Showing posts with label polar representation. Show all posts
Showing posts with label polar representation. Show all posts

Saturday, June 4, 2022

Chapter 5.7 - Miscellaneous Examples

In the previous section, we completed a discussion on quadratic equations. We saw some miscellaneous examples also. In this section, we will see a few more miscellaneous examples.

Solved example 5.13
If $x+yi~=~\frac{a+bi}{a-bi}$, prove that $x^2+y^2=1$
Solution:
1. We will change the right side into the general form:
$\begin{array}{ll}
\frac{a+bi}{a-bi}&{}={}&\frac{a+bi}{a-bi} × \frac{a+bi}{a+bi}& {} &{} \\
\phantom{\frac{a+bi}{a-bi}}&{}={}&\frac{a^2+2abi-b^2}{a^2+b^2}&{} \\
\phantom{\frac{a+bi}{a-bi}}&{}={}&\frac{a^2-b^2}{a^2+b^2}~+~\frac{2abi}{a^2+b^2}&{} \\
\phantom{\frac{a+bi}{a-bi}}&{}={}&\frac{a^2-b^2}{a^2+b^2}~+~\left(\frac{2ab}{a^2+b^2}\right)i&{} \\
\end{array}$
2. So the given expression becomes: $x+yi~=~\frac{a^2-b^2}{a^2+b^2}~+~\left(\frac{2ab}{a^2+b^2}\right)i$
3. Equating the corresponding real and imaginary parts, we get:
$x~=~\frac{a^2-b^2}{a^2+b^2}$
$y~=~\frac{2ab}{a^2+b^2}$
4. Now we can find $x^2+y^2$:
$\begin{array}{ll}
x^2+y^2&{}={}&\left(\frac{a^2-b^2}{a^2+b^2} \right)^2~+~\left(\frac{2ab}{a^2+b^2} \right)^2& {} &{} \\
\phantom{x^2+y^2}&{}={}&\frac{(a^2-b^2)^2~+~(2ab)^2}{(a^2+b^2)^2}&{} \\
\phantom{x^2+y^2}&{}={}&\frac{a^4-2a^2 b^2+b^4~+~4a^2 b^2}{(a^2+b^2)^2}&{} \\
\phantom{x^2+y^2}&{}={}&\frac{a^4+2a^2 b^2+b^4}{(a^2+b^2)^2}&{} \\
\phantom{x^2+y^2}&{}={}&\frac{(a^2+b^2)^2}{(a^2+b^2)^2}&{} \\
\phantom{x^2+y^2}&{}={}&1&{} \\
\end{array}$

Solved example 5.14
Find real šœ½ such that $\frac{3+2i\sin \theta}{1-2i\sin \theta}$ is purely real
Solution:
1. We will change the given expression into the general form:
$\begin{array}{ll}
\frac{3+2i\sin \theta}{1-2i\sin \theta}&{}={}&\frac{3+2i\sin \theta}{1-2i\sin \theta}~ × ~\frac{1+2i\sin \theta}{1+2i\sin \theta}& {} &{} \\
\phantom{\frac{3+2i\sin \theta}{1-2i\sin \theta}}&{}={}&\frac{3+6i \sin \theta +2i \sin \theta - 4 \sin^2 \theta}{1+4 \sin^2 \theta}&{} \\
\phantom{\frac{3+2i\sin \theta}{1-2i\sin \theta}}&{}={}&\frac{3+8i \sin \theta - 4 \sin^2 \theta}{1+4 \sin^2 \theta}&{} \\
\phantom{\frac{3+2i\sin \theta}{1-2i\sin \theta}}&{}={}&\frac{3- 4 \sin^2 \theta}{1+4 \sin^2 \theta}~+~\frac{8i \sin \theta}{1+4 \sin^2 \theta}&{} \\
\phantom{\frac{3+2i\sin \theta}{1-2i\sin \theta}}&{}={}&\frac{3- 4 \sin^2 \theta}{1+4 \sin^2 \theta}~+~\left(\frac{8 \sin \theta}{1+4 \sin^2 \theta}\right)i&{} \\
\end{array}$
2. So the given complex number is: $\frac{3- 4 \sin^2 \theta}{1+4 \sin^2 \theta}~+~\left(\frac{8 \sin \theta}{1+4 \sin^2 \theta}\right)i$
3. If this complex number is to be purely real, the imaginary part must be zero.
• That is., $\frac{8 \sin \theta}{1+4 \sin^2 \theta}$ must be zero.
• Denominator cannot be zero because, division by zero will give a number which does not exist.
• So we can write:
If the given complex number is to be purely real, $8 \sin \theta$ must be zero.
   ♦ That is., $8 \sin \theta~=~0$
   ♦ This is true only when sin šœ½ = 0
4. sin šœ½ = 0 is a trigonometrical equation.
• We know that, this equation is true whenever šœ½ is a multiple of šž¹
5. So we can write:
The given complex number will be purely real when šœ½ = nšž¹
   ♦ Where n is member of the set of integers Z.

