Friday, December 30, 2022

Normal Form Example

It is necessary to practice how to give appropriate signs for sine and cosine terms in the normal form. We have seen an example in section 10.8. A similar example is given below:

Equation of a line is 3x - 5y - 15 = 0. Reduce this equation to normal form. Find the values of p and 𝜔.
Solution:
1. From the given equation, we get:
A = 3, B = -5 and C = -15
2. Calculation of p

$\begin{array}{ll}
{}&{p}
&{}={}& {\pm \frac{C}{\sqrt{A^2~+~B^2}}}
&{} \\

{}&{}
&{}={}& {\pm \frac{-15}{\sqrt{3^2~+~(-5)^2}}}
&{} \\

{}&{}
&{}={}& {\pm \frac{15}{\sqrt{34}}}
&{} \\

\end{array}$

2. Calculation of cos 𝜔

$\begin{array}{ll}
{}&{\cos \omega }
&{}={}& {\pm \frac{A}{\sqrt{A^2~+~B^2}}}
&{} \\

{}&{}
&{}={}& {\pm \frac{3}{\sqrt{3^2~+~(-5)^2}}}
&{} \\

{}&{}
&{}={}& {\pm \frac{3}{\sqrt{34}}}
&{} \\

\end{array}$

3. Calculation of sin 𝜔

$\begin{array}{ll}
{}&{\sin \omega }
&{}={}& {\pm \frac{B}{\sqrt{A^2~+~B^2}}}
&{} \\

{}&{}
&{}={}& {\pm \frac{-5}{\sqrt{3^2~+~(-5)^2}}}
&{} \\

{}&{}
&{}={}& {\pm \frac{5}{\sqrt{34}}}
&{} \\

\end{array}$

4. Now we determine the signs:
(i) Slope of the line = $m=-\frac{A}{B}~=~-\frac{3}{-5}~=~\frac{3}{5}$
• This is +ve. So we move along the left arrow of the chart in fig.13.36.
• The chart is shown again below:


(ii) x-intercept of the line = $a=-\frac{C}{A}~=~-\frac{-15}{3}~=~5$
• This is +ve. So sin 𝜔 is -ve and cos 𝜔 is +ve.

5. So we can write:

$\begin{array}{ll}
{}&{\sin \omega }
&{}={}& {- \frac{5}{\sqrt{35}}}
&{} \\

{}&{\cos \omega}
&{}={}& {\frac{3}{\sqrt{35}}}
&{} \\

\end{array}$

6.  The sign of p will be always +ve because, it is a distance.

7. Now we can write the normal form:

$\begin{array}{ll}
{}&{x \cos \omega~+~y \sin \omega}
&{}={}& {p}
&{} \\

{\Rightarrow}&{x × \frac{3}{\sqrt{35}}~+~y × - \frac{5}{\sqrt{35}}}
&{}={}& {\frac{15}{\sqrt{35}}}
&{} \\

{\Rightarrow}&{ \frac{3x}{\sqrt{35}}~+~ - \frac{5y}{\sqrt{35}}}
&{}={}& {\frac{15}{\sqrt{35}}}
&{} \\

{\Rightarrow}&{\frac{3x}{\sqrt{35}}~-~ \frac{5y}{\sqrt{35}}}
&{}={}& {\frac{15}{\sqrt{35}}}
&{} \\

\end{array}$

8. Calculation of 𝜔:
(i) From (5), we have: tan 𝜔 = -5/3
• Using a scientific calculator, we get: 𝜔 = -59.04o
(ii) In our present case, 𝜔 is in the fourth quadrant (sin is -ve and cos is +ve).
• -59.04o indeed lies in the fourth quadrant. But we want the +ve angle. The +ve angle corresponding to -59.04o is (360 - 59.04) = 300.96o
• We get: tan 𝜔 = tan -59.04 = tan 300.96
(iii) So the value of 𝜔 is 300.96o

9. So the normal form can be written as:
x cos 300.96o + y sin 300.96o = $\frac{15}{\sqrt{35}}$

• The actual plot is shown below:


 

 

Chapter 10.8 - More Details about Normal Form

In the previous section, we saw how slope, intercepts, 𝜔 and p can be obtained from the general equation of a line. We saw that, $\pm$ sign is present for p, cos 𝜔 and sin 𝜔. In this section, we will see how to apply those signs.

• We know that, sign of sin 𝜔, cos 𝜔 etc., will depend upon the position of the angle 𝜔.
• For example:
    ♦ If 𝜔 is in the I quadrant, sin 𝜔 will be +ve, cos 𝜔 will be +ve.
    ♦ If 𝜔 is in the III quadrant, sin 𝜔 will be -ve, cos 𝜔 will be +ve.
• There is an easy method to find the position of 𝜔. It involves the use of the flow chart in fig.10.34 below. It can be written in 5 steps:

Fig.10.34


1. We are given the equation of a line in the form Ax +By +C = 0.
• We want to find the signs of sin 𝜔, cos 𝜔 and p.
• The first step is to calculate the slope using the equation: $m=-\frac{A}{B}$
• If the slope is +ve, we move along the left arrow of the chart. All our works will then be in the left side of the vertical cyan line. 
• If the slope is -ve, we move along the right arrow of the chart. All our works will then be in the right side of the vertical cyan line.
2. Suppose that, the slope is +ve. Then we are in the left side of the cyan line.
• The second step is to calculate the x-intercept ‘a’ using the equation: $a=-\frac{C}{A}$
3. If ‘a’ is +ve, then we move along the left arrow.
• The y-intercept ‘b’ will be -ve.
• This condition is shown in fig.10.35(d) below. Note that in the fig.d, the line has a +ve slope, and x-intercept ‘a’ is +ve. Then the y-intercept will be -ve.

Fig.10.35

4. From the fig.d, it is clear that, if ‘a’ is +ve and ‘b’ is -ve, then the normal p will lie in the IV quadrant.
• Then sin will be -ve and cos will be +ve
• Thus we get the required signs.
5. With practice, we will not need to go through all the above steps. We can simply move along the appropriate arrows and write:
If m is +ve and a is +ve, then: sin is -ve and cos is +ve.
6. The sign of p will be always +ve because, it is a distance.

Let us see another case from the chart. It can be written in 5 steps:
1. Suppose that, the slope is -ve. Then we are in the right side of the cyan line.
• The second step is to calculate the x-intercept ‘a’ using the equation: $a=-\frac{C}{A}$
2. If ‘a’ is -ve, then we move along the right arrow.
• The y-intercept ‘b’ will be -ve.
• This condition is shown in fig.10.35(c) above. Note that in the fig.c, the line have a -ve slope, and x-intercept ‘a’ is -ve. Then the y-intercept will be -ve.
3. From the fig.c, it is clear that, if ‘a’ is -ve and ‘b’ is -ve, then the normal p will lie in the III quadrant.
• Then sin will be -ve and cos will be -ve
• Thus we get the required signs.
4. With practice, we will not need to go through all the above steps. We can simply move along the appropriate arrows and write:
If m is -ve and a is -ve, then: sin is -ve and cos is -ve.
5. The sign of p will be always +ve because, it is a distance.


Once we obtain a through knowledge on fig.10.34 and fig.10.35, we can avoid some intermediate steps and use a simplified chart. It is shown in fig.10.36 below:

Fig.10.36


Let us see an example where we use the simplified chart:

Equation of a line is 3x + 2y + 6 = 0. Reduce this equation to normal form. Find the values of p and 𝜔.
Solution:
1. From the given equation, we get:
A = 3, B = 2 and C = 6
2. Calculation of p

$\begin{array}{ll}
{}&{p}
&{}={}& {\pm \frac{C}{\sqrt{A^2~+~B^2}}}
&{} \\

{}&{}
&{}={}& {\pm \frac{6}{\sqrt{3^2~+~2^2}}}
&{} \\

{}&{}
&{}={}& {\pm \frac{6}{\sqrt{13}}}
&{} \\

\end{array}$

2. Calculation of cos 𝜔

$\begin{array}{ll}
{}&{\cos \omega }
&{}={}& {\pm \frac{A}{\sqrt{A^2~+~B^2}}}
&{} \\

{}&{}
&{}={}& {\pm \frac{3}{\sqrt{3^2~+~2^2}}}
&{} \\

{}&{}
&{}={}& {\pm \frac{3}{\sqrt{13}}}
&{} \\

\end{array}$

3. Calculation of sin 𝜔

$\begin{array}{ll}
{}&{\sin \omega }
&{}={}& {\pm \frac{B}{\sqrt{A^2~+~B^2}}}
&{} \\

{}&{}
&{}={}& {\pm \frac{2}{\sqrt{3^2~+~2^2}}}
&{} \\

{}&{}
&{}={}& {\pm \frac{2}{\sqrt{13}}}
&{} \\

\end{array}$

4. Now we determine the signs:
(i) Slope of the line = $m=-\frac{A}{B}~=~-\frac{3}{2}$
• This is -ve. So we move along the right arrow of the chart in fig.13.36
(ii) x-intercept of the line = $a=-\frac{C}{A}~=~-\frac{6}{3}~=~-2$
• This is -ve. So sin 𝜔 is -ve and cos 𝜔 is -ve.

