  3. 5 ∠ 120 ° _  = 5(cos 120 °  + jsin 120 ° )

  4. 14.5 ∠ 306.2 ° _  = 14.5(cos 306.2 °  + jsin 306.2 ° )

EXAMPLE 3 Rectangular form to polar form

Represent the complex number  − 1.04 − 1.56j graphically and give its polar form.

The graphical representation is shown in Fig. 12.11. From Eqs. (12.8), we have

A position vector goes to (negative 1.04, negative 1.56) at counterclockwise angle 236.3 degrees.

Fig. 12.11

r = ( − 1.04)2 + ( − 1.56)2 = 1.87θref = tan − 11.561.04 = 56.3 ° θ = 180 °  + 56.3 °  = 236.3 ° 

Because both the real and imaginary parts are negative, θ is a third-quadrant angle. Therefore, we found the reference angle before finding θ .  This means the polar forms are

1.87(cos 236.3 °  + jsin 236.3 ° ) = 1.87 ∠ 236.3 ° _ 

EXAMPLE 4 Polar form to rectangular form—impedance

The impedance Z (in  Ω ) in an alternating-current circuit is given by Z = 3560 ∠  − 32.4 ° _  .  Express this in rectangular form.

From the polar form, we have r = 3560 Ω  and θ =  − 32.4 °  (it is common to use negative angles in this type of application). This means that we can also write

Z = 3560[ (cos ( − 32.4 ° ) + jsin( − 32.4 ° )] 

See Fig. 12.12. This means that

A position vector goes to Z in quadrant 4 at clockwise angle negative 32.4 degrees.

Fig. 12.12

x = 3560 cos( − 32.4 ° ) = 3010y = 3560 sin( − 32.4 ° ) =  − 1910

Therefore, the rectangular form is Z = 3010 − 1910j Ω  . 

Complex numbers can be converted between rectangular and polar forms on most calculators. Figure 12.13 shows the calculator conversions for Examples 3 and 4. Note that for Example 3, the calculator returns an angle of  − 123.7 °  .  This is coterminal to 236.3 ° , the angle we found.

A calculator screen.

Fig. 12.13

EXAMPLE 5 Polar form—real and imaginary numbers

Represent the numbers 5,  − 5 ,  7j, and  − 7j in polar form. See Fig. 12.14.

Four numbers are represented on a plane. Five is at (5, 0), 7 j is (0, 7), negative 5 is (negative 5, 0), and negative 7 j is (0, negative 7).

Fig. 12.14

Real numbers lie on the real axis in the complex plane, while imaginary numbers lie on the imaginary axis. Therefore, the polar form angle of any real or imaginary number is a multiple of 90 °  as shown below:

5 = 5(cos 0 °  + jsin 0 ° ) = 5 ∠ 0 ° _ 5 units from the origin at an angle of 0°  − 5 = 5(cos 180 °  + jsin 180 ° ) = 5 ∠ 180 ° _ 5 units from the origin at an angle of 180° 7j = 7(cos 90 °  + jsin 90 ° ) = 7 ∠ 90 ° _ 7 units from the origin at an angle of 90°  − 7j = 7(cos 270 °  + jsin 270 ° ) = 7 ∠ 270 ° _ 7 units from the origin at an angle of 270° 

EXERCISES 12.4

In Exercises 1 and 2, change the sign of the real part of the complex number in the indicated example of this section and then perform the indicated operations for the resulting complex number.

In Exercises 318, represent each complex number graphically and give the polar form of each.

  1. 8 + 6j

  2.  − 8 − 15j

  3. 30 − 40j

  4. 12j − 5

  5. 3.00j − 2.00

  6. 7.00 − 5.00j

  7.  − 0.55 − 0.24j

  8. 460 − 460j

  9. 1 + j3

  10. 2 − j2

  11. 3.514 − 7.256j

  12. 95.27j + 62.31

  13.  − 3

  14. 60

  15. 9j

  16.  − 2j

In Exercises 1936, represent each complex number graphically and give the rectangular form of each.

  1. 5.00(cos 54.0 °  + jsin 54.0 ° )

  2. 6(cos 180 °  + jsin 180 ° )

  3. 160(cos 150.0 °  + jsin 150.0 ° )

  4. 2.50(cos 315.0 °  + jsin 315.0 ° )

  5. 3.00(cos 232.0 °  + jsin 232.0 ° )

  6. 220.8(cos 155.13 °  + jsin 155.13 ° )

  7. 0.08(cos 360 °  + jsin 360 ° )

  8. 15(cos 0 °  + jsin 0 ° )

  9. 120(cos 270 °  + jsin 270 ° )

  10. cos 600.0 °  + jsin 600.0 ° 

  11. 4.75 ∠ 172.8 ° _ 

  12. 1.50 ∠ 897.7 ° _ 

  13. 0.9326 ∠ 229.54 ° _ 

  14. 277.8 ∠  − 342.63 ° _ 

  15. 7.32 ∠  − 270 ° _ 

  16. 18.3 ∠ 540.0 ° _ 

  17. 86.42 ∠ 94.62 ° _ 

  18. 4629 ∠ 182.44 ° _ 

In Exercises 3744, solve the given problems.

  1. What is the argument for any negative real number?

  2. For x + yj ,  what is the argument if x = y < 0 ? 

  3. Show that the conjugate of r ∠ θ_  is r ∠  − θ_  . 

  4. The impedance in a certain circuit is Z = 8.5 ∠  − 36 ° _  Ω  . Write this in rectangular form.

  5. The voltage of a certain generator is represented by 2.84 − 1.06j kV .  Write this voltage in polar form.

  6. Find the magnitude and direction of a force on a bolt that is represented by 40.5 + 24.5j newtons.

  7. The electric field intensity of a light wave can be described by 12.4 ∠ 78.3 ° _  V / m .  Write this in rectangular form.

  8. The current in a certain microprocessor circuit is represented by 3.75 ∠ 15.0 ° _  μA .  Write this in rectangular form.

Answers to Practice Exercises

  1. 17(cos 331.9 °  + jsin 331.9 ° )

  2.  − 1.25 + 2.17j

  3. 10 ∠ 270 ° _ 

..................Content has been hidden....................

You can't read the all page of ebook, please click here login for view all page.
Reset
3.15.229.113