Solved example 5.15
Convert the complex number $\frac{i-1}{\cos \frac{\pi}{3}+i \sin \frac{\pi}{3}}$ in the polar form.
Solution:
1. We will change the given expression into the general form:
$\begin{array}{ll}
\frac{i-1}{\cos \frac{\pi}{3}+i \sin \frac{\pi}{3}}&{}={}&\frac{i-1}{\cos \frac{\pi}{3}+i \sin \frac{\pi}{3}}~ × ~\frac{\cos \frac{\pi}{3}-i \sin \frac{\pi}{3}}{\cos \frac{\pi}{3}-i \sin \frac{\pi}{3}}& {} &{} \\
\phantom{\frac{i-1}{\cos \frac{\pi}{3}+i \sin \frac{\pi}{3}}}&{}={}&\frac{(i-1)(\cos \frac{\pi}{3}-i \sin \frac{\pi}{3})}{\cos^2 \frac{\pi}{3}+ \sin^2 \frac{\pi}{3}}&{} \\
\phantom{\frac{i-1}{\cos \frac{\pi}{3}+i \sin \frac{\pi}{3}}}&{}={}&\frac{(i-1)( \frac{1}{2}- \frac{\sqrt{3}}{2}i)}{1}&{} \\
\phantom{\frac{i-1}{\cos \frac{\pi}{3}+ \frac{\pi}{3}}}&{}={}&(i-1)( \frac{1}{2}- \frac{\sqrt{3}}{2}i)&{} \\
\phantom{\frac{i-1}{\cos \frac{\pi}{3}+ \frac{\pi}{3}}}&{}={}&{\frac{1}{2}}i+\frac{\sqrt{3}}{2}-\frac{1}{2}+{\frac{\sqrt{3}}{2}}i&{} \\
\phantom{\frac{i-1}{\cos \frac{\pi}{3}+ \frac{\pi}{3}}}&{}={}&\frac{\sqrt{3}-1}{2}~+~\left(\frac{\sqrt{3}+1}{2} \right)i&{} \\
\end{array}$
2. Now the complex number is in the form x+yi
We have to convert it into the form r[cos šœ½+ i sin šœ½]
3. We know that the modulus r is given by: $r=\sqrt{x^2+y^2}$
So in our present case,
$\begin{array}{ll}
r&{}={}&\sqrt{x^2+y^2}& {} &{} \\
\phantom{r}&{}={}&\sqrt{\left(\frac{\sqrt{3}-1}{2} \right)^2+\left(\frac{\sqrt{3}+1}{2} \right)^2}&{} \\
\phantom{r}&{}={}&\sqrt{\frac{(\sqrt{3}-1)^2+(\sqrt{3}+1)^2}{4}}&{} \\
\phantom{r}&{}={}&\sqrt{\frac{3-2\sqrt{3}+1~+~3+2\sqrt{3}+1}{4}}&{} \\
\phantom{r}&{}={}&\sqrt{\frac{8}{4}}&{} \\
\phantom{r}&{}={}&\sqrt{2}&{} \\
\end{array}$
4. Since x+yi and r[cos šœ½+ i sin šœ½] represent the same complex number, we can equate the corresponding real and imaginary parts. We get:
    ♦ x = r cos šœ½
    ♦ y = r sin šœ½
5. From this we get:
(i) $\frac{\sqrt{3}-1}{2}=\sqrt{2} \cos \theta$
(ii) $\frac{\sqrt{3}+1}{2}=\sqrt{2} \sin \theta$
• sin šœ½ is +ve. cos šœ½ is also +ve. So it is in the first quadrant.
6. Taking ratios, (ii) to (i), we get:
$\frac{\sqrt{2} \sin \theta}{\sqrt{2} \cos \theta}=\frac{\frac{\sqrt{3}+1}{2}}{\frac{\sqrt{3}-1}{2}}$
$\Rightarrow \tan \theta = \frac{\sqrt{3}+1}{\sqrt{3}-1}$
• This is a trigonometrical equation. We learned to solve them in chapter 3. (Details here)
7. We have, $\tan \frac{5\pi}{12}~=~ \tan 75^o~=~\frac{\sqrt{3}+1}{\sqrt{3}-1}$
Proof:
$\begin{array}{ll}
\tan \frac{5 \pi}{12}&{}={}&\tan \left(\frac{5 \pi}{12}~\times ~\frac{2}{2}\right)~=~\tan \frac{10 \pi}{24}& {} &{} \\
\phantom{\tan \frac{5 \pi}{12}}&{}={}&\tan \left(\frac{\pi}{4}+\frac{\pi}{6} \right)&{} \\
\phantom{\tan \frac{5 \pi}{12}}&{}={}&\frac{\tan \frac{\pi}{4}~+~\tan \frac{\pi}{6}}{1-\tan \frac{\pi}{4}\tan \frac{\pi}{6}}&{} \\
\phantom{\tan \frac{5 \pi}{12}}&{}&\color {green}{\because \tan(p+q)=\frac{\tan p + \tan q}{1-\tan p \tan q}}&{} \\
\phantom{\tan \frac{5 \pi}{12}}&{}={}&\frac{1~+~\frac{1}{\sqrt3}}{1-1 \times \frac{1}{\sqrt3}}&{} \\
\phantom{\tan \frac{5 \pi}{12}}&{}={}&\frac{\sqrt3+1}{\sqrt3-1}&{} \\
\end{array}$
• From this we get: $\theta = \frac{5\pi}{12}$
• This šœ½ is in the first quadrant. So there is no need to find the other value of šœ½.
8. Thus we get the values of r and šœ½:
   ♦ From (3), we get: $r= \sqrt{2}$
   ♦ From (7),we get: $\theta = \frac{5\pi}{12}$
• So the polar form is: $\sqrt{2}\left[\cos \frac{5\pi}{12} + i \sin \frac{5\pi}{12} \right]$
• The red dot in fig.5.9 below represents the complex number:

