Imagine trying to describe the position of an airplane flying in the sky. You can’t explain it using just length and breadth, like on a flat map, you also need height. This is exactly what three dimensional geometry does. It helps us locate a point in space using three coordinates, and that’s why it is introduced in Class 11 Introduction to Three Dimensional Geometry and further explored in detail in Three Dimensional Geometry Class 12 with advanced concepts, formulas, and applications. In this article, we will cover the basics, important formulas, solutions, and questions from both Class 11 and Class 12 Three Dimensional Geometry to help you prepare effectively in mathematics.
This Story also Contains
Three dimensional geometry is the one which defines the world. Three dimensional geometry is one of the fundamental topics in various domains like astronomy, engineering, architecture, and so on.
The position of a point in two-dimension (2D) is given by two numbers $P(x, y)$ but in three-dimension geometry, the position of a point $P$ is given by three numbers $P(x, y, z)$.
Three mutually perpendicular lines intersect at one point, the point $O(0, 0, 0)$ is known as the origin in the space. These three mutually perpendicular lines form three planes namely $XY, YZ, ZX$ called coordinate planes. The $x$ and $y$ axis make $X Y$ plane, $y, z$ axis make $Y Z$ plane, similarly, ${x}, z$ axis make $XZ$ plane. This three-plane divides space into eight regions called octants.
The sign of the coordinates of a point determines the octant in which the point lies. The following table shows the signs of the coordinates in eight octants.
Octant | 1st | 2nd | 3rd | 4th | 5th | 6th | 7th | 8th |
---|---|---|---|---|---|---|---|---|
X | + | - | - | + | + | - | - | + |
Y | + | + | - | - | + | + | - | - |
Z | + | + | + | + | - | - | - | - |
Direction Cosine(DC) gives the relation of a vector or a line in a three-dimensional space, with each of the three axes. The direction cosine is the cosine of the angle subtended by this line with the $x$-axis, $y$-axis, and $z$-axis respectively. Let $r$ be the position vector of a point $P(x, y, z)$. Then, the direction cosines of vector $r$ are the cosines of angles $α, β,$ and $γ$ (i.e. $\cos α, \cos β,$ and $\cos γ$) that the vector $r$ makes with the positive direction of $X, Y,$ and $Z$ -axes respectively. Direction cosines are usually denoted by $l, m,$ and $n$ respectively.
$\alpha, \beta, \gamma$ are the angles that a vector makes with positive $X$ -axis, $Y$ -axis, and $Z$ -axis respectively then $\cos \alpha, \cos \beta, \cos \gamma$ are known as direction cosines, generally denoted by $(l,m,n)$.
$
\begin{aligned}
& l=\cos \alpha, m=\cos \beta, n=\cos \gamma \\
& l^2+m^2+n^2=1 \\
& \cos ^2 \alpha+\cos ^2 \beta+\cos ^2 \gamma=1
\end{aligned}
$
Let $\mathrm{P}\left(\mathrm{x}_1, \mathrm{y}_1, \mathrm{z}_1\right)$ and $\mathrm{Q}\left(\mathrm{x}_2, \mathrm{y}_2, \mathrm{z}_2\right)$ be two points on the line L .
Let $1, \mathrm{~m}$, and n be the direction cosines of the line $P Q$, and let it make angles $\alpha, \beta$, and $y$ with the $x$-axis, $y$-axis, and $z$-axis respectively.
The direction cosines of the line segment joining the points $P$ and $Q$ are given by
$
\left(\frac{x_2-x_1}{P Q}, \frac{y_2-y_1}{P Q}, \frac{z_2-z_1}{P Q}\right)
$
i) $\sin ^2 \alpha+\sin ^2 \beta+\sin ^2 \gamma=2$
ii) If $\mathrm{OP}=\mathrm{r}$ then the co-ordinates of P will be ( $\mathrm{lr}, \mathrm{mr}, \mathrm{nr}$ )
iii) Direction cosines of the $X$ -axis are $(1,0,0)$
iv) Direction cosines of the $Y$ -axis are $(0,1,0)$
v) Direction cosines of the $Z$ -axis are $(0,0,1)$
Direction Ratios are any set of three numbers that are proportional to the Direction cosines. Direction cosines and Direction ratios are related to each other.