5. So we can write:

$\begin{array}{ll}
{}&{\sin \omega }
&{}={}& {- \frac{2}{\sqrt{13}}}
&{} \\

{}&{\cos \omega}
&{}={}& {- \frac{3}{\sqrt{13}}}
&{} \\

\end{array}$

6.  The sign of p will be always +ve because, it is a distance.

7. Now we can write the normal form:

$\begin{array}{ll}
{}&{x \cos \omega~+~y \sin \omega}
&{}={}& {p}
&{} \\

{\Rightarrow}&{x × - \frac{3}{\sqrt{13}}~+~y × - \frac{2}{\sqrt{13}}}
&{}={}& {\frac{6}{\sqrt{13}}}
&{} \\

{\Rightarrow}&{- \frac{3x}{\sqrt{13}}~+~ - \frac{2y}{\sqrt{13}}}
&{}={}& {\frac{6}{\sqrt{13}}}
&{} \\

{\Rightarrow}&{\frac{3x}{\sqrt{13}}~+~ \frac{2y}{\sqrt{13}}}
&{}={}& {-\frac{6}{\sqrt{13}}}
&{} \\

\end{array}$

8. Calculation of 𝜔:
(i) From (5), we have: tan 𝜔 = 2/3
• Using a scientific calculator, we get: 𝜔 = 33.69o
(ii) But in our present case, 𝜔 is in the third quadrant (both sin and cos are -ve).
• So we find the other value of 𝜔 using the identity: tan x = tan (180 + x)
• We get: tan 𝜔 = tan 33.69 = tan (180 + 33.69) = tan 213.69
(iii) So the value of 𝜔 is 213.69o

9. So the normal form can be written as:
x cos 213.69o + y sin 213.69o = $\frac{6}{\sqrt{13}}$

• The actual plot is shown below:

Fig.10.37

 

• Another example can be seen here.


Now we will see some solved examples.

Solved example 10.13
The equation of a line is 3x - 4y + 10 = 0. Find it's (i) slope (ii) x - and y-intercepts.
Solution:
1. From the given equation, we can write:
A = 3, B = -4 and C = 10
2. Slope can be calculated as:
$m=-\frac{A}{B}~=~-\frac{3}{-4}~=~\frac{3}{4}$
3. x-intercept can be calculated as:
$a=-\frac{C}{A}~=~-\frac{10}{3}$
4. y-intercept can be calculated as:
$b=-\frac{C}{B}~=~-\frac{10}{-4}~=~\frac{5}{2}$

Solved example 10.14
Reduce the equation (√3)x + y - 8 = 0 into normal form. Find the values of p and 𝜔.
Solution:
1. From the given equation, we get:
A = √3, B = 1 and C = -8
2. Calculation of p

$\begin{array}{ll}
{}&{p}
&{}={}& {\pm \frac{C}{\sqrt{A^2~+~B^2}}}
&{} \\

{}&{}
&{}={}& {\pm \frac{-8}{\sqrt{(\sqrt{3})^2~+~1^2}}}
&{} \\

{}&{}
&{}={}& {\pm \frac{8}{\sqrt{4}}}
&{} \\

{}&{}
&{}={}& {\pm 4}
&{} \\

\end{array}$

2. Calculation of cos 𝜔

$\begin{array}{ll}
{}&{\cos \omega }
&{}={}& {\pm \frac{A}{\sqrt{A^2~+~B^2}}}
&{} \\

{}&{}
&{}={}& {\pm \frac{\sqrt{3}}{\sqrt{(\sqrt{3})^2~+~1^2}}}
&{} \\

{}&{}
&{}={}& {\pm \frac{\sqrt{3}}{\sqrt{4}}}
&{} \\

{}&{}
&{}={}& {\pm \frac{\sqrt{3}}{2}}
&{} \\

\end{array}$

3. Calculation of sin 𝜔

$\begin{array}{ll}
{}&{\sin \omega }
&{}={}& {\pm \frac{B}{\sqrt{A^2~+~B^2}}}
&{} \\

{}&{}
&{}={}& {\pm \frac{1}{\sqrt{(\sqrt{3})^2~+~1^2}}}
&{} \\

{}&{}
&{}={}& {\pm \frac{1}{\sqrt{4}}}
&{} \\

{}&{}
&{}={}& {\pm \frac{1}{2}}
&{} \\

\end{array}$

4. Now we determine the signs:
(i) Slope of the line = $m=-\frac{A}{B}~=~-\frac{\sqrt{3}}{1}~=~-\sqrt{3}$
• This is -ve. So we move along the right arrow of the chart in fig.13.36
(ii) x-intercept of the line = $a=-\frac{C}{A}~=~-\frac{-8}{\sqrt{3}}~=~\frac{8}{\sqrt{3}}$
• This is +ve. So sin 𝜔 is +ve and cos 𝜔 is +ve.

5. So we can write:

$\begin{array}{ll}
{}&{\sin \omega }
&{}={}& {\frac{1}{2}}
&{} \\

{}&{\cos \omega}
&{}={}& {\frac{\sqrt{3}}{2}}
&{} \\

\end{array}$

6.  The sign of p will be always +ve because, it is a distance.

7. Now we can write the normal form:

$\begin{array}{ll}
{}&{x \cos \omega~+~y \sin \omega}
&{}={}& {p}
&{} \\

{\Rightarrow}&{x × \frac{\sqrt{3}}{2}~+~y × \frac{1}{2}}
&{}={}& {4}
&{} \\

{\Rightarrow}&{\frac{\sqrt{3}x}{2}~+~\frac{y}{2}}
&{}={}& {4}
&{} \\

\end{array}$

8. Calculation of 𝜔:
(i) From (5), we have: $\tan \omega ~=~\frac{1}{\sqrt{3}}$
• We know that $\tan 30 ~=~\frac{1}{\sqrt{3}}$
(ii) In our present case, 𝜔 is in the first quadrant (both sin and cos are +ve).
• So 30o is the correct value of 𝜔

9. So the normal form can be written as:
x cos cos 30o + y sin 30o = 4

Solved example 10.15
Find the angle between the lines y - (√3)x - 5 = 0 and (√3)y - x + 6 = 0
Solution:
1. The first line given is: y - (√3)x - 5 = 0
• Rearranging this into the general form, we get: (√3)x - y + 5 = 0
• So we can write:
A = √3, B = -1 and C = 5
• Thus we get: $m_1=-\frac{A}{B}~=~-\frac{\sqrt{3}}{-1}~=~\sqrt{3}$
2. The second line given is: (√3)y - x + 6 = 0
• Rearranging this into the general form, we get: x - (√3)y - 6 = 0
• So we can write:
A = 1, B = -√3 and C = -6
• Thus we get: $m_2=-\frac{A}{B}~=~-\frac{1}{-\sqrt{3}}~=~\frac{1}{\sqrt{3}}$

3. We have two slopes and we are asked to find the angle between the lines
   ♦ So this problem belongs to case I.
• We have seen the details about case I and case II here.
• Since this problem belongs to case I, there is no need to interchange the slopes and explore the two possibilities.
• We have the equation: $\tan \theta~=~\frac{m_2~-~m_1}{1~+~m_1 m_2}$
• Substituting the known values, we get:
$\begin{array}{ll}
{}&{\tan \theta}
&{}={}& {\frac{\frac{1}{\sqrt{3}}~-~\sqrt{3}}{1~+~\sqrt{3}  × \frac{1}{\sqrt{3}}}}
&{} \\

{\Rightarrow}&{\tan \theta}
&{}={}& {\frac{1 ~-~3}{\sqrt{3}~+~\sqrt{3}}}
&{} \\

{\Rightarrow}&{\tan \theta}
&{}={}& {\frac{-2}{2 \sqrt{3}}}
&{} \\

{\Rightarrow}&{\tan \theta}
&{}={}& {\frac{-1}{\sqrt{3}}}
&{} \\

\end{array}$

4. So we have to solve the equation: tan 𝜃 = $-\frac{1}{\sqrt{3}}$
It can be solved in 5 steps:
(i) Given that, tan θ = $-\frac{1}{\sqrt{3}}$
(ii) We know that, tan 30 = $\frac{1}{\sqrt{3}}$
• Using the identities 9.d and 9.c, we have: tan (180 – θ) = - tan θ
(See the list of identities here)
• So we can write: tan (180 – 30) = -tan 30
• That means: tan 150 = -tan 30
(iii) But tan 30 = $\frac{1}{\sqrt{3}}$
• So the result in (ii) becomes:
tan 150 = -tan 30 = $-\frac{1}{\sqrt{3}}$
(iv) We are given that, tan θ = $-\frac{1}{\sqrt{3}}$
• Including this in (iii), we get:
tan 150 = -tan 30 = $-\frac{1}{\sqrt{3}}$ = tan θ
• Picking the first and last items , we get:
tan 150 = tan θ
(v) So the first principal solution is: θ = 150o
5. We need only one principal solution. It indicates that, one of the angls between the two given lines is 150o.
• If one of the angles is 150o, then obviously, the other angle will be (180 - 150) = 30o

Solved example 10.16
Show that the two lines a1x + b1y + c1 = 0 and a2x + b2y + c2 = 0, where b1, b2 ≠ 0 are: (i) Parallel if $\frac{a_1}{b_1}~=~\frac{a_2}{b_2}$ and (ii) Perpendicular if a1a2 + b1b2 = 0
Solution:
1. The first line given is: a1x + b1 y + c1 = 0
• So we can write:
A = a1, B = b1 and C = c1
• Thus we get: $m_1=-\frac{A}{B}~=~-\frac{a_1}{b_1}$
2. The second line given is: a2x + b2 y + c2 = 0
• So we can write:
A = a2, B = b2 and C = c2
• Thus we get: $m_2=-\frac{A}{B}~=~-\frac{a_2}{b_2}$
3. If the two lines are parallel, then the two slopes will be equal.
• In such a situation, we get:

$\begin{array}{ll}
{}&{m_1}
&{}={}& {m_2}
&{} \\

{\Rightarrow}&{-\frac{a_1}{b_1}}
&{}={}& {-\frac{a_2}{b_2}}
&{} \\

{\Rightarrow}&{\frac{a_1}{b_1}}
&{}={}& {\frac{a_2}{b_2}}
&{} \\

\end{array}$

4. If the two lines are perpendicular, then m1 will be the -ve reciprocal of m2.
• In such a situation, we get:

$\begin{array}{ll}
{}&{m_1}
&{}={}& {-\frac{1}{m_2}}
&{} \\

{\Rightarrow}&{-\frac{a_1}{b_1}}
&{}={}& {\frac{-1}{-\frac{a_2}{b_2}}}
&{} \\

{\Rightarrow}&{-\frac{a_1}{b_1}}
&{}={}& {\frac{1}{\frac{a_2}{b_2}}}
&{} \\

{\Rightarrow}&{-\frac{a_1}{b_1}}
&{}={}& {\frac{b_2}{a_2}}
&{} \\

{\Rightarrow}&{-a_1 a_2}
&{}={}& {b_1 b_2}
&{} \\

{\Rightarrow}&{a_1 a_2~+~b_1 b_2}
&{}={}& {0}
&{} \\

\end{array}$

Solved example 10.17
Find the equation of a line perpendicular to the line x - 2y + 3 = 0 and passing through the point (1, -2)
Solution:
1. The line given is: x - 2y + 3 = 0
• So we can write:
A = 1, B = -2 and C = 5
• Thus we get: $m=-\frac{A}{B}~=~-\frac{1}{-2}~=~\frac{1}{2}$
2. So slope of the line perpendicular to the given line will be the -ve reciprocal, which is -2.
3. Now we have the slope of the required line. A point on the line is given.
We can use the point-slope form: y - y0 = m(x-x0)

$\begin{array}{ll}
{}&{y~-~-2}
&{}={}& {-2(x~-~1)}
&{} \\

{\Rightarrow}&{y~+~2}
&{}={}& {-2x~+~2}
&{} \\

{\Rightarrow}&{2x~+~y}
&{}={}& {0}
&{} \\

\end{array}$


In the next section, we will see distance of a point from a line.

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Thursday, December 29, 2022

Chapter 10.7 - General Equation of A Line

In the previous section, we saw the normal form of the equation of a line. In this section, we will see the general equation of a line.

Some basics about the general equation can be written in 4 steps:
1. Consider the equation: Ax + By + C = 0
• It is a first degree equation in two variables.
2. Let us put some random values for A, B and C:
A = 2, B = 3 and C = 5. Now the equation becomes: 2x + 3y + 5 = 0
• In this equation, if we put some random values for x, we will get corresponding values for y.
• For example:
    ♦ If x = 2, then y will be -3
    ♦ If x = 3, then y will be -3.67
    ♦ If x = 6, then y will be -5.67
    ♦ If x = 7, then y will be -6.33
3. So we get some coordinates: (2,-3), (3,-3.67), (6,-5.67), (7,-6.33)
• If we plot these coordinates, they will lie on a straight line. This is shown in fig.10.33 below:

Fig.10.33

4. So we can write:
• Any equation of the form Ax + By + C = 0 is called general linear equation.
• It is also called general equation of a line.
◼ But there is one condition:
A and B should not be zero simultaneously.
• This can be explained in 3 steps:
(i) If A = 0, the general equation will become: By + C = 0
    ♦ This is OK because, By + C = 0 will give a straight line.
(ii) If B = 0, the general equation will become: Ax + C = 0
    ♦ This is OK because, Ax + C = 0 will give a straight line.
(iii) If A = 0 and B = 0, the general equation will become: C = 0
    ♦ This is not OK because, C = 0 will not give a straight line.


• Now we will see the different forms of Ax + By + C = 0
• We have seen:
    ♦ Slope-intercept form
    ♦ Intercept form
    ♦ Normal form.
• The general equation can be written in each of these three forms.


First we will see the slope-intercept form. It can be written in 11 steps:
1. The slope-intercept form is: y = mx + c
2. The general form is: Ax + By + C = 0
3. Let the equations in both (1) and (2) represent the same line.
4. The point at which (1) intersects the x-axis can be obtained by putting y = 0.
So we get:

$\begin{array}{ll}
{}&{y}
&{}={}& {mx+c}
&{} \\

{\Rightarrow}&{0}
&{}={}& {mx+c}
&{} \\

{\Rightarrow}&{x}
&{}={}& {-\frac{c}{m}}
&{} \\

\end{array}$

5. So the line in (1) intersects the x-axis at $\left(-\frac{c}{m},~0 \right)$
• But the equations in both (1) and (2) represent the same line. So this point must satisfy (2) also.

• We can write:
$\begin{array}{ll}
{}&{Ax + By + C}
&{}={}& {0}
&{} \\

{\Rightarrow}&{A × -\frac{c}{m} ~+~B × 0~+~C}
&{}={}& {0}
&{} \\

{\Rightarrow}&{-\frac{Ac}{m}~+~C}
&{}={}& {0}
&{} \\

\end{array}$

6. The point at which (1) intersects the y-axis can be obtained by putting x = 0.
So we get:

$\begin{array}{ll}
{}&{y}
&{}={}& {mx+c}
&{} \\

{\Rightarrow}&{y}
&{}={}& {m × 0+c}
&{} \\

{\Rightarrow}&{y}
&{}={}& {c}
&{} \\

\end{array}$

7. So the line in (1) intersects the y-axis at (0,c)
• But the equations in both (1) and (2) represent the same line. So this point must satisfy (2) also.

• We can write:
$\begin{array}{ll}
{}&{Ax + By + C}
&{}={}& {0}
&{} \\

{\Rightarrow}&{A × 0 ~+~B × c~+~C}
&{}={}& {0}
&{} \\

{\Rightarrow}&{B × c~+~C}
&{}={}& {0}
&{} \\

{\Rightarrow}&{c}
&{}={}& {-\frac{C}{B}}
&{} \\

\end{array}$

8. Substituting this value of c in (5), we get:

$\begin{array}{ll}
{}&{-\frac{Ac}{m}~+~C}
&{}={}& {0}
&{} \\

{\Rightarrow}&{-\frac{A}{m} × -\frac{C}{B}~+~C}
&{}={}& {0}
&{} \\

{\Rightarrow}&{-\frac{A}{m} × -\frac{1}{B}~+~1}
&{}={}& {0}
&{} \\

{\Rightarrow}&{\frac{A}{B m}~+~1}
&{}={}& {0}
&{} \\

{\Rightarrow}&{\frac{A}{Bm}}
&{}={}& {-1}
&{} \\

{\Rightarrow}&{m}
&{}={}& {-\frac{A}{B}}
&{} \\

\end{array}$

9. So we get the following results:
    ♦ From (7), we get: $c~=~-\frac{C}{B}$
    ♦ From (8), we get: $m~=~-\frac{A}{B}$
10. Now we can write:
• If we are given the equation of a line in the general form Ax + By + C = 0, then:
    ♦ Slope of that line can be obtained as: $m~=~-\frac{A}{B}$
    ♦ y-intercept of that line can be obtained as: $c~=~-\frac{C}{B}$
11. If B = 0, then the general equation becomes: $x~=~-\frac{C}{A}$
    ♦ This is an equation of vertical line.
    ♦ It’s slope is undefined.
        ✰ Indeed "$m~=~-\frac{A}{B}$" is undefined if B = 0
    ♦ It intersects the x axis at $-\frac{C}{A}$.


Next we will see the intercept form. It can be written in 10 steps:
1. The intercept form is: $\frac{x}{a}~+~\frac{y}{b}~=~1$
2. The general form is: Ax + By + C = 0
3. Let the equations in both (1) and (2) represent the same line.
4. The point at which (1) intersects the x-axis can be obtained by putting y = 0.
So we get:

$\begin{array}{ll}
{}&{\frac{x}{a}~+~\frac{y}{b}}
&{}={}& {1}
&{} \\

{\Rightarrow}&{\frac{x}{a}~+~\frac{0}{b}}
&{}={}& {1}
&{} \\

{\Rightarrow}&{\frac{x}{a}}
&{}={}& {1}
&{} \\

{\Rightarrow}&{x}
&{}={}& {a}
&{} \\

\end{array}$

5. So the line in (1) intersects the x-axis at (a,0)
• But the equations in both (1) and (2) represent the same line. So this point must satisfy (2) also.

• We can write:
$\begin{array}{ll}
{}&{Ax + By + C}
&{}={}& {0}
&{} \\

{\Rightarrow}&{A × a ~+~B × 0~+~C}
&{}={}& {0}
&{} \\

{\Rightarrow}&{Aa~+~C}
&{}={}& {0}
&{} \\

{\Rightarrow}&{a}
&{}={}& {-\frac{C}{A}}
&{} \\

\end{array}$

6. The point at which (1) intersects the y-axis can be obtained by putting x = 0.
So we get:

$\begin{array}{ll}
{}&{\frac{x}{a}~+~\frac{y}{b}}
&{}={}& {1}
&{} \\

{\Rightarrow}&{\frac{0}{a}~+~\frac{y}{b}}
&{}={}& {1}
&{} \\

{\Rightarrow}&{\frac{y}{b}}
&{}={}& {1}
&{} \\

{\Rightarrow}&{y}
&{}={}& {b}
&{} \\

\end{array}$

7. So the line in (1) intersects the x-axis at (0,b)
• But the equations in both (1) and (2) represent the same line. So this point must satisfy (2) also.