Fig.5.9

Solved example 5.16
Find the complex number z if $|z+1|=z+2(1+i)$.
Solution:
1. Let z = a+bi. Then the given equation becomes:
$\begin{array}{ll}
|a+bi+1|&{}={}&a+bi+2(1+i)& {} &{} \\
\Rightarrow |(a+1)+bi|&{}={}&a+bi+2+2i& {} &{} \\
\Rightarrow \sqrt{(a+1)^2+b^2}&{}={}&a+2+(b+2)i& {} &{} \\
\end{array}$
2. Equating the corresponding real and imaginary parts, we get:
(i) $\sqrt{(a+1)^2+b^2}~=~a+2$
(ii) $0 ~=~b+2$
3. From (ii), we get: b = -2
• Substituting for b in (i), we get:
$\begin{array}{ll}
\sqrt{(a+1)^2+b^2}&{}={}&a+2& {} &{} \\
\Rightarrow \sqrt{(a+1)^2+(-2)^2}&{}={}&a+2& {} &{} \\
\Rightarrow \sqrt{a^2+2a+1+4}&{}={}&a+2& {} &{} \\
\Rightarrow \sqrt{a^2+2a+5}&{}={}&a+2& {} &{} \\
\Rightarrow a^2+2a+5&{}={}&(a+2)^2& {} &{} \\
\phantom{\frac{1}{2-3i}}&{}&\color {green}{\text{(Squaring both sides)}} &{} \\
\Rightarrow a^2+2a+5&{}={}&a^2+4a+4& {} &{} \\
\Rightarrow 1&{}={}&2a& {} &{} \\
\Rightarrow a&{}={}&\frac{1}{2}& {} &{} \\
\end{array}$
4. Thus the complex number z = a+bi is $\frac{1}{2}-2i$


The link below gives a PDF file with more miscellaneous examples

Miscellaneous exercise on chapter 5


In the next chapter, we will see linear inequalities.

Previous

Contents

Next

Copyright©2022 Higher secondary mathematics.blogspot.com

Monday, May 23, 2022

Chapter 5.5 - Polar Representation of A Complex Number

In the previous section, we saw the details about Argand plane. In this section, we will see Polar representation.