If $\mathrm{l}, \mathrm{m}, \mathrm{n}$ are DCs of a vector then $\lambda l, \lambda m, \lambda n$ are DRs of this vector, where $\lambda$ can take any real value.
DRs are also denoted as $\mathrm{a}, \mathrm{b}$, and c respectively.
A vector has only one set of DCs, but infinite sets of DRs.
Note:
The coordinates of a point equal Ir, mr, and nr, which are proportional to the direction cosines. Hence the coordinates of a point are also its DRs.
If $\vec{r}=a i+b \hat{j}+c \hat{k}$, then $a, b$ and $c$ are one of the direction ratios of the given vector. Also, if $a^2+b^2+c^2=1$, then $a, b$ and $c$ will be direction cosines of given vector.
(i) If $a, b,$ and $c$ are direction ratios then direction cosines will be
$
l=\frac{ \pm a}{\sqrt{a^2+b^2+c^2}}, m=\frac{ \pm b}{\sqrt{a^2+b^2+c^2}}, n=\frac{ \pm c}{\sqrt{a^2+b^2+c^2}}
$
(ii) Direction ratios of a line joining two given points
$A\left(x_1, y_1, z_1\right)$ and $B\left(x_2, y_2, z_2\right)$ is given by
$
\left(x_2-x_1, y_2-y_1, z_2-z_1\right)
$
(iii) If $r=a \hat{i}+b \hat{j}+c \hat{k}$ be a vector with direction cosines $\mathrm{I}, \mathrm{m}, \mathrm{n}$ then
$
l=\frac{a}{|r|}, m=\frac{b}{|r|}, n=\frac{c}{|r|}
$
If the point $R(x, y, z)$ divides the line joining the points $P\left(x_1, y_1, z_1\right)$ and $Q\left(x_2, y_2, z_2\right)$ internally in the ratio $m: n$, then the coordinate of $R(x, y, z)$ is given by :
$\mathrm{R}(\mathrm{x}, \mathrm{y} . \mathrm{z})=\left(\frac{m x_2+n x_1}{m+n}, \frac{m y_2+n y_1}{m+n}, \frac{m z_2+n z_1}{m+n}\right)$
If the point $R$ divides $P Q$ externally in the ratio $m$ : $n$, then its coordinates are obtained by replacing $n$ with $(-n)$, so that the coordinates of point $R$ will be
$\mathrm{R}(\mathrm{x}, \mathrm{y}, \mathrm{z})=\left(\frac{m x_2-n x_1}{m-n}, \frac{m y_2-n y_1}{m-n}, \frac{m z_2-n z_1}{m-n}\right)$
The equation of the straight line in 3D requires two points that are located in space. The point in three coordinates is expressed as ( $x, y, z)$.
Let $L$ be $a$ line in space passing through point $P\left(x_0, y_0, z_0\right)$. Let $\overrightarrow{\mathbf{b}}=a \hat{\mathbf{i}}+b \hat{\mathbf{j}}+c \hat{\mathbf{k}}$ be a vector parallel to $L$ . Then, for any point on line $\mathrm{Q}(\mathrm{x}, \mathrm{y}, \mathrm{z})$, we know that vector $P Q$ is parallel to vector $b$ . Thus, there is a scalar, $\lambda$, such that $\overrightarrow{P Q}=\lambda \overrightarrow{\mathbf{b}}$, which gives,
$
\begin{gathered}
\overrightarrow{P Q}=\lambda \tilde{\mathbf{b}} \\
\left(x-x_0\right) \hat{i}+\left(y-y_0\right) \hat{j}+\left(z-z_0\right) \hat{k}=\lambda(a \hat{i}+b \hat{j}+c \hat{k})
\end{gathered}
$
Using vector operations, we can rewrite,
$
\begin{aligned}
(x \hat{i}+y \hat{j}+z \hat{k})-\left(x_0 \hat{i}+y_0 \hat{j}+z_0 \hat{k}\right) & =\lambda(a \hat{i}+b \hat{j}+c \hat{k}) \\
(x \hat{i}+y \hat{j}+z \hat{k}) & =\left(x_0 \hat{i}+y_0 \hat{j}+z_0 \hat{k}\right)+\lambda(a \hat{i}+b \hat{j}+c \hat{k})
\end{aligned}
$
Setting $\overrightarrow{\mathbf{r}}=x \hat{i}+y \hat{j}+z \hat{k}$ and $\overrightarrow{\mathbf{r}}_0=x_0 \hat{i}+y_0 \hat{j}+z_0 \hat{k}$ we now have the vector equation of a line:
$
\overrightarrow{\mathbf{r}}=\overrightarrow{\mathbf{r}}_0+\lambda \overrightarrow{\mathbf{b}}
$
Equation of a line through a given point and parallel to a given vector in Cartesian Form
The Equation of a line through a given point and parallel to a given vector in Cartesian Form is $
\frac{x-x_0}{a}=\frac{y-y_0}{b}=\frac{z-z_0}{c}
$
We can also find parametric equations for the line segment $\overrightarrow{\mathbf{r}}=\overrightarrow{\mathbf{p}}+\lambda(\overrightarrow{\mathbf{q}}-\overrightarrow{\mathbf{p}})$.
