Definitions [11]
The angle between two skew lines is the angle between two intersecting lines drawn from any point parallel to each of the given lines.
If a line joins A(x1,y1,z1) and B(x2,y2,z2), then the direction ratios are: \[(x_2-x_1,y_2-y_1,z_2-z_1)\]
A straight line in space is uniquely determined if
- It passes through a given point and has a given direction;
- It passes through two given points.
Coplanar:
Two straight lines are coplanar if they are either parallel or intersecting.
Skew Lines:
Two straight lines (in space) which are neither parallel nor intersecting are called skew lines.
Line of shortest distance:
Let l1,l2 be two skew lines, then there is one and only one line (say l3) which is perpendicular to both 11 and l2. The line l3 is known as the line of shortest distance.
Shortest distance (S.D.):
Let the line of shortest distance l3 meet the given skew lines 11 and l2 in points P and Q, respectively. Then \[\mid PQ\mid\] is the shortest distance between 11 and l2.
If (l1,m1,n1) and (l2,m2,n2) are the direction cosines of two lines, then the angle θ between them is given by
\[\cos\theta=l_{1}l_{2}+m_{1}m_{2}+n_{1}n_{2}=\Sigma l_{1}l_{2}\]
Angle in Terms of Direction Ratios:
If the direction ratios of two lines are proportional to
(a1,b1,c1) and (a2,b2,c2) then:
\[\cos\theta=\frac{a_1a_2+b_1b_2+c_1c_2}{\sqrt{a_1^2+b_1^2+c_1^2}\sqrt{a_2^2+b_2^2+c_2^2}}\]
If a, b, c are three numbers proportional to the actual direction cosines l, m, n of a line, then the numbers a, b, c are called direction ratios (d.r.s.) of the line.
If a straight line passes through two points whose position vectors are \[\vec{a}\] and \[\vec{b}\], then the vector equation of the line is:
\[\vec{r}=\vec{a}+\lambda(\vec{b}-\vec{a})\]
or
\[\vec{r}=(1-\lambda)\vec{a}+\lambda\vec{b}\]
If a line passes through a point whose position vector is \[\vec{a}\] and is parallel to a given vector \[\vec{b}\], then its vector equation is:
\[\vec{r}=\vec{a}+\lambda\vec{b}\]
Where λ is a scalar parameter.
Line Through the Origin:
\[\vec{r}=\lambda\vec{b}\]
A plane is a surface such that if two points are taken in it, the straight line joining them lies wholly in the surface.
General Equation of a Plane:
\[ax+by+cz+d=0\]
Plane Passing Through the Origin:
\[ax+by+cz=0\]
- Definition: Direction cosines are the cosines of the angles a line makes with the X, Y, Z axes.
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Notation: l = cosα, m = cosβ, n = cosγ
-
\[l^2+m^2+n^2=1\]
Formulae [20]
Vector form:
If planes are: \[\vec{r}\cdot\vec{n}_1=q_1,\quad\vec{r}\cdot\vec{n}_2=q_2\] then:
\[\cos\theta=\frac{\vec{n}_1\cdot\vec{n}_2}{|\vec{n}_1||\vec{n}_2|}\]
Cartesian Form:
\[\cos\theta=\frac{a_1a_2+b_1b_2+c_1c_2}{\sqrt{a_1^2+b_1^2+c_1^2}\sqrt{a_2^2+b_2^2+c_2^2}}\]
- Distance between P(x₁, y₁, z₁) and Q(x₂, y₂, z₂):
-
Distance of point (x, y, z) from origin
\[OP=\sqrt{x^2+y^2+z^2}\]
For points A(x₁, y₁, z₁) and B(x₂, y₂, z₂) divided in ratio m₁ : m₂
(a) Internal Division
\[\left(\frac{m_1x_2+m_2x_1}{m_1+m_2},\frac{m_1y_2+m_2y_1}{m_1+m_2},\frac{m_1z_2+m_2z_1}{m_1+m_2}\right)\]
(b) External Division
\[\left(\frac{m_1x_2-m_2x_1}{m_1-m_2},\frac{m_1y_2-m_2y_1}{m_1-m_2},\frac{m_1z_2-m_2z_1}{m_1-m_2}\right)\]
(c) Mid-Point Formula
\[\left(\frac{x_1+x_2}{2},\frac{y_1+y_2}{2},\frac{z_1+z_2}{2}\right)\]
\[l=\frac{a}{\sqrt{a^2+b^2+c^2}},\quad m=\frac{b}{\sqrt{a^2+b^2+c^2}},\quad n=\frac{c}{\sqrt{a^2+b^2+c^2}}\]
\[\sin\theta=\frac{\sqrt{\left(a_1b_2-a_2b_1\right)^2+\left(b_1c_2-b_2c_1\right)^2+\left(c_1a_2-c_2a_1\right)^2}}{\sqrt{\Sigma a_1^2}\sqrt{\Sigma a_2^2}}\]