• We can write:
$\begin{array}{ll}
{}&{Ax + By + C}
&{}={}& {0}
&{} \\

{\Rightarrow}&{A × 0 ~+~B × b~+~C}
&{}={}& {0}
&{} \\

{\Rightarrow}&{B × b~+~C}
&{}={}& {0}
&{} \\

{\Rightarrow}&{b}
&{}={}& {-\frac{C}{B}}
&{} \\

\end{array}$

8. So we get the following results:
    ♦ From (5), we get: $a~=~-\frac{C}{A}$
    ♦ From (7), we get: $b~=~-\frac{C}{B}$
9. Now we can write:
• If we are given the equation of a line in the general form Ax + By + C = 0, then:
    ♦ x-intercept of that line can be obtained as: $a~=~-\frac{C}{A}$
    ♦ y-intercept of that line can be obtained as: $b~=~-\frac{C}{B}$
        ✰ Note that, we obtained the same y-intercept in slope-intercept form also.
10.If C = 0, then:
    ♦ x-intercept = $-\frac{0}{A}$ = 0
    ♦ y-intercept = $-\frac{0}{B}$ = 0
• That means, the line will pass through the origin.
◼ We can write:
In the general equation of a line, if "term with no variable" is absent, then that line will pass through the origin.


Next we will see the normal form. It can be written in 12 steps:
1. The normal form is: $x \cos \omega~+~y \sin \omega~=~p$
2. The general form is: Ax + By + C = 0
3. Let the equations in both (1) and (2) represent the same line.
4. The point at which (1) intersects the x-axis can be obtained by putting y = 0.
So we get:

$\begin{array}{ll}
{}&{x \cos \omega~+~y \sin \omega}
&{}={}& {p}
&{} \\

{\Rightarrow}&{x \cos \omega~+~0 × \sin \omega}
&{}={}& {p}
&{} \\

{\Rightarrow}&{x \cos \omega}
&{}={}& {p}
&{} \\

{\Rightarrow}&{x}
&{}={}& {\frac{p}{\cos \omega}}
&{} \\

\end{array}$

5. So the line in (1) intersects the x-axis at $\left(\frac{p}{\cos \omega},~0 \right)$
• But the equations in both (1) and (2) represent the same line. So this point must satisfy (2) also.

• We can write:
$\begin{array}{ll}
{}&{Ax + By + C}
&{}={}& {0}
&{} \\

{\Rightarrow}&{A × \frac{p}{\cos \omega} ~+~B × 0~+~C}
&{}={}& {0}
&{} \\

{\Rightarrow}&{\frac{A p}{\cos \omega}~+~C}
&{}={}& {0}
&{} \\

{\Rightarrow}&{\cos \omega}
&{}={}& {-\frac{Ap}{C}}
&{} \\

\end{array}$

6. The point at which (1) intersects the y-axis can be obtained by putting x = 0.
So we get:

$\begin{array}{ll}
{}&{x \cos \omega~+~y \sin \omega}
&{}={}& {p}
&{} \\

{\Rightarrow}&{0 × \cos \omega~+~ y \sin \omega}
&{}={}& {p}
&{} \\

{\Rightarrow}&{y \sin \omega}
&{}={}& {p}
&{} \\

{\Rightarrow}&{y}
&{}={}& {\frac{p}{\sin \omega}}
&{} \\

\end{array}$

7. So the line in (1) intersects the x-axis at $\left(0,~\frac{p}{\sin \omega} \right)$
• But the equations in both (1) and (2) represent the same line. So this point must satisfy (2) also.

• We can write:
$\begin{array}{ll}
{}&{Ax + By + C}
&{}={}& {0}
&{} \\

{\Rightarrow}&{A × 0 ~+~B × \frac{p}{\sin \omega}~+~C}
&{}={}& {0}
&{} \\

{\Rightarrow}&{\frac{B p}{\sin \omega}~+~C}
&{}={}& {0}
&{} \\

{\Rightarrow}&{\sin \omega}
&{}={}& {-\frac{Bp}{C}}
&{} \\

\end{array}$

8. So we get the following results:
    ♦ From (5), we get: $\cos \omega~=~-\frac{Ap}{C}$
    ♦ From (7), we get: $\sin \omega~=~-\frac{Bp}{C}$
9. But $\sin^2 \omega~+~\cos^2 \omega~=~1$
So we get:
$\begin{array}{ll}
{}&{\left(-\frac{Bp}{C} \right)^2~+~\left(-\frac{Ap}{C} \right)^2}
&{}={}& {1}
&{} \\

{\Rightarrow}&{\frac{B^2 p^2}{C^2}~+~\frac{A^2 p^2}{C^2}}
&{}={}& {1}
&{} \\

{\Rightarrow}&{\frac{ p^2(A^2~+~B^2)}{C^2}}
&{}={}& {1}
&{} \\

{\Rightarrow}&{p^2}
&{}={}& {\frac{C^2}{A^2~+~B^2}}
&{} \\

{\Rightarrow}&{p}
&{}={}& {\pm \frac{C}{\sqrt{A^2~+~B^2}}}
&{} \\

\end{array}$

10. We can substitute this value of p in (5). We get:

$\begin{array}{ll}
{}&{\cos \omega}
&{}={}& {-\frac{Ap}{C}}
&{} \\

{}&{}
&{}={}& {-\frac{A}{C}~ × ~\pm \frac{C}{\sqrt{A^2~+~B^2}}}
&{} \\

{}&{}
&{}={}& {\pm \frac{A}{\sqrt{A^2~+~B^2}}}
&{} \\

\end{array}$

11. Similarly, we can substitute this value of p in (7). We get:

$\begin{array}{ll}
{}&{\sin \omega}
&{}={}& {-\frac{Bp}{C}}
&{} \\

{}&{}
&{}={}& {-\frac{B}{C}~ × ~\pm \frac{C}{\sqrt{A^2~+~B^2}}}
&{} \\

{}&{}
&{}={}& {\pm \frac{B}{\sqrt{A^2~+~B^2}}}
&{} \\

\end{array}$

12. Thus we get three results:
    ♦ From (9), we get: $p~=~\pm \frac{C}{\sqrt{A^2~+~B^2}}$ 
    ♦ From (10), we get: $\cos \omega~=~\pm \frac{A}{\sqrt{A^2~+~B^2}}$ 
    ♦ From (11), we get: $\sin \omega~=~\pm \frac{B}{\sqrt{A^2~+~B^2}}$


Let us compile the above results. It can be done in 5 steps:
1. Slope of a given line can be calculated as: $m~=~-\frac{A}{B}$
• This result is available from slope-intercept form.
2. x-intercept of a given line can be calculated as: $c~=~-\frac{C}{A}$
• This result is available from intercept form.
3. y-intercept of a given line can be calculated as: $c~=~-\frac{C}{B}$
• This result is available from both slope-intercept form and intercept form.
4. For writing the normal form, we can use three results:
    ♦ $p~=~\pm \frac{C}{\sqrt{A^2~+~B^2}}$ 
    ♦ $\cos \omega~=~\pm \frac{A}{\sqrt{A^2~+~B^2}}$ 
    ♦ $\sin \omega~=~\pm \frac{B}{\sqrt{A^2~+~B^2}}$
5. These results are easy to remember because, they follow a pattern.


• In the above results, we have $\pm$ sign for p, $\cos \omega$ and $\sin \omega$.
• So two questions arise:
    ♦ When do we use the '+' sign ?  
    ♦ When do we use the '-' sign ?
• We will see the answers in the next section.

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Friday, December 16, 2022

Chapter 10.6 - Normal Form

In the previous section, we saw the intercept form of the equation of a line. In this section, we will see normal form.

Normal form

Let us first see what a normal is. It can be written in 3 steps:
1. 'Normal' is another word of 'perpendicular line'.
2. Suppose that, we have a line L1. We can draw another line L2 in such a way that, L2 is perpendicular to L1.
3. Then we say that, L2 is a normal to L1


• Suppose that, we are give the following two items:
    ♦ Length of the normal from the origin to the line
    ♦ Angle which the normal makes with the +ve direction of the x-axis.
• Then we can quickly write the equation of the line. Let us see how it is done.    

Case I
This can be written in 5 steps:
1. In fig.10.29(a) below, OA is the normal to the line L1.
• The length OA is p
• OA makes an angle of ω with the +ve direction of the x-axis.

Derivation of the normal form of the equation of a line in analytic geometry.
Fig.10.29


2. Our first task is to find the slope of OA
• We know that, the slope of any line is the tangent of the inclination (angle with the +ve side of the x-axis).
• So the slope of OA = tan ω
3. Our next task is to find the slope of L1
• In step (2), we have calculated the slope of OA.
• OA is perpendicular to L1. So the slope of L1 will be the -ve reciprocal of the slope of OA.
• Thus we get:  
 Slope of L1 = $\frac{-1}{\tan \omega}$
4. Next, we want the coordinates of point A
• For that, we drop a perpendicular from A to the x-axis. M is the foot of the perpendicular.
• From the triangle OAM, we have:
    ♦ OM = p cos ω
    ♦ AM = p sin ω
• So the coordinates of A will be (p cos ω , p sin ω)
5. So now we have the slope of L1. We also have a point on L1.
• We can use the point-slope form. We get:
$\begin{array}{ll}
{}&{y-y_0}
&{}={}& {m(x-x_0)}
&{} \\

{\Rightarrow}&{y~-~p \sin \omega}
&{}={}& {\frac{-1}{\tan \omega}(x~-~p \cos \omega)}
&{} \\

{\Rightarrow}&{y~-~p \sin \omega}
&{}={}& {\frac{- \cos \omega}{\sin \omega}(x~-~p \cos \omega)}
&{} \\

{\Rightarrow}&{y \sin \omega~-~p \sin^2 \omega}
&{}={}& {-x \cos \omega~+~p \cos^2 \omega}
&{} \\