As the position vector of point $\mathrm{R}(\mathrm{x}, \mathrm{y}, \mathrm{z})$ is $\overrightarrow{\mathbf{r}}=(x \hat{i}+y \hat{j}+z \hat{k})$.
The intersection of two straight lines forms an angle. For two intersecting lines, there are two types of angles between the lines, the acute angle and the obtuse angle. The angle between two lines generally gives the acute angle between the two lines.
Let the given lines be,
$
\begin{aligned}
& \overrightarrow{\mathbf{r}}=\overrightarrow{\mathbf{r}}_0+\lambda \overrightarrow{\mathbf{b}} \\
& \overrightarrow{\mathbf{r}}={\overrightarrow{\mathbf{r}^{\prime}}}_0+\lambda \overrightarrow{\mathbf{b}}^{\prime}
\end{aligned}
$
As equation (i) and equation (ii) are straight lines in the directions of $\overrightarrow{\mathbf{b}}$ and $\overrightarrow{\mathbf{b}}^{\prime}$, respectively.
Let $\theta$ be the angle between the vectors $\overrightarrow{\mathbf{b}}$ and $\overrightarrow{\mathbf{b}}^{\prime}$
Using the dot product,
$
\begin{aligned}
\overrightarrow{\mathbf{b}} \cdot \overrightarrow{\mathbf{b}}^{\prime} & =|\overrightarrow{\mathbf{b}}|\left|\overrightarrow{\mathbf{b}}^{\prime}\right| \cos \theta \\
\Rightarrow \quad \cos \theta & =\frac{\overrightarrow{\mathbf{b}} \cdot \overrightarrow{\mathbf{b}^{\prime}}}{|\overrightarrow{\mathbf{b}}|\left|\overrightarrow{\mathbf{b}^{\prime}}\right|}
\end{aligned}
$
The equation of a straight line in cartesian form is
$
\begin{aligned}
& \frac{x-x_1}{a_1}=\frac{y-y_1}{b_1}=\frac{z-z_1}{c_1} \\
& \frac{x-x_2}{a_2}=\frac{y-y_2}{b_2}=\frac{z-z_2}{c_2}
\end{aligned}
$
Then,
$
\overrightarrow{\mathbf{b}}=a_1 \hat{i}+b_1 \hat{j}+c_1 \hat{k} \quad \text { and } \quad \overrightarrow{\mathbf{b}}^{\prime}=a_2 \hat{i}+b_2 \hat{j}+c_2 \hat{k}
$
So that,
$
\overrightarrow{\mathbf{b}} \cdot \overrightarrow{\mathbf{b}}^{\prime}=a_1 a_2+b_1 b_2+c_1 c_2
$
$
\begin{aligned}
|\overrightarrow{\mathbf{b}}| & =\sqrt{a_1^2+b_1^2+c_1^2}, \quad \text { and } \quad\left|\overrightarrow{\mathbf{b}}^{\prime}\right|=\sqrt{a_2^2+b_2^2+c_2^2} \\
\cos \theta & =\frac{a_1 a_2+b_1 b_2+c_1 c_2}{\sqrt{a_1^2+b_1^2+c_1^2} \sqrt{a_2^2+b_2^2+c_2^2}}
\end{aligned}
$
If two lines having direction ratios $\mathrm{a}_1, \mathrm{~b}_1, \mathrm{c}_1$ and $\mathrm{a}_2, \mathrm{~b}_2, \mathrm{c}_2$ then the angle between them is given by
$
\cos \theta=\frac{a_1 a_2+b_1 b_2+c_1 c_2}{\sqrt{a_1^2+b_1^2+c_1^2} \sqrt{a_2^2+b_2^2+c_2^2}}
$
If two lines have direction ratios as $\mathrm{l}_1, \mathrm{~m}_1, \mathrm{n}_1$ and $\mathrm{l}_2, \mathrm{~m}_2, \mathrm{n}_2$ then the angle between them is given by$
\cos \theta=l_1 l_2+m_1 m_2+n_1 n_2
$
The shortest distance between two lines in three-dimensional space is the length of the perpendicular segment drawn from a point on one line to the other line.