Some basics can be written in 9 steps:
1. In fig.5.4 below, P(x,y) represents the complex number z = x+yi

Method of representing a complex number by polar coordinates.
Fig.5.4

• We have seen that, OP will be the modulus of z.
• Let the length of OP be r. Then we can write: OP = r = |z|
• PP1 is the perpendicular dropped from P onto the x axis.
• PP2 is the perpendicular dropped from P onto the y axis.
2. Let OP make an angle of šœ½ radians with the positive side of the x axis.
• Then we get:
   ♦ OP1 = r cos šœ½
   ♦ PP1 = r sin šœ½
3. Now we can write the complex number in terms of r and šœ½:
   ♦ OP1 = x. So we get x = r cos šœ½
   ♦ PP1 = OP2 = y. So we get: y = r sin šœ½
• Then the complex number z = x+yi can be written as: r cos šœ½ + r i sin šœ½
   ♦ This is same as: z = r(cos šœ½ + i sin šœ½)
4. So we have two methods to represent a complex number:
(i) z = x+yi
(ii) z = r(cos šœ½ + i sin šœ½)
• In the first method, two distances (x and y) will give the complex number.
   ♦ That is., the ordered pair (x,y) will give the complex number.
• In the second method, a distance (r) and an angle (šœ½) will give the complex number.
   ♦ That is., the ordered pair (r,šœ½) will give the complex number.
[Since šœ½ is measured in radians, it will be a real number. So (r,šœ½) is an ordered pair of real numbers.]
• We have already seen that, r (which is the modulus) can be calculated using x and y as: $|z|=\sqrt{x^2+y^2}$
5. Writing a complex number in the form  r(cos šœ½ + i sin šœ½) is called polar representation of a complex number.
• (r,šœ½) is called polar coordinates of the complex number.
• The origin is considered as the pole.
• šœ½ should be measured from the +ve direction of the x axis.
   ♦ šœ½ is called the argument of the complex number z.
   ♦ šœ½ is also called the amplitude of the complex number z.
6. In the above five steps, the complex number that we considered was in the first quadrant.
• But we may have to deal with complex numbers which are in the second, third or fourth quadrants also. This is shown in fig.5.5 below: 

Fig.5.5

• So šœ½ can be any value between 0 and 2Ļ€.
• šœ½ can be zero also. (This happens when the complex number is on the positive side of the x axis)
7. In chapter 3, we have seen that, even if šœ½ is greater than $\frac{\pi}{2}$,
   ♦ cosine will give the x coordinate of P   
   ♦ sine will give the y coordinate of P
   ♦ (Details here)   
• So even if šœ½ (argument) of a complex number is greater than $\frac{\pi}{2}$, we can use the polar representation for that complex number.
8. In chapter 3, we also saw that, šœ½ can be greater than 2Ļ€. But then the results will be same as completing one or more full rotations.
• So we will need only those values 'which are between 0 and 2Ļ€'. It will take care of all the four quadrants.
9. However, while dealing with complex numbers, mathematicians prefer another method. It can be written in 3 steps:
(i) If P is in the first or second quadrants, the argument is considered to be +ve.
• That is.,
    ♦ the rotation starts from the +ve side of the x axis in the anti-clockwise direction.
    ♦ the rotation ends at the -ve side of the x axis.    
(ii) If P is in the third or fourth quadrants, the argument is considered to be -ve.
• That is.,
    ♦ the rotation starts from the +ve side of the x axis in the clockwise direction.   
    ♦ the rotation ends at the -ve side of the x axis.
(iii) This method will also take care of all the four quadrants. It is shown in fig.5.6 below:

Fig.5.6



Now we will see some solved examples

Solved example 5.6
Represent the complex number $z=1+\sqrt{3}\,i$ in the polar form.
Solution:
1. The complex number is given to us in the form x+yi. We have to convert it into the form:
r[cos šœ½ + i sin šœ½]
• For that, we have to find the polar coordinates (r,šœ½)
2. Since the two forms are equal, we can equate the corresponding parts:
    ♦ Equating the real parts, we get: x = r cos šœ½
    ♦ Equating the imaginary parts, we get: y = r sin šœ½
3. We know that $r=|z|=\sqrt{x^2+y^2}$
• So in our present case, we get:
$r=\sqrt{1^2+(\sqrt{3})^2}=\sqrt{1+3}=\sqrt{4}=\pm 2$
• r is the distance between the complex number and the origin. A distance cannot be -ve. So we can write: r = 2 
4. From the results in (2), we get:
(i) $x=1=2 \cos \theta$
(ii) $y=\sqrt{3}=2 \sin \theta$
• We must find that value of šœ½ which satisfies both (i) and (ii)
5. Taking ratios, (ii) to (i), we get:
$\frac{2 \sin \theta}{2 \cos \theta}=\frac{\sqrt{3}}{1}$
$\Rightarrow \tan \theta = \sqrt{3}$
• This is a trigonometrical equation. We learned to solve them in chapter 3. (Details here)
6. We know that, $\tan \frac{\pi}{3}=\sqrt{3}$
• So we can write: $\tan \frac{\pi}{3}=\tan \theta = \sqrt{3}$
• From this we get: $\theta = \frac{\pi}{3}$
Check:
• Substituting this value of šœ½ in 4(i), we get:
$1=2 \cos \frac{\pi}{3} = 2 × \frac{1}{2} = 1$. This is true.
• Substituting this value of šœ½ in 4(ii), we get:
$\sqrt{3}=2 \sin \frac{\pi}{3} = 2 × \frac{\sqrt{3}}{2} = \sqrt{3}$. This is true.
• So $\theta = \frac{\pi}{3}$ is acceptable.
7. There is another possible value for šœ½. It can be calculated using the identity: tan šœ½ = tan (Ļ€+šœ½)
• So we can write:
$\tan \frac{\pi}{3}=\tan \theta = \tan \left(\pi + \theta \right)= \tan \left(\pi + \frac{\pi}{3}\right) = \sqrt{3}$
• From this we get: $\tan \theta = \tan \left( \frac{4\pi}{3}\right) = \sqrt{3}$
• So $\theta = \frac{4\pi}{3}$
Check:
• Substituting this value of šœ½ in 4(i), we get:
$1=2 \cos \frac{4\pi}{3} = 2 × -\frac{1}{2} = -1$. This is not true.
• Substituting this value of šœ½ in 4(ii), we get:
$\sqrt{3}=2 \sin \frac{4\pi}{3} = 2 × - \frac{\sqrt{3}}{2} = -\sqrt{3}$. This is not true.
• Value of šœ½ will be acceptable only if both equations 4(i) and 4(ii) are satisfied. So $\theta = \frac{4\pi}{3}$ is not acceptable.
8. Thus we get the values of r and šœ½:
   ♦ From (3), we get: r = 2
   ♦ From (6),we get: $\theta = \frac{4\pi}{3}$
9. So the required polar form is: $z=2\left(\sin \frac{\pi}{3}+i \cos \frac{\pi}{3}  \right)$.
• The point P in fig.5.7(a) below represents the given complex number in the Argand plane.

Fig.5.7


In the above example, we had to perform two checks. Those two checks can be avoided by using a simple trick. This can be explained in 4 steps:
1. We saw that two values of šœ½ are possible. This is because, tangent of šœ½ can be $\sqrt{3}$ on two occasions:
(i) When šœ½ = $\frac{\pi}{3}$  
(ii) When šœ½ = $\frac{4\pi}{3}$
2. But only one value is acceptable because in total, three equations should be satisfied:
(i) $1=2 \cos \theta$
(ii) $\sqrt{3}=2 \sin \theta$
(iii) $\sqrt{3}=\tan \theta$
3. We see that both sin šœ½ and cos šœ½ are +ve.
• This is possible only when šœ½ is in the first quadrant.
4. So we must choose that šœ½ which is in the first quadrant.
• Using this trick, the two checks can be avoided.