{\Rightarrow}&{x \cos \omega~+~y \sin \omega}
&{}={}& {p \sin^2 \omega~+~p \cos^2 \omega}
&{} \\

{\Rightarrow}&{x \cos \omega~+~y \sin \omega}
&{}={}& {p (\sin^2 \omega~+~ \cos^2 \omega)}
&{} \\

{\Rightarrow}&{x \cos \omega~+~y \sin \omega}
&{}={}& {p}
&{\color {green}{\text{- - - (a)}}} \\

\end{array}$

◼ Remarks:
• Line marked as (a):
sin2ω + cos2ω = 1

Case II
This can be written in 8 steps:
1. In case I, we derived an equation based on fig.10.29(a) above.
• In this fig.,
    ♦ the line intersects the x-axis at the +ve side.
    ♦ the line intersects the y-axis also at the +ve side.
2. What if
    ♦ the line intersect the x-axis at the -ve side.
    ♦ the line intersect the y-axis at the +ve side.
• Such a situation is shown in fig.10.29(b) above.
3. But this situation should not discourage us. Because here also, we can obtain the slope of the red line. Also we can obtain the coordinates of A.
4. In fig.10.29(b) above, OA is the normal to the line L2.
• The length OA is p
• OA makes an angle of ω with the +ve direction of the x-axis.  
5. Our first task is to find the slope of OA
• We know that, the slope of any line is the tangent of the inclination (angle with the +ve side of the x-axis).
• So the slope of OA = tan ω
• We see that, OA is sloping downwards. That means, as we move along the x-axis towards the +ve side, the line OA is falling. So OA must have a -ve slope.
• Consider the angle ω in fig.10.29(b). It lies in the second quadrant. In the second quadrant, tan is -ve. So the slope tan ω will be -ve.
• We do not have to worry about the sign of the slope of OA. All we need to write is that: Slope of OA is tan ω. The ω will take care of the sign. 
6. Our next task is to find the slope of L2
• In step (5), we have calculated the slope of OA.
• OA is perpendicular to L2. So the slope of L2 will be the -ve reciprocal of the slope of OA.
• Thus we get:  
Slope of L2 = $\frac{-1}{\tan \omega}$
7. Next, we have to find the coordinates of point A
• For that, we drop a perpendicular from A to the x-axis. M is the foot of the perpendicular.
• From the triangle OAM, we have:
    ♦ OM = p cos (180 - ω) = -pcos ω
        ✰ See identity 9.c in the list of trigonometric identities.
    ♦ AM = p sin (180 - ω) = p sin ω
        ✰ See identity 9.d in the list of trigonometric identities.
• So the coordinates of A will be (-p cos ω , p sin ω)
• Here also, we do not have to worry about the sign of the x-coordinate. Since ω is in the second quadrant, cos ω will automatically become -ve.
• We can write the coordinates of A as: (p cos ω , p sin ω)
8. So now we have the slope of L2. We also have a point on L2.
• Both are same as in case I. So we will get the same equation as in case I:
The equation of line L2 is: $x \cos \omega~+~y \sin \omega = p$

Case III
This can be written in 8 steps:
1. In case I, we derived an equation based on fig.10.29(a) above.
• In this fig.,
    ♦ the line intersects the x-axis at the +ve side.
    ♦ the line intersects the y-axis also at the +ve side.
2. What if
    ♦ the line intersect the x-axis at the -ve side.
    ♦ the line intersect the y-axis also  at the -ve side.
• Such a situation is shown in fig.10.30(a) below:

Fig.10.30

3. But this situation should not discourage us. Because here also, we can obtain the slope of the red line. Also we can obtain the coordinates of A.
4. In fig.10.30(a) above, OA is the normal to the line L3.
• The length OA is p
• OA makes an angle of ω with the +ve direction of the x-axis.  
5. Our first task is to find the slope of OA
• We know that, the slope of any line is the tangent of the inclination (angle with the +ve side of the x-axis).
• So the slope of OA = tan ω
• We see that, OA is sloping upwards. That means, as we move along the x-axis towards the +ve side, the line OA is rising. So OA must have a +ve slope.
• Consider the angle ω in fig.10.30(a). It lies in the third quadrant. In the third quadrant, tan is +ve. So the slope tan ω will be +ve.
• We do not have to worry about the sign of the slope of OA. All we need to write is that: Slope of OA is tan ω. The ω will take care of the sign. 
6. Our next task is to find the slope of L3
• In step (5), we have calculated the slope of OA.
• OA is perpendicular to L3. So the slope of L3 will be the -ve reciprocal of the slope of OA.
• Thus we get:  
Slope of L3 = $\frac{-1}{\tan \omega}$
7. Next, we have to find the coordinates of point A
• For that, we drop a perpendicular from A to the x-axis. M is the foot of the perpendicular.
• From the triangle OAM, we have:
    ♦ OM = p cos (ω - 180) = pcos [-(180 - ω)] = pcos (180 - ω) = -p cos ω
        ✰ See identities 2 and 9.c in the list of trigonometric identities.
    ♦ AM = p sin (ω - 180) = p sin [-(180 - ω)] = -p sin (180 - ω) = -p sin ω
        ✰ See identities 1 and 9.d in the list of trigonometric identities.
• So the coordinates of A will be (-p cos ω , -p sin ω)
• Here also, we do not have to worry about the sign of the x and y coordinates. Since ω is in the third quadrant, both sin ω and cos ω will automatically become -ve.
• We can write the coordinates of A as: (p cos ω , p sin ω)
8. So now we have the slope of L3. We also have a point on L3.
• Both are same as in case I. So we will get the same equation as in case I:
The equation of line L3 is: $x \cos \omega~+~y \sin \omega = p$

Case IV
This can be written in 8 steps:
1. In case I, we derived an equation based on fig.10.29(a) above.
• In this fig.,
    ♦ the line intersects the x-axis at the +ve side.
    ♦ the line intersects the y-axis also at the +ve side.
2. What if
    ♦ the line intersect the x-axis at the +ve side.
    ♦ the line intersect the y-axis at the -ve side.
• Such a situation is shown in fig.10.30(b) above.

3. But this situation should not discourage us. Because here also, we can obtain the slope of the red line. Also we can obtain the coordinates of A.
4. In fig.10.30(b) above, OA is the normal to the line L4.
• The length OA is p
• OA makes an angle of ω with the +ve direction of the x-axis.  
5. Our first task is to find the slope of OA
• We know that, the slope of any line is the tangent of the inclination (angle with the +ve side of the x-axis).
• So the slope of OA = tan ω
• We see that, OA is sloping downwards. That means, as we move along the x-axis towards the +ve side, the line OA is falling. So OA must have a -ve slope.
• Consider the angle ω in fig.10.30(b). It lies in the fourth quadrant. In the fourth quadrant, tan is -ve. So the slope tan ω will be -ve.
• We do not have to worry about the sign of the slope of OA. All we need to write is that: Slope of OA is tan ω. The ω will take care of the sign. 
6. Our next task is to find the slope of L4
• In step (5), we have calculated the slope of OA.
• OA is perpendicular to L4. So the slope of L4 will be the -ve reciprocal of the slope of OA.
• Thus we get:  
Slope of L4 = $\frac{-1}{\tan \omega}$
7. Next, we have to find the coordinates of point A
• For that, we drop a perpendicular from A to the x-axis. M is the foot of the perpendicular.
• From the triangle OAM, we have:
    ♦ OM = p cos (360 - ω) = pcos ω
        ✰ See identity 9.g in the list of trigonometric identities.
    ♦ AM = p sin (360 - ω) = -p sin ω
        ✰ See identity 9.h in the list of trigonometric identities.
• So the coordinates of A will be (p cos ω , -p sin ω)
• Here also, we do not have to worry about the sign of the x and y coordinates. Since ω is in the fourth quadrant, sin ω will be -ve and cos ω will be +ve.
• We can write the coordinates of A as: (p cos ω , p sin ω)
8. So now we have the slope of L4. We also have a point on L4.
• Both are same as in case I. So we will get the same equation as in case I:
The equation of line L4 is: $x \cos \omega~+~y \sin \omega = p$


• Based on the four cases, we can write:
Whatever be the orientation of the line, we can use the equation:
$x \cos \omega~+~y \sin \omega = p$
    ♦ The required signs will be taken care of by the angle ω.


Let us see some solved examples:

Solved example 10.12
Find the equation of the line whose perpendicular distance from the origin is 4 units and the angle which the normal makes with +ve direction of x-axis is 15o
Solution:
1. Given that:
p = 4 units and ω = 15o
2. We can use the equation: $x \cos \omega~+~y \sin \omega = p$
• So we have to find cos ω and sin ω
3. We have calculated the cosine and sine of 15o in chapter 3.
    ♦ cos ω = cos 15 = $\frac{\sqrt{3} + 1}{2 \sqrt{2}}$
    ♦ sin ω = sin 15 = $\frac{\sqrt{3} - 1}{2 \sqrt{2}}$
4. Substituting the known values in the equation in (2), we get:

$\begin{array}{ll}
{}&{x \cos \omega~+~y \sin \omega}
&{}={}& {p}
&{} \\

{\Rightarrow}&{\frac{(\sqrt{3} + 1)x}{2 \sqrt{2}}~+~\frac{(\sqrt{3} - 1)y}{2 \sqrt{2}}}
&{}={}& {4}
&{} \\

{\Rightarrow}&{(\sqrt{3} + 1)x~+~(\sqrt{3} - 1)y}
&{}={}& {8\sqrt{2}}
&{} \\

\end{array}$

5. The actual plot is shown in fig.10.31 below:

Fig.10.31


(i) The red line is the line for which we determined the equation.
(ii) Note the magenta dashed arc. It is drawn with center as O.
• This arc passes through:
    ♦ The point of intersection of the cyan and red lines.
    ♦ The point (0,4)
• So it is clear that, the length of the cyan line is four units.