Shortest Distance between two skew lines
When two lines are neither parallel nor intersecting at a point they are referred to as Skew Lines.
If $\vec{r}=\vec{a}+\lambda \vec{b}$ and $\vec{r}=\overrightarrow{a_1}+\mu \vec{b}$ are skew lines then the shortest distance between them is given by
$
\left|\frac{\left(\vec{b} \times \overrightarrow{b_1}\right) \cdot\left(\vec{a}-\overrightarrow{a_1}\right)}{\left|\vec{b} \times \overrightarrow{b_1}\right|}\right|
$
The shortest distance between intersecting lines is $0$.
$\left(\vec{b} \times \overrightarrow{b_1}\right) \cdot\left(\overrightarrow{\mathbf{r}}_0^{\prime}-\overrightarrow{\mathbf{r}}_0\right)=0$
If the direction vectors of two lines are parallel and the two lines never meet they are referred as Parallel Lines.
If $\vec{r}=\overrightarrow{p_1}+\lambda \vec{\nu}$ and $\vec{r}=\overrightarrow{p_2}+\mu \vec{\nu}$ are Parallel Lines then the shortest distance between them is given by $
\frac{\left|\left(\overrightarrow{p_2}-\overrightarrow{p_1}\right) \times \vec{\nu}\right|}{|\vec{\nu}|}
$
We know that a line is determined by two points. In other words, for any two distinct points, there is exactly one line that passes through those points, whether in two dimensions or three. Similarly, given any three points that do not all lie on the same line, there is a unique plane that passes through these points. Just as a line is determined by two points, a plane is determined by three.
This may be the simplest way to characterize a plane, but we can use other descriptions as well. For example, given two distinct, intersecting lines, there is exactly one plane containing both lines. A plane is also determined by a line and any point that does not lie on the line.
The equation of a plane in a cartesian coordinate system can be computed through different methods based on the available input values about the plane.
The vector equation of a plane normal to unit vector $\hat{\mathbf{n}}$ and at a distance d from the origin is $\overrightarrow{\mathbf{r}} \cdot \hat{\mathbf{n}}=d$.
If $\mathrm{P}(\mathrm{x}, \mathrm{y}, \mathrm{z})$ is any point in the plane and $\hat{\mathbf{n}}$ is the unit vector normal to the plane.
Let $\mathrm{l}, \mathrm{m}, \mathrm{n}$ be the direction cosines. Then Cartesian equation of the plane in the normal form is given by
$\begin{array}{r}(x \hat{i}+y \hat{j}+z \hat{k}) \cdot({l} \hat{i}+m \hat{j}+n \hat{k})=d \\ \mathbf{l x}+\mathbf{m y}+\mathbf{n z}=\mathbf{d}\end{array}$
Let $\overrightarrow{\mathbf{n}}=a \hat{\mathbf{i}}+b \hat{\mathbf{j}}+c \hat{\mathbf{k}}$ be a vector and $\mathrm{P}\left(\mathrm{x}_0, \mathrm{y}_0, \mathrm{z}_0\right)$ be a point. Then the set of all points $Q(\mathrm{x}, \mathrm{y}, \mathrm{z})$ such that $\overrightarrow{P Q}$ orthogonal to $\overrightarrow{\mathbf{n}}$ forms a plane.
We say that $\overrightarrow{\mathbf{n}}$ is a normal vector, or perpendicular to the plane.
