In the previous section, we saw how slope, intercepts, π and p can be obtained from the general equation of a line. We saw that, Β± sign is present for p, cos π and sin π. In this section, we will see how to apply those signs.
β’ We know that, sign of sin π, cos π etc., will depend upon the position of the angle π.
β’ For example:
β¦ If π is in the I quadrant, sin π will be +ve, cos π will be +ve.
β¦ If π is in the III quadrant, sin π will be -ve, cos π will be +ve.
β’ There is an easy method to find the position of π. It involves the use of the flow chart in fig.10.34 below. It can be written in 5 steps:
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Fig.10.34 |
1. We are given the equation of a line in the form Ax +By +C = 0.
β’ We want to find the signs of sin π, cos π and p.
β’ The first step is to calculate the slope using the equation: m=βAB
β’ 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.
β’ 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.
β’ The second step is to calculate the x-intercept βaβ using the equation: a=βCA
3. If βaβ is +ve, then we move along the left arrow.
β’ The y-intercept βbβ will be -ve.
β’ 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 βaβ is +ve. Then the y-intercept will be -ve.
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Fig.10.35 |
β’ Then sin will be -ve and cos will be +ve
β’ 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.
β’ The second step is to calculate the x-intercept βaβ using the equation: a=βCA
2. If βaβ is -ve, then we move along the right arrow.
β’ The y-intercept βbβ will be -ve.
β’
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 βaβ is -ve. Then the
y-intercept will be -ve.
3. From the fig.c, it is clear that, if βaβ is -ve and βbβ is -ve, then the normal p will lie in the III quadrant.
β’ Then sin will be -ve and cos will be -ve
β’ 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:
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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 π.
Solution:
1. From the given equation, we get:
A = 3, B = 2 and C = 6
2. Calculation of p
p=Β±CβA2 + B2=Β±6β32 + 22=Β±6β13
2. Calculation of cos π
cosΟ=Β±AβA2 + B2=Β±3β32 + 22=Β±3β13
3. Calculation of sin π
sinΟ=Β±BβA2 + B2=Β±2β32 + 22=Β±2β13
4. Now we determine the signs:
(i) Slope of the line = m=βAB = β32
β’ This is -ve. So we move along the right arrow of the chart in fig.13.36
(ii) x-intercept of the line = a=βCA = β63 = β2
β’ This is -ve. So sin π is -ve and cos π is -ve.
5. So we can write:
sinΟ=β2β13cosΟ=β3β13
6. The sign of p will be always +ve because, it is a distance.
7. Now we can write the normal form:
xcosΟ + ysinΟ=pβxΓβ3β13 + yΓβ2β13=6β13ββ3xβ13 + β2yβ13=6β13β3xβ13 + 2yβ13=β6β13
8. Calculation of π:
(i) From (5), we have: tan π = 2/3
β’ Using a scientific calculator, we get: π = 33.69o
(ii) But in our present case, π is in the third quadrant (both sin and cos are -ve).
β’ So we find the other value of π using the identity: tan x = tan (180 + x)
β’ We get: tan π = tan 33.69 = tan (180 + 33.69) = tan 213.69
(iii) So the value of π is 213.69o
9. So the normal form can be written as:
x cos 213.69o + y sin 213.69o = 6β13
β’ The actual plot is shown below:
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Fig.10.37 |
β’ 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=βAB = β3β4 = 34
3. x-intercept can be calculated as:
a=βCA = β103
4. y-intercept can be calculated as:
b=βCB = β10β4 = 52
Solved example 10.14
Reduce the equation (β3)x + y - 8 = 0 into normal form. Find the values of p and π.
Solution:
1. From the given equation, we get:
A = β3, B = 1 and C = -8
2. Calculation of p
p=Β±CβA2 + B2=Β±β8β(β3)2 + 12=Β±8β4=Β±4
2. Calculation of cos π
cosΟ=Β±AβA2 + B2=Β±β3β(β3)2 + 12=Β±β3β4=Β±β32
3. Calculation of sin π
sinΟ=Β±BβA2 + B2=Β±1β(β3)2 + 12=Β±1β4=Β±12
4. Now we determine the signs:
(i) Slope of the line = m=βAB = ββ31 = ββ3
β’ This is -ve. So we move along the right arrow of the chart in fig.13.36
(ii) x-intercept of the line = a=βCA = ββ8β3 = 8β3
β’ This is +ve. So sin π is +ve and cos π is +ve.