Solved example 10.13
The Fahrenheit temperature F and absolute temperature K satisfy a linear relation. Given that K = 273 when F = 32 and that K = 373 when F = 212. Express K in terms of F and find the value of F, when K = 0
Solution:
1. Given that: Fahrenheit temperature F and absolute temperature K satisfy a linear relation.
That means, if we plot the relation between F and K on a graph paper, the plot will be a straight line.
2. Also given that:
    ♦ K = 273 when F = 32
        ✰ This is just like: when x = 32, y is 273
    ♦ K = 373 when F = 212.
        ✰ This is just like: when x = 212, y is 373
• So we have two points on the straight line: (32, 273) and (212, 373).
3. It is important to keep in mind that, the points are in the form (F, K).
• That means,
    ♦ F is plotted along the x-axis.
    ♦ K is plotted along the y-axis.
4. We have two points on the line. So we can use the two point form:
$y-y_1~=~\frac{y_2 - y_1}{x_2 - x_1}(x-x_1)$
• For our present problem, we can modify this as:
$K-K_1~=~\frac{K_2 - K_1}{F_2 - F_1}(F-F_1)$
• Substituting the known values, we get:

$\begin{array}{ll}
{}&{K-K_1}
&{}={}& {\frac{K_2 - K_1}{F_2 - F_1}(F-F_1)}
&{} \\

{\Rightarrow}&{K-273}
&{}={}& {\frac{373 - 273}{212 - 32}(F-32)}
&{} \\

{\Rightarrow}&{K-273}
&{}={}& {\frac{100}{180}(F-32)}
&{} \\

{\Rightarrow}&{K-273}
&{}={}& {\frac{5}{9}(F-32)}
&{} \\

{\Rightarrow}&{9K-2457}
&{}={}& {5F-160}
&{} \\

{\Rightarrow}&{9K}
&{}={}& {5F+2297}
&{} \\

{\Rightarrow}&{K}
&{}={}& {\frac{5F}{9}+\frac{2297}{9}}
&{} \\

\end{array}$

• Thus we get a relation between K and F.
5. We want the value of F when K = 0
For that, we put K = 0 in the above relation. We get:

$\begin{array}{ll}
{}&{K}
&{}={}& {\frac{5F}{9}+\frac{2297}{9}}
&{} \\

{\Rightarrow}&{0}
&{}={}& {\frac{5F}{9}+\frac{2297}{9}}
&{} \\

{\Rightarrow}&{\frac{5F}{9}}
&{}={}& {-\frac{2297}{9}}
&{} \\

{\Rightarrow}&{5F}
&{}={}& {-2297}
&{} \\

{\Rightarrow}&{F}
&{}={}& {-459.4}
&{} \\

\end{array}$

6. The actual plot is shown in fig.10.32 below:

Fig.10.32

• Points A and B represent the given data.
• Point C represent the value of F when K is zero.


The link to a few more solved examples is given below:

Exercise 10.2


In the next section, we will see General equation of a line.

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Thursday, December 15, 2022

Chapter 10.5 - Intercept Form

In the previous section, we saw some of the different forms of the equation of a line. In this section, we will see intercept form.

Intercept form

• Suppose that, we are given the following two items:
   ♦ x-intercept of a line.
   ♦ y-intercept of that line.
• Then we can quickly write the equation of that line. Let us see how it is done.

Case I
This can be written in 4 steps:
1. Let the x-intercept be 'a'.
• Then the point of intersection of the line with the x-axis will be (a,0).
    ♦ This is shown in fig.10.26(a) below:

Derivation of the intercept form of the equation of a line in analytic geometry.
Fig.10.26

2. Let the y-intercept be 'b'.
• Then the point of intersection of the line with the y-axis will be (0,b)
3. Now we have two points on the line. They are: (a,0) and (0,b).
• So we can use the two-point form: $y-y_1~=~\frac{y_2-y_1}{x_2-x_1} (x-x_1)$
• Substituting the known values, we get:
$\begin{array}{ll}
{}&{y-0}
&{}={}& {\frac{b-0}{0-a} (x-a)}
&{} \\

{\Rightarrow}&{y-0}
&{}={}& {\frac{-b}{a} (x-a)}
&{} \\

{\Rightarrow}&{ya}
&{}={}& {-bx+ab}
&{} \\

{\Rightarrow}&{\frac{y}{b}}
&{}={}& {\frac{-x}{a}~+~1}
&{\color{green}{\text{- - - (a)}}} \\

{\Rightarrow}&{\frac{x}{a} + \frac{y}{b}}
&{}={}& {1}
&{} \\

\end{array}$

◼ Remarks:
• Line marked as (a):
In this line, we divide both sides by ab
4. So we get an equation: $\frac{x}{a} + \frac{y}{b} = 1$
 

Case II
This can be written in 4 steps:
1. In case I, we derived an equation based on fig.10.26(a) above.
• In this fig.,
    ♦ the line intersects the x-axis at the +ve side.
    ♦ the line intersects the y-axis also at the +ve side.
2. What if
    ♦ the line intersect the x-axis at the -ve side.
    ♦ the line intersect the y-axis at the +ve side.
• Such a situation is shown in fig.10.26(b) above.
3. But this situation should not discourage us. Because, we have the two points where the line cuts the x-axis and y-axis. The points are (-a,0) and (0,b).
• Using the two-point form as before, we get:
$\begin{array}{ll}
{}&{y-0}
&{}={}& {\frac{b-0}{0-~-a} (x-~-a)}
&{} \\

{\Rightarrow}&{y-0}
&{}={}& {\frac{b}{a} (x+a)}
&{} \\

{\Rightarrow}&{ya}
&{}={}& {bx+ab}
&{} \\

{\Rightarrow}&{\frac{y}{b}}
&{}={}& {\frac{x}{a}~+~1}
&{} \\

{\Rightarrow}&{\frac{-x}{a} + \frac{y}{b}}
&{}={}& {1}
&{} \\

{\Rightarrow}&{\frac{x}{-a} + \frac{y}{b}}
&{}={}& {1}
&{} \\

\end{array}$

4. This is similar to the equation that we derived in case I. The 'a' has become '-a' because, the x-intercept in this case is -ve.

Case III
This can be written in 2 steps:
1. A third possible situation is shown in fig.10.27(a) below:

Fig.10.27

• Here the points are: (a,0) and (0,-b). Proceeding as before, we get:

$\begin{array}{ll}
{}&{y-0}
&{}={}& {\frac{-b-0}{0-a} (x-a)}
&{} \\

{\Rightarrow}&{y-0}
&{}={}& {\frac{-b}{-a} (x-a)}
&{} \\

{\Rightarrow}&{y-0}
&{}={}& {\frac{b}{a} (x-a)}
&{} \\

{\Rightarrow}&{ya}
&{}={}& {bx-ab}
&{} \\

{\Rightarrow}&{\frac{y}{b}}
&{}={}& {\frac{x}{a}~-~1}
&{} \\

{\Rightarrow}&{\frac{x}{a} - \frac{y}{b}}
&{}={}& {1}
&{} \\

{\Rightarrow}&{\frac{x}{a} + \frac{y}{-b}}
&{}={}& {1}
&{} \\

\end{array}$

2. This is similar to the equation that we derived in case I. The 'b' has become '-b' because, the y-intercept in this case is -ve.  

Case IV
This can be written in 2 steps:
1. The fourth and last possible situation is shown in fig.10.27(b) above.

• Here the points are: (-a,0) and (0,-b). Proceeding as before, we get:

$\begin{array}{ll}
{}&{y-0}
&{}={}& {\frac{-b-0}{0-~-a} (x-~-a)}
&{} \\

{\Rightarrow}&{y-0}
&{}={}& {\frac{-b}{a} (x+a)}
&{} \\

{\Rightarrow}&{ya}
&{}={}& {-bx-ab}
&{} \\

{\Rightarrow}&{\frac{y}{b}}
&{}={}& {\frac{-x}{a}~-~1}
&{} \\

{\Rightarrow}&{\frac{x}{a} + \frac{y}{b}}
&{}={}& {-1}
&{} \\

{\Rightarrow}&{\frac{x}{-a} + \frac{y}{-b}}
&{}={}& {1}
&{} \\

\end{array}$

2. This is similar to the equation that we derived in case I.
    ♦ The 'a' has become '-a' because, the x-intercept in this case is -ve. 
    ♦ The 'b' has become '-b' because, the y-intercept in this case is -ve. 


Based on the four cases, we can write:
• In the intercept form, we can use the general equation: $\frac{x}{a} + \frac{y}{b} = 1$
• But care must be taken regarding the signs of 'a' and 'b'.
(This equation is easy to remember because, x is divided by the x-intercept. Similarly, y is divided by the y-intercept)


• Fig.10.28 below shows the actual plot of four lines.
1. Equation of the red line L1 is: $\frac{x}{-3} + \frac{y}{4} = 1$
• We see that:
    ♦ L1 cuts the x-axis at (-3,0) 
    ♦ L1 cuts the y-axis at (0,4)
Fig.10.28
 
2. Equation of the green line L2 is: $\frac{x}{-6} + \frac{y}{-4} = 1$
• We see that:
    ♦ L2 cuts the x-axis at (-6,0) 
    ♦ L2 cuts the y-axis at (0,-4)
3. Equation of the magenta line L3 is: $\frac{x}{3} + \frac{y}{5} = 1$
• We see that:
    ♦ L3 cuts the x-axis at (3,0) 
    ♦ L3 cuts the y-axis at (0,5)      
4. Equation of the pink line L4 is: $\frac{x}{6} + \frac{y}{-3} = 1$
• We see that:
    ♦ L4 cuts the x-axis at (6,0) 
    ♦ L4 cuts the y-axis at (0,-3)

In the next section, we will see normal form.