Remember, the dot product of orthogonal vectors is zero. This fact generates the vector equation of a plane:
$\overrightarrow{\mathbf{n}} \cdot \overrightarrow{P Q}=0$
If the position vector of point $P$ is $\overrightarrow{\mathbf{P}}$ and the plosition vector of point $Q$ is $\overrightarrow{\mathbf{q}}$ , then
$(\overrightarrow{\mathbf{q}}-\overrightarrow{\mathbf{p}}) \cdot \overrightarrow{\mathbf{n}}=\mathbf{0} \quad($ As $\overrightarrow{P Q}=\overrightarrow{\mathbf{q}}-\overrightarrow{\mathbf{p}})$
This is the vector equation of the plane.
Position vector of point P and point Q is $\overrightarrow{\mathbf{p}}=x_0 \hat{i}+y_0 \hat{j}+z_0 \hat{k}$ and $\overrightarrow{\mathbf{q}}=x \hat{i}+y \hat{j}+z \hat{k}$ respectively and vector $\overrightarrow{\mathbf{n}}$ is $a \hat{i}+b \hat{j}+c \hat{k}$ Then,
$
\begin{array}{lc}
& (\overrightarrow{\mathbf{q}}-\overrightarrow{\mathbf{p}}) \cdot \overrightarrow{\mathbf{n}}=\mathbf{0} \\
\Rightarrow & \left((x \hat{i}+y \hat{j}+z \hat{k})-\left(x_0 \hat{i}+y_0 \hat{j}+z_0 \hat{k}\right)\right) \cdot(a \hat{i}+b \hat{j}+c \hat{k})=0 \\
\Rightarrow & {\left[\left(x-x_0\right) \hat{i}+\left(y-y_0\right) \hat{j}+\left(z-z_0\right) \hat{k}\right] \cdot(\mathrm{a} \hat{i}+\mathrm{b} \hat{j}+c \hat{k})=0} \\
\text { i.e. } & \mathbf{a}\left(x-x_0\right)+\mathbf{b}\left(y-y_0\right)+\mathbf{c}\left(z-z_0\right)=\mathbf{0}
\end{array}
$
Thus, the coefficients of $x, y,$ and $z$ in the cartesian equation of a plane are the direction ratios of the normal to the plane.
Let $\mathrm{A}, \mathrm{B}$, and C be three non-collinear points on the plane with position vectors $\overrightarrow{\mathbf{a}}, \overrightarrow{\mathbf{b}}$ and $\overrightarrow{\mathbf{c}}$ respectively.
The vectors, $\overrightarrow{A B}=\overrightarrow{\mathbf{b}}-\overrightarrow{\mathbf{a}}$ and $\overrightarrow{A C}=\overrightarrow{\mathbf{c}}-\overrightarrow{\mathbf{a}}$ are in the given plane. Therefore, the vector $\overrightarrow{A B} \times \overrightarrow{A C}$ is perpendicular to the plane containing points $A, B$, and $C$.
Let $P$ be any point in the plane with a position vector $\overrightarrow{\mathbf{r}}$
Therefore, the equation of the plane passing through $OP$ and perpendicular to the vector $\overrightarrow{A B} \times \overrightarrow{A C}$ is
$
\begin{aligned}
(\vec{r}-\vec{a}) \cdot(\overrightarrow{\mathrm{AB}} \times \overrightarrow{\mathrm{AC}}) & =0 \\
\text { or } \quad(\tilde{\mathbf{r}}-\tilde{\mathbf{a}}) \cdot[(\tilde{\mathbf{b}}-\tilde{\mathbf{a}}) \times(\tilde{\mathbf{c}}-\tilde{\mathbf{a}})] & =0
\end{aligned} \quad(\because \overrightarrow{A R}=(\vec{r}-\vec{a}))
$
This is the equation of the plane in vector form passing through three non-collinear points.
Let $\left(x_1, y_1, z_1\right),\left(x_2, y_2, z_2\right)$ and $\left(x_3, y_3, z_3\right)$ be the coordinates of points $A$ , $B$ and $C$ respectively.
Let $P(x, y, z)$ be any point on the plane.
Then, the vectors $\overrightarrow{P A}, \overrightarrow{B A}$ and $\overrightarrow{C A}$ are coplanar.
which is required equation of the plane.