5. So we can write:
sinΟ=12cosΟ=β32
6. The sign of p will be always +ve because, it is a distance.
7. Now we can write the normal form:
xcosΟ + ysinΟ=pβxΓβ32 + yΓ12=4ββ3x2 + y2=4
8. Calculation of π:
(i) From (5), we have: tanΟ = 1β3
β’ We know that tan30 = 1β3
(ii) In our present case, π is in the first quadrant (both sin and cos are +ve).
β’ So 30o is the correct value of π
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 - (β3)x - 5 = 0 and (β3)y - x + 6 = 0
Solution:
1. The first line given is: y - (β3)x - 5 = 0
β’ Rearranging this into the general form, we get: (β3)x - y + 5 = 0
β’ So we can write:
A = β3, B = -1 and C = 5
β’ Thus we get: m1=βAB = ββ3β1 = β3
2. The second line given is: (β3)y - x + 6 = 0
β’ Rearranging this into the general form, we get: x - (β3)y - 6 = 0
β’ So we can write:
A = 1, B = -β3 and C = -6
β’ Thus we get: m2=βAB = β1ββ3 = 1β3
3. We have two slopes and we are asked to find the angle between the lines
β¦ So this problem belongs to case I.
β’ We have seen the details about case I and case II here.
β’ Since this problem belongs to case I, there is no need to interchange the slopes and explore the two possibilities.
β’ We have the equation: tanΞΈ = m2 β m11 + m1m2
β’
Substituting the known values, we get:
tanΞΈ=1β3 β β31 + β3Γ1β3βtanΞΈ=1 β 3β3 + β3βtanΞΈ=β22β3βtanΞΈ=β1β3
4. So we have to solve the equation: tan π = β1β3
It can be solved in 5 steps:
(i) Given that, tan ΞΈ = β1β3
(ii) We know that, tan 30 = 1β3
β’ Using the identities 9.d and 9.c, we have: tan (180 β ΞΈ) = - tan ΞΈ
(See the list of identities here)
β’ So we can write: tan (180 β 30) = -tan 30
β’ That means: tan 150 = -tan 30
(iii) But tan 30 = 1β3
β’ So the result in (ii) becomes:
tan 150 = -tan 30 = β1β3
(iv) We are given that, tan ΞΈ = β1β3
β’ Including this in (iii), we get:
tan 150 = -tan 30 = β1β3 = tan ΞΈ
β’ Picking the first and last items , we get:
tan 150 = tan ΞΈ
(v) So the first principal solution is: ΞΈ = 150o
5. We need only one principal solution. It indicates that, one of the angls between the two given lines is 150o.
β’ 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 β 0 are: (i) Parallel if a1b1 = a2b2 and (ii) Perpendicular if a1a2 + b1b2 = 0
Solution:
1. The first line given is: a1x + b1 y + c1 = 0
β’ So we can write:
A = a1, B = b1 and C = c1
β’ Thus we get: m1=βAB = βa1b1
2. The second line given is: a2x + b2 y + c2 = 0
β’ So we can write:
A = a2, B = b2 and C = c2
β’ Thus we get: m2=βAB = βa2b2
3. If the two lines are parallel, then the two slopes will be equal.
β’ In such a situation, we get:
m1=m2ββa1b1=βa2b2βa1b1=a2b2
4. If the two lines are perpendicular, then m1 will be the -ve reciprocal of m2.
β’ In such a situation, we get:
m1=β1m2ββa1b1=β1βa2b2ββa1b1=1a2b2ββa1b1=b2a2ββa1a2=b1b2βa1a2 + b1b2=0
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
β’ So we can write:
A = 1, B = -2 and C = 5
β’ Thus we get: m=βAB = β1β2 = 12
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)
y β β2=β2(x β 1)βy + 2=β2x + 2β2x + y=0
In the next section, we will see distance of a point from a line.
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