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Tuesday, December 13, 2022

Chapter 10.4 - Various Forms of Equations of A Line

In the previous section, we saw collinearity of three points. In this section, we will see the various forms of the equation of a line.

Some basics can be written in 3 steps:
1. Consider a line L lying in the xy-plane.
• We know that in any line, there will be infinite number of points.
• But there are other infinite points which do not lie on the line.
2. Then what is the difference between the following two types of points:
(i) Points which lie on L
(ii) Points which do not lie on L  
• The answer is:
   ♦ All points lying on L, will satisfy a particular condition.
   ♦ The points which do not lie on L, will not satisfy that condition.
3. We can write this is another way also:
Take any point on the xy-plane. If that point satisfies a particular condition, then that point will lie on L.


• So our next aim is to find the conditions for different types of lines.
• First we will see horizontal lines.

Equation of a horizontal line

This can be written in 9 steps.
1. The red line L1 in fig.10.16(a) is parallel to the x-axis.
   ♦ It is a horizontal line.
   ♦ It is at a distance of ‘a’ from the x-axis.

Fig.10.16

2. Consider any point on L1. The ordinate (y-coordinate) of that point will be 'a'.
• Conversely, any point whose ordinate is a, will lie on L1
3. So we can write:
The condition for a point to lie on L1 is that, the ordinate of that point must be ‘a’
4. In algebraic form, we can write: y = a
• This algebraic form is the equation of line L1
• We can write:
Equation of L1 is: y = a
5. Now consider the red line L1' in fig.10.16(b) above.
   ♦ It is parallel to the x-axis
   ♦ It is a horizontal line.
   ♦ It is at a distance of ‘a’ from the x-axis.
6. Consider any point on L1'. The ordinate (y-coordinate) of that point will be '-a'.
• Conversely, any point whose ordinate is -a, will lie on L1'
7. So we can write:
The condition for a point to lie on L1' is that, the ordinate of that point must be ‘-a’
8. In algebraic form, we can write: y = -a
• This algebraic form is the equation of line L1'
• We can write:
Equation of L1' is: y = -a
9. In general, we can write:
Equation of any horizontal line will be in the form: $y=\pm a$
   ♦ Where ‘a’ is a constant.
         ✰ We use the ‘+’ sign when the horizontal line is above the x-axis.
         ✰ We use the ‘-’ sign when the horizontal line is below the x-axis.

Equation of a vertical line

This can be written in 9 steps.
1. The red line L2 in fig.10.17(a) is parallel to the y-axis.
   ♦ It is a vertical line.
   ♦ It is at a distance of ‘b’ from the y-axis.

Equation of a vertical line in analytic geometry.
Fig.10.17

2. Consider any point on L2. The abscissa (x-coordinate) of that point will be 'b'.
• Conversely, any point whose abscissa is 'b', will lie on L2
3. So we can write:
The condition for a point to lie on L2 is that, the abscissa of that point must be ‘b’
4. In algebraic form, we can write: x = b
• This algebraic form is the equation of line L2
• We can write:
Equation of L2 is: x = b
5. Now consider the red line L2' in fig.10.17(b) above.
   ♦ It is parallel to the y-axis
   ♦ It is a vertical line.
   ♦ It is at a distance of ‘b’ from the y-axis.
6. Consider any point on L2'. The abscissa (x-coordinate) of that point will be '-b'.
• Conversely, any point whose abscissa is -b, will lie on L2'
7. So we can write:
The condition for a point to lie on L2' is that, the abscissa of that point must be ‘-b’
8. In algebraic form, we can write: x = -b
• This algebraic form is the equation of line L2'
• We can write:
Equation of L2' is: x = -b
9. In general, we can write:
Equation of any vertical line will be in the form: $x=\pm b$
   ♦ Where ‘b’ is a constant.
         ✰ We use the ‘+’ sign when the vertical line is on the right side of the y-axis.
         ✰ We use the ‘-’ sign when the vertical line is on the left side of the y-axis.

Solved Example 10.8
Write the equation of the line parallel to x-axis and passing through (-2,3). Also write the equation of the line parallel to y-axis and passing through the same point.
Solution:
1. First we will consider the line parallel to the x-axis.
• It's equation will be of the form $y = \pm a$
• This line passes through (-2,3). So it's distance from the x-axis is 3 units.
   ♦ That means, a = 3
• Also, (-2,3) is above the x-axis.
   ♦ So we use the +ve sign
• So the required equation is: $y = 3$
2. Next we will consider the line parallel to the y-axis.
• It's equation will be of the form $x = \pm b$
• This line passes through (-2,3). So it's distance from the y-axis is 2 units.
   ♦ That means, a = 2
• Also, (-2,3) is on the left side of the y-axis.
   ♦ So we use the -ve sign
• So the required equation is: $x = -2$
3. The actual lines are shown in the fig.10.18 below:

Fig.10.18

• In the above fig,
   ♦ The red line is the required line parallel to the x-axis.
   ♦ The green line is the required line parallel to the y-axis.


Point-slope form

• Suppose that, we are given the following two items:
   ♦ Slope of a line.
   ♦ A point through which the line passes.
• Then we can quickly write the equation of that line. Let us see how it is done. It can be written in 7 steps:
1. Let the slope of the line be m
2. Let the line pass through a known point P0 (x0,y0)
• By saying "Known point", we mean that, the values of x0 and y0 are known.
3. Let P(x,y) be any point on the line.
4. Now we have two points on the line. They are: P0(x0,y0) and P(x,y). This is shown in fig.10.19 below:

Derivation of the slope-point form of a line in coordinate geometry.
Fig.10.19

5. If we have two points on a line, we can write the slope of the line.
• So in our present case, the slope will be $\frac{y-y_0}{x-x_0}$
6. But we are already given the slope. It is m. So we can write:

$\begin{array}{ll}
{}&{m}
&{}={}& {\frac{y-y_0}{x-x_0}}
&{} \\

{\Rightarrow}&{y-y_0}
&{}={}& {m(x-x_0)}
&{} \\
\end{array}$

7. So we get an equation: y-y0 = m(x-x0)
• We derived this equation by assuming that, the point (x,y) lies on the line (see fig.10.19).
• That means,
   ♦ if we take any point outside the line, this equation will not be satisfied.
   ♦ if we take any point on the line, this equation will be satisfied.
• So we can say that, y-y0 = m(x-x0) is the equation of the line.
   ♦ This is the equation of a line written in slope-point form.
         ✰ The slope is m.
         ✰ The point is (x0,y0).


Let us see a solved example:
Solved example 10.9
Three lines L1, L2 and L3 pass through the point (-3,4). Write the equation of each of those lines, if their slopes are -3, 2 and 4 respectively. 
Solution:
• Given that,
   ♦ (x0,y0) = (-3,4)
   ♦ m1 = -3
   ♦ m2 = 2
   ♦ m3 = 4
• We have the slope-point form: y-y0 = m(x-x0)
1. So for L1, the equation will be:
$\begin{array}{ll}
{}&{y-4}
&{}={}& {-3(x-~-3)}
&{} \\

{\Rightarrow}&{y-4}
&{}={}& {-3x-9}
&{} \\

{\Rightarrow}&{3x + y +5}
&{}={}& {0}
&{} \\
\end{array}$

2. Similarly for L2, the equation will be:
$\begin{array}{ll}
{}&{y-4}
&{}={}& {2(x-~-3)}
&{} \\

{\Rightarrow}&{y-4}
&{}={}& {2x+6}
&{} \\

{\Rightarrow}&{2x - y +10}
&{}={}& {0}
&{} \\
\end{array}$

3. Finally for L3, the equation will be:
$\begin{array}{ll}
{}&{y-4}
&{}={}& {4(x-~-3)}
&{} \\

{\Rightarrow}&{y-4}
&{}={}& {4x+12}
&{} \\

{\Rightarrow}&{4x - y +16}
&{}={}& {0}
&{} \\
\end{array}$

4. The actual plot of the three lines are shown in fig.10.20 below:

Fig.10.20

5. We can infer some general information from the plot. They can be written in 3 steps:
(i) If the slope of a line is +ve, that line will have an upward slope. That means, when we move along the x-axis towards the +ve side, the line will be sloping upwards.
   ♦ Lines L2 and L3 are examples.
(ii) If the slope of a line is -ve, that line will have a downward slope. That means, when we move along the x-axis towards the +ve side, the line will be sloping downwards.
   ♦ Line L1 is an example.
(iii) Compare the slopes of two lines.
   ♦ The line with the greater slope will be steeper.
   ♦ The line with the lesser slope will be flatter.
• This will become clear when we compare L2 and L3.