$
\begin{aligned}
& {\left[\begin{array}{lll}
\overrightarrow{\mathrm{PA}} & \overrightarrow{\mathrm{BA}} & \overrightarrow{\mathrm{CA}}
\end{array}\right]=0} \\
& \left|\begin{array}{ccc}
\mathrm{x}-\mathrm{x}_1 & \mathrm{y}-\mathrm{y}_1 & \mathrm{z}-\mathrm{z}_1 \\
\mathrm{x}_2-\mathrm{x}_1 & \mathrm{y}_2-\mathrm{y}_1 & \mathrm{z}_2-\mathrm{z}_1 \\
\mathrm{x}_3-\mathrm{x}_1 & \mathrm{y}_3-\mathrm{y}_1 & \mathrm{z}_3-\mathrm{z}_1
\end{array}\right|=0
\end{aligned}
$
which is required equation of the plane.
The equation of a plane having intercepting lengths $a, b$, and $c$ with $X$-axis, $Y$-axis, and $Z$-axis, respectively is
$
\frac{\mathrm{x}}{\mathrm{a}}+\frac{\mathrm{y}}{\mathrm{b}}+\frac{\mathrm{z}}{\mathrm{c}}=1
$
Let a plane pass through point A with a position vector $\overrightarrow{\mathbf{a}}$ and parallel to two vectors $\overrightarrow{\mathbf{b}}$ and $\overrightarrow{\mathbf{c}}$.
Let $\overrightarrow{\mathbf{r}}$ be the position vector of any point $P$ on the plane.
$
\overrightarrow{A P}=\overrightarrow{O P}-\overrightarrow{O A}=\vec{r}-\vec{a}
$
Since $AP$ lies in the plane, hence, $\overrightarrow{\mathbf{r}}-\overrightarrow{\mathbf{a}}, \overrightarrow{\mathbf{b}}$ and $\overrightarrow{\mathbf{c}}$ are coplanar.
We have,
$
\begin{aligned}
(\overrightarrow{\mathbf{r}}-\overrightarrow{\mathbf{a}}) \cdot(\vec{b} \times \overrightarrow{\mathbf{c}}) & =0 \\
(\overrightarrow{\mathbf{r}}) \cdot(\vec{b} \times \overrightarrow{\mathbf{c}}) & =(\overrightarrow{\mathbf{a}}) \cdot(\overrightarrow{\mathbf{b}} \times \overrightarrow{\mathbf{c}}) \\
{\left[\begin{array}{lll}
\overrightarrow{\mathbf{r}} & \vec{b} & \overrightarrow{\mathbf{c}}
\end{array}\right] } & =\left[\begin{array}{lll}
\overrightarrow{\mathbf{a}} & \vec{b} & \overrightarrow{\mathbf{c}}
\end{array}\right]
\end{aligned}
$
Which is the required equation of plane.
$
\begin{aligned}
& \text { From }(\overrightarrow{\mathbf{r}}-\overrightarrow{\mathbf{a}}) \cdot(\overrightarrow{\mathbf{b}} \times \overrightarrow{\mathbf{c}})=0 \text { we have, }[\overrightarrow{\mathbf{r}}-\overrightarrow{\mathbf{a}} \overrightarrow{\mathbf{b } } \overrightarrow{\mathbf{c}}] \\
& \Rightarrow \quad\left|\begin{array}{ccc}
x-x_1 & y-y_1 & z-z_1 \\
x_2 & y_2 & z_2 \\
x_3 & y_3 & z_3
\end{array}\right|=0
\end{aligned}
$
Which is the required equation of a plane in the cartesian form where
$
\overrightarrow{\mathbf{b}}=x_2 \hat{\mathbf{i}}+y_2 \hat{\mathbf{j}}+z_2 \hat{\mathbf{k}} \text { and } \overrightarrow{\mathbf{c}}=x_3 \hat{\mathbf{i}}+y_3 \hat{\mathbf{j}}+z_3 \hat{\mathbf{k}}
$
The angle between two planes is defined as the angle between the normals of the two planes. It is also called dihedral angles.