Solved example 5.7
Convert the complex number $z=\frac{-16}{1+\sqrt{3}\,i}$ in the polar form.
Solution:
1. First we have to convert the given complex number into the form x+yi. It can be done as shown below:
$\begin{array}{ll}
\frac{-16}{1+\sqrt{3}\,i}&{}={}&\frac{-16}{1+\sqrt{3}\,i} × \frac{1-\sqrt{3}\,i}{1-\sqrt{3}\,i}& {} &{} \\
\phantom{\frac{-16}{1+\sqrt{3}\,i}}&{}={}& \frac{(-16)(1-\sqrt{3}\,i)}{1^2-(\sqrt{3})^2(i)^2}&{} \\
\phantom{\frac{1}{2-3i}}&{}&\color {green}{(a+b)(a-b)=a^2-b^2} &{} \\
\phantom{\frac{-16}{1+\sqrt{3}\,i}}&{}={}& \frac{(-16)(1-\sqrt{3}\,i)}{1-(3)(-1)}&{} \\
\phantom{\frac{-16}{1+\sqrt{3}\,i}}&{}={}& \frac{(-16)(1-\sqrt{3}\,i)}{4}&{} \\
\phantom{\frac{-16}{1+\sqrt{3}\,i}}&{}={}& -4(1-\sqrt{3}\,i)&{} \\
\phantom{\frac{-16}{1+\sqrt{3}\,i}}&{}={}& -4+4\sqrt{3}\,i&{} \\
\end{array}$
2. Now the complex number is in the form x+yi. We have to convert this into the form:
r[cos šœ½ + i sin šœ½]
• For that, we have to find the polar coordinates (r,šœ½)
3. Since the two forms are equal, we can equate the corresponding parts:
    ♦ Equating the real parts, we get: x = r cos šœ½
    ♦ Equating the imaginary parts, we get: y = r sin šœ½
4. We know that $r=|z|=\sqrt{x^2+y^2}$
• So in our present case, we get:
$r=\sqrt{(-4)^2+(4\sqrt{3})^2}=\sqrt{16+(16 × 3)}=\sqrt{64}=\pm 8$
• r is the distance between the complex number and the origin. A distance cannot be -ve. So we can write: r = 8 
5. From the results in (3), we get:
(i) $x=-4=8 \cos \theta$
(ii) $y=4\sqrt{3}=8 \sin \theta$
• cos šœ½ is -ve and sin šœ½ is +ve. So šœ½ is in the second quadrant.
6. Taking ratios, (ii) to (i), we get:
$\frac{8 \sin \theta}{8 \cos \theta}=\frac{4\sqrt{3}}{-4}$
$\Rightarrow \tan \theta = -\sqrt{3}$
• This is a trigonometrical equation. We learned to solve them in chapter 3. (Details here)
7. We know that, $\tan \frac{\pi}{3}=\sqrt{3}$
• We have the identity: tan (Ļ€-šœ½) = -tan šœ½
If we put $\theta = \frac{\pi}{3}$, we get:
$\tan \left(\pi - \frac{\pi}{3}  \right)=-\tan \frac{\pi}{3} = -\sqrt{3}$
$\Rightarrow \tan \left(\frac{2\pi}{3}  \right)=-tan \frac{\pi}{3} = -\sqrt{3}$
$\Rightarrow \tan \theta = \tan \left(\frac{2\pi}{3}  \right) = -\sqrt{3}$
• From this we get: $\theta = \frac{2\pi}{3}$
8. There is another possible value for šœ½. It can be calculated using the identity: tan šœ½ = tan (Ļ€+šœ½)
• So we can write:
$\tan \frac{2\pi}{3}=\tan \theta = \tan \left(\pi + \theta \right)= \tan \left(\pi + \frac{2\pi}{3}\right) = -\sqrt{3}$
• From this we get: $\tan \theta = \tan \left( \frac{5\pi}{3}\right) = -\sqrt{3}$
• So $\theta = \frac{5\pi}{3}$
9. So we have two values:
• From (7), we have: $\theta = \frac{2\pi}{3}$
    ♦ This is in the second quadrant.
• From (8), we have: $\theta = \frac{5\pi}{3}$
    ♦ This is in the fourth quadrant.
10. In step (5), we saw that šœ½ is in the second quadrant.
• So $\theta = \frac{2\pi}{3}$ is the acceptable value.
11. Thus we get the values of r and šœ½:
   ♦ From (4), we get: r = 8
   ♦ From (10),we get: $\theta = \frac{2\pi}{3}$
12. So the required polar form is: $z=8\left(\sin \frac{2\pi}{3}+i \cos \frac{2\pi}{3}  \right)$.
• The point P in fig.5.7(b) above represents the given complex number in the Argand plane.


The link below gives a PDF file with more solved examples:

Exercise 5.2


• In the next section, we will see quadratic equations.

Previous

Contents

Next

Copyright©2022 Higher secondary mathematics.blogspot.com