Two-point form

• Suppose that, we are given two known points on a line.
• Then we can quickly write the equation of that line. Let us see how it is done. It can be written in 6 steps:
1. Let the line pass through two known points P1 (x1,y1) and P2 (x2,y2)
• By saying "Known points", we mean that, the values of x1, y1, x2 and y2 are known.
2. Let P(x,y) be any point on the line.
3. Now we have three points on the line. They are: P1(x1,y1), P2(x2,y2) and P(x,y). This is shown in fig.10.21 below:


Fig.10.21

4. If there are three points, we can write slopes.
• So in our present case,
   ♦ the slope of line P1P will be $\frac{y-y_1}{x-x_1}$
   ♦ the slope of line P1P2 will be $\frac{y_2-y_1}{x_2-x_1}$
5. But since the three points are collinear, the slopes will be equal. So we can write:

$\begin{array}{ll}
{}&{\frac{y-y_1}{x-x_1}}
&{}={}& {\frac{y_2-y_1}{x_2-x_1}}
&{} \\

{\Rightarrow}&{y-y_1}
&{}={}& {\frac{y_2-y_1}{x_2-x_1} (x-x_0)}
&{} \\
\end{array}$

6. So we get an equation: $y-y_1~=~\frac{y_2-y_1}{x_2-x_1} (x-x_1)$
• We derived this equation by assuming that, the point (x,y) lies on the line (see fig.10.21).
• That means,
   ♦ if we take any point outside the line, this equation will not be satisfied.
   ♦ if we take any point on the line, this equation will be satisfied.
• So we can say that, $y-y_1~=~\frac{y_2-y_1}{x_2-x_1} (x-x_1)$ is the equation of the line.
   ♦ This is the equation of a line written in two-point form.
         ✰ The two points are: (x1,y1) and (x2,y2).


Let us see a solved example:
Solved example 10.10
Write the equations of the following lines:
(i) Line L1, passing through (-1, -3) and (2, 4). 
(ii) Line L2, passing through (-3, 7) and (6, 7). 
Solution:
Part (i):
• We have the two-point form: $y-y_1~=~\frac{y_2-y_1}{x_2-x_1} (x-x_1)$
• Substituting the known values, we get:
$\begin{array}{ll}
{}&{y-~-3}
&{}={}& {\frac{4-~-3}{2-~-1} (x-~-1)}
&{} \\

{\Rightarrow}&{y+3}
&{}={}& {\frac{7}{3} (x+1)}
&{} \\

{\Rightarrow}&{3y+9}
&{}={}& {7x+7}
&{} \\

{\Rightarrow}&{7x-3y-2}
&{}={}& {0}
&{} \\

\end{array}$

Part (ii):
• We have the two-point form: $y-y_1~=~\frac{y_2-y_1}{x_2-x_1} (x-x_1)$
• Substituting the known values, we get:
$\begin{array}{ll}
{}&{y-7}
&{}={}& {\frac{7-7}{6-~-3} (x-~-3)}
&{} \\

{\Rightarrow}&{y-7}
&{}={}& {\frac{0}{9} (x+3)}
&{} \\

{\Rightarrow}&{y-7}
&{}={}& {0}
&{} \\

{\Rightarrow}&{y}
&{}={}& {7}
&{} \\

\end{array}$

• The actual plots are shown in fig.10.22 below:

Fig.10.22

• Note:
In the case of L2, we see that, it is horizontal. Indeed we obtained the slope $\frac{y_2 - y_1}{x_2 - x_1}$ = 0 for L2


Slope-intercept form

• Let us first see, what intercept is. It can be written in 6 steps:
1. In fig.10.23(a) below, the line L1 intersects the x-axis at (a,0)
• The distance of the ‘point of intersection’ from the origin O is ‘a’.
• We say that, the x-intercept of the line is +a.

Fig.10.23

2. In fig.10.23(b) above, the line L2 intersects the x-axis at (-b,0)
• The distance of the ‘point of intersection’ from the origin O is ‘b’
• We say that, the x-intercept of the line is -b.
3. In fig.10.24(a) below, the line L3 intersects the y-axis at (c,0)
• The distance of the ‘point of intersection’ from the origin O is ‘c’.
• We say that, the y-intercept of the line is +c.

Derivation of slope-intercept form of a line in coordinate geometry.
Fig.10.,24

4. In fig.10.24(b) above, the line L4 intersects the x-axis at (-d,0)
• The distance of the ‘point of intersection’ from the origin O is ‘d’
• We say that, the x-intercept of the line is -d.
5. So intercept is the distance of the point of intersection from O with the proper sign.
6. While writing intercepts, it is better to remember that:
• Any non-parallel line will intersect the x-axis.
   ♦ In some cases, the point of intersection will be on the right side of y-axis.
         ✰ Then the point of intersection will be of the type (a,0)
   ♦ In the remaining cases, the point of intersection will be on the left side of y-axis.
         ✰ Then the point of intersection will be of the type (-b,0)
• Any non-parallel line will intersect the y-axis.
   ♦ In some cases, the point of intersection will be above the x-axis.
         ✰ Then the point of intersection will be of the type (0,c)
   ♦ In the remaining cases, the point of intersection will be below the x-axis.
         ✰ Then the point of intersection will be of the type (0,-d)


• Suppose that, we are given the following two items:
   ♦ Slope of a line.
   ♦ x-intercept or y-intercept of the line.
• Then we can quickly write the equation of that line. Let us see how it is done.

Case I: The x-intercept is +ve.
This can be written in 4 steps:
1. Let the slope of the line be m
2. Let the x-intercept be +a
• Then we can say that, the line passes through (a,0). See fig.10.23(a) above.
3. Now we have two items:
   ♦ Slope of the line.
   ♦ A point through which the line passes.
4. So we can use the point-slope form: y-y0 = m(x-x0)
• Here, x0 is 'a' and y0 is 0
• Thus the equation becomes:
$\begin{array}{ll}
{}&{y-0}
&{}={}& {m(x-a)}
&{} \\

{\Rightarrow}&{y}
&{}={}& {m(x-a)}
&{} \\
\end{array}$

Case II: The x-intercept is -ve.
This can be written in 4 steps:
1. Let the slope of the line be m
2. Let the x-intercept be -b
• Then we can say that, the line passes through (-b,0). See fig.10.23(b) above.
3. Now we have two items:
   ♦ Slope of the line.
   ♦ A point through which the line passes.
4. So we can use the point-slope form: y-y0 = m(x-x0)
• Here, x0 is '-b' and y0 is 0
• Thus the equation becomes:
$\begin{array}{ll}
{}&{y-0}
&{}={}& {m(x- -b)}
&{} \\

{\Rightarrow}&{y}
&{}={}& {m(x+b)}
&{} \\
\end{array}$

• Based on cases I and II, we can write:
When the slope and x-intercept is given, we can use the general form: y = m(x-a)
    ♦ When the intercept is +ve, we give a +ve value for 'a'.
    ♦ When the intercept is -ve, we give a -ve value for 'a'.

Case III: The y-intercept is +ve.
This can be written in 4 steps:
1. Let the slope of the line be m
2. Let the y-intercept be +c
• Then we can say that, the line passes through (0,c). See fig.10.24(a) above.
3. Now we have two items:
   ♦ Slope of the line.
   ♦ A point through which the line passes.
4. So we can use the point-slope form: y-y0 = m(x-x0)
• Here, x0 is 0 and y0 is 'c'
• Thus the equation becomes:
$\begin{array}{ll}
{}&{y-c}
&{}={}& {m(x-0)}
&{} \\

{\Rightarrow}&{y-c}
&{}={}& {mx}
&{} \\

{\Rightarrow}&{y}
&{}={}& {mx + c}
&{} \\
\end{array}$

Case IV: The y-intercept is -ve.
This can be written in 4 steps:
1. Let the slope of the line be m
2. Let the y-intercept be -d
• Then we can say that, the line passes through (0,-d). See fig.10.24(b) above.
3. Now we have two items:
   ♦ Slope of the line.
   ♦ A point through which the line passes.
4. So we can use the point-slope form: y-y0 = m(x-x0)
• Here, x0 is 0 and y0 is '-d'
• Thus the equation becomes:
$\begin{array}{ll}
{}&{y-~-d}
&{}={}& {m(x-0)}
&{} \\

{\Rightarrow}&{y+d}
&{}={}& {mx}
&{} \\

{\Rightarrow}&{y}
&{}={}& {mx - d}
&{} \\
\end{array}$

• Based on cases III and IV, we can write:
When the slope and y-intercept is given, we can use the general form: y = mx+c
    ♦ When the intercept is +ve, we give a +ve value for 'c'.
    ♦ When the intercept is -ve, we give a -ve value for 'c'.


Let us see a solved example:
Solved example 10.11
Write the equations of the following lines:
(i) Line L1 for which tan 𝜃 = 1/3 and x-intercept is 4. 
(ii) Line L2 for which tan 𝜃 = 1/2 and y-intercept is -(11/2).
𝜃 is the inclination of the line. 
Solution:
Part (i):
• 𝜃 is the inclination of the line.  So tan 𝜃 will be the slope.
   ♦ So we can write: m = 1/3
• x-intercept is 4.
   ♦ We use the general equation: y = m(x-a)
   ♦ Here 'a' is 4.
• Substituting the known values, we get:
$\begin{array}{ll}
{}&{y}
&{}={}& {\frac{1}{3} (x-4)}
&{} \\

{\Rightarrow}&{3y}
&{}={}& {x-4}
&{} \\

{\Rightarrow}&{x-3y-4}
&{}={}& {0}
&{} \\

\end{array}$

Part (ii):
• 𝜃 is the inclination of the line.  So tan 𝜃 will be the slope.
   ♦ So we can write: m = 1/2
• y-intercept is -(11/2).
   ♦ We use the general equation: y = mx + c
   ♦ Here 'c' is -(11/2)
• Substituting the known values, we get:
$\begin{array}{ll}
{}&{y}
&{}={}& {\frac{1 x}{2} - \frac{11}{2}}
&{} \\

{\Rightarrow}&{2y}
&{}={}& {x-11}
&{} \\

{\Rightarrow}&{x-2y-11}
&{}={}& {0}
&{} \\

\end{array}$

• The actual plots are shown in fig.10.25 below:


Fig.10.25

• We can see that:
   ♦ L1 intersects the x-axis at (4,0)
   ♦ L2 intersects the x-axis at (0,-11/2)


In the next section, we will see intercept form and normal form.

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