Equation of the Angle Between Two Planes in Vector Form
Let $\theta$ be the angle between two planes $\overrightarrow{\mathbf{r}} \cdot \overrightarrow{\mathbf{n}}_1=\mathbf{d}_1$ and $\overrightarrow{\mathbf{r}} \cdot \overrightarrow{\mathbf{n}}_2=\mathbf{d}_2$ then,
$
\cos \theta=\frac{\overrightarrow{\mathbf{n}}_1 \cdot \overrightarrow{\mathbf{n}}_2}{\left|\overrightarrow{\mathbf{n}}_1\right|\left|\overrightarrow{\mathbf{n}}_1\right|}
$
Let $\theta$ be the angle between the planes, $a_1 x+b_1 y+c_1 z+d_1=0$ and $a_2 x+$ $b_2 y+c_2 z+d_2=0$
Then,
$
\cos \theta=\left|\frac{a_1 a_2+b_1 b_2+c_1 c_2}{\sqrt{a_1^2+b_1^2+c_1^2} \sqrt{a_2^2+b_2^2+c_2^2}}\right|
$
The direction ratios of the normal to the planes are $a_1, b_1, c_1$, and $a_2, b_2$ $\mathrm{c}_2$ respectively.
Concept | Formula |
---|---|
Distance between two points $P(x_1, y_1, z_1)$ and $Q(x_2, y_2, z_2)$ | $d = \sqrt{(x_2 - x_1)^2 + (y_2 - y_1)^2 + (z_2 - z_1)^2}$ |
Section formula (internal division, ratio $m:n$) | $P\left(\dfrac{mx_2 + nx_1}{m+n}, \dfrac{my_2 + ny_1}{m+n}, \dfrac{mz_2 + nz_1}{m+n}\right)$ |
Section formula (external division, ratio $m:n$) | $P\left(\dfrac{mx_2 - nx_1}{m-n}, \dfrac{my_2 - ny_1}{m-n}, \dfrac{mz_2 - nz_1}{m-n}\right)$ |
Midpoint formula | $M\left(\dfrac{x_1 + x_2}{2}, \dfrac{y_1 + y_2}{2}, \dfrac{z_1 + z_2}{2}\right)$ |
Direction cosines $(l, m, n)$ of vector $(a, b, c)$ | $l = \dfrac{a}{\sqrt{a^2+b^2+c^2}}, ; m = \dfrac{b}{\sqrt{a^2+b^2+c^2}}, ; n = \dfrac{c}{\sqrt{a^2+b^2+c^2}}$ |
Relation between direction cosines | $l^2 + m^2 + n^2 = 1$ |
Angle between two lines with direction cosines $(l_1,m_1,n_1)$ and $(l_2,m_2,n_2)$ | $\cos \theta = l_1l_2 + m_1m_2 + n_1n_2$ |
Equation of a line (vector form) | $\vec{r} = \vec{a} + \lambda \vec{b}$ |
Equation of a line (cartesian/parametric form) | $\dfrac{x - x_1}{a} = \dfrac{y - y_1}{b} = \dfrac{z - z_1}{c}$ |
Equation of a plane (vector form) | $\vec{r} \cdot \vec{n} = d$ |
Equation of a plane (cartesian form) | $ax + by + cz + d = 0$ |
Normal form of a plane | $x\cos\alpha + y\cos\beta + z\cos\gamma = p$ |
Distance of a point $P(x_1, y_1, z_1)$ from a plane $ax+by+cz+d=0$ | $D = \dfrac{|ax_1 + by_1 + cz_1 + d|}{\sqrt{a^2 + b^2 + c^2}}$ |
Angle between two planes $a_1x+b_1y+c_1z+d_1=0$ and $a_2x+b_2y+c_2z+d_2=0$ | $\cos \theta = \dfrac{a_1a_2 + b_1b_2 + c_1c_2}{\sqrt{a_1^2+b_1^2+c_1^2},\sqrt{a_2^2+b_2^2+c_2^2}}$ |
Angle between a line (direction ratios $l,m,n$) and a plane $ax+by+cz+d=0$ | $\sin \theta = \dfrac{|al + bm + cn|}{\sqrt{a^2+b^2+c^2} \, \sqrt{l^2+m^2+n^2}}$ |
Equation of a sphere (center $(x_1,y_1,z_1)$, radius $r$) | $(x-x_1)^2 + (y-y_1)^2 + (z-z_1)^2 = r^2$ |
General equation of a sphere | $x^2 + y^2 + z^2 + 2ux + 2vy + 2wz + d = 0$ |
Equation of a cone (vertex at origin, axis $z$-axis, semi-vertical angle $\alpha$) | $x^2