\[\cos\theta=\pm\frac{a_{1}a_{2}+b_{1}b_{2}+c_{1}c_{2}}{\sqrt{\Sigma a_{1}^{2}}\sqrt{\Sigma a_{2}^{2}}}\]
\[\tan\theta=\frac{\sqrt{\Sigma\left(a_{1}b_{2}-a_{2}b_{1}\right)^{2}}}{\Sigma a_{1}a_{2}}\]
If
-
p = length of the perpendicular from the origin to the plane
-
(l,m,n) = direction cosines of the normal to the plane
Then the equation of the plane is:
\[lx+my+nz=p\]
Vector form:
\[\frac{|\vec{a}\cdot\vec{n}-d|}{|\vec{n}|}\]
Cartesian form:
\[\frac{|ax_1+by_1+cz_1+d|}{\sqrt{a^2+b^2+c^2}}\]
\[\frac{x}{a}+\frac{y}{b}+\frac{z}{c}=1\]
S.D. between lines \[\begin{array}
{rcl}\vec{r} & = & a_1+\lambda\vec{b_1} & \mathrm{and} & \vec{r}=a_2+\mu\vec{b_2} & \mathrm{is}
\end{array}\]
\[\frac{\left(\overrightarrow{a}_{2}-\overrightarrow{a}_{1}\right)\cdot\left(\overrightarrow{b}_{1}\times\overrightarrow{b}_{2}\right)}{\left|\overrightarrow{b}_{1}\times\overrightarrow{b}_{2}\right|}=\frac{\left|\overrightarrow{a}_{2}-\overrightarrow{a}_{1},\overrightarrow{b}_{1},\overrightarrow{b}_{2}\right|}{\left|\overrightarrow{b}_{1}\times\overrightarrow{b}_{2}\right|}.\]
If the lines are: \[l_1:\vec{r}=\vec{a}_1+\lambda\vec{b}\] and \[l_2:\vec{r}=\vec{a}_2+\lambda\vec{b}\]
Then the shortest distance between them is:
\[\mathrm{S.D.}=\frac{|\vec{b}\times(\vec{a}_2-\vec{a}_1)|}{|\vec{b}|}\]
If the plane passes through (x1,y1,z1) (x2,y2,z2),(x3,y3,z3), then its equation is:
\[\begin{vmatrix}
x-x_1 & y-y_1 & z-z_1 \\
x_2-x_1 & y_2-y_1 & z_2-z_1 \\
x_3-x_1 & y_3-y_1 & z_3-z_1
\end{vmatrix}=0\]
\[\frac{x-x_1}{x_2-x_1}=\frac{y-y_1}{y_2-y_1}=\frac{z-z_1}{z_2-z_1}\]
1. Cartesian → Vector Form
If the Cartesian equation of a line is:
\[\frac{x-x_1}{a}=\frac{y-y_1}{b}=\frac{z-z_1}{c}\]
Then its vector form is:
\[\vec{r}=(x_1\hat{i}+y_1\hat{j}+z_1\hat{k})+\lambda(a\hat{i}+b\hat{j}+c\hat{k})\]
2. Vector → Cartesian Form
If the vector equation of a line is:
\[\vec{r}=\vec{a}+\lambda\vec{m}\]
Then the Cartesian form is:
\[\frac{x-x_1}{a}=\frac{y-y_1}{b}=\frac{z-z_1}{c}\]
1. Symmetric (Standard) Form of a Line
If a line passes through (x1,y1,z1) and has direction cosines (l,m,n) then its equation is:
\[\frac{x-x_{1}}{l}=\frac{y-y_{1}}{m}=\frac{z-z_{1}}{n}=r\]
2. Parametric Form (Coordinates of any Point)
\[x=x_1+lr,\quad y=y_1+mr, \quad z=z_1+nr\]
3. Line with Given Direction Ratios
\[\frac{x-x_1}{a}=\frac{y-y_1}{b}=\frac{z-z_1}{c}\]
Vector Form:
\[\cos\theta=\frac{\vec{b}_1\cdot\vec{b}_2}{|\vec{b}_1||\vec{b}_2|}\]
Cartesian form:
\[\cos\theta=\frac{a_1a_2+b_1b_2+c_1c_2}{\sqrt{a_1^2+b_1^2+c_1^2}\sqrt{a_2^2+b_2^2+c_2^2}}\]
Perpendicular condition:
\[a_1a_2+b_1b_2+c_1c_2=0\]
Parallel Condition:
\[\frac{a_1}{a_2}=\frac{b_1}{b_2}=\frac{c_1}{c_2}\]
If the plane passes through (x1,y1,z1) then:
\[a(x-x_1)+b(y-y_1)+c(z-z_1)=0\]
\[\vec{r}\cdot\hat{n}=p\]
If the plane passes through the origin:
\[\vec{r}\cdot\hat{n}=0\]
Corresponding Cartesian form:
\[lx+my+nz=p\]
Vector form:
\[(\vec{r}-\vec{a})\cdot\vec{n}=0\]
Cartesian form:
\[a(x-x_1)+b(y-y_1)+c(z-z_1)=0\]
Vector Form:
\[\sin\theta=\frac{\overrightarrow{b}.\overrightarrow{n}}{|\overrightarrow{b}|.|\overrightarrow{n}|}\]
Cartesian Form:
\[\sin\theta=\frac{al+bm+cn}{\sqrt{a^2+b^2+c^2}\sqrt{l^2+m^2+n^2}}\]
Vector form:
If the planes are: \[\vec{r}\cdot\vec{n}_1=d_1\quad\mathrm{and}\quad\vec{r}\cdot\vec{n}_2=d_2\]
Then the plane through their intersection is:
\[(\vec{r}\cdot\vec{n}_1-d_1)+\lambda(\vec{r}\cdot\vec{n}_2-d_2)=0\]
Key Points
-
XY-plane → z = 0
-
YZ-plane → x = 0
-
ZX-plane → y = 0
If the general equation of a plane is:
ax + by + cz + d = 0
Rewrite as:
ax + by + cz = −d
Then divide throughout by −d, to get:
\[\frac{x}{\frac{-d}{a}}+\frac{y}{\frac{-d}{b}}+\frac{z}{\frac{-d}{c}}=1\]
