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Question: If \(l,m,n\) are direction cosines of a straight line then prove that \({l^2} + {m^2} + {n^2} = 1\)....

If l,m,nl,m,n are direction cosines of a straight line then prove that l2+m2+n2=1{l^2} + {m^2} + {n^2} = 1.

Explanation

Solution

Find the dimensions of the lines joining the x,yx,y and zz axes, to use it further into the equation formed by solving the equations of direction cosines using the distance formula. We use simple coordinates to represent the values of the given angles and the points.

Complete step-by-step solution:

Let OO be the origin and OPOP be a line Which has the direction cosines as l,m,nl,m,n.
Let the coordinates of PP be (x,y,z)(x,y,z).
Let the length of the line OPOP be rr.
The coordinates of origin O=(0,0,0)O = (0,0,0).
Using the three- coordinates distance formula:
OP=(x0)2+(y0)2+(z0)2OP = \sqrt {{{(x - 0)}^2} + {{(y - 0)}^2} + {{(z - 0)}^2}}
OP=x2+y2+z2\Rightarrow OP = \sqrt {{x^2} + {y^2} + {z^2}}
Squaring on both sides of the equation, we get:
OP2=x2+y2+z2O{P^2} = {x^2} + {y^2} + {z^2}
Now, OP=rOP = r
Substituting OP=rOP = r in the above equation
r2=x2+y2+z2(1){r^2} = {x^2} + {y^2} + {z^2} - - - - \left( 1 \right)
PA,PB,PCPA,PB,PC are joined perpendicularly on the coordinate axes such that:
OA=xOA = x, OB=yOB = y, OC=zOC = z
The angles between the following lines with the origin are as follows:
POA=α\angle POA = \alpha , POB=β\angle POB = \beta , POC=γ\angle POC = \gamma
Now,
Given direction cosines are l,m,nl,m,n.
cosα=l\cos \alpha = l, cosβ=m\cos \beta = m, cosγ=n\cos \gamma = n
Let us consider the AOP\vartriangle AOP,
cosα=xr\cos \alpha = \dfrac{x}{r}
By using cosα=l\cos \alpha = l we get,
l=xr\Rightarrow l = \dfrac{x}{r}
Hence,
x=lr\Rightarrow x = lr
Squaring on both sides:
x2=l2r2(2){x^2} = {l^2}{r^2} - - - - \left( 2 \right)
Similarly,
cosβ=yr\cos \beta = \dfrac{y}{r}
By using cosβ=m\cos \beta = m we get,
m=yr\Rightarrow m = \dfrac{y}{r}
Hence,
y=mr\Rightarrow y = mr
Squaring on both sides:
y2=m2r2(3){y^2} = {m^2}{r^2} - - - - \left( 3 \right)
And,
cosγ=zr\cos \gamma = \dfrac{z}{r}
By using cosγ=n\cos \gamma = n we get,
n=zr\Rightarrow n = \dfrac{z}{r}
Hence,
z=nr\Rightarrow z = nr
Squaring on both sides:
z2=n2r2(4){z^2} = {n^2}{r^2} - - - - \left( 4 \right)
 x=lr\therefore {\text{ }}x = lr, y=mry = mr, z=nrz = nr
Adding 2, 3, 42,{\text{ }}3,{\text{ }}4, we get:
x2+y2+z2=l2r2+m2r2+n2r2{x^2} + {y^2} + {z^2} = {l^2}{r^2} + {m^2}{r^2} + {n^2}{r^2}
Taking out the common terms
x2+y2+z2=(l2+m2+n2)r2\Rightarrow {x^2} + {y^2} + {z^2} = ({l^2} + {m^2} + {n^2}){r^2}
From equation 11:
r2=(l2+m2+n2)r2\Rightarrow {r^2} = ({l^2} + {m^2} + {n^2}){r^2}
Cancelling the common terms on both the sides, that is diving both the sides using r2{r^2}
l2+m2+n2=1{l^2} + {m^2} + {n^2} = 1
Hence proved

Note: In analytic geometry, the direction cosines (or directional cosines) of a vector are the cosines of the angles between the vector and the three coordinate axes. Equivalently, they are the contributions of each component of the basis to a unit vector in that direction. Direction cosines are an analogous extension of the usual notion of slope to higher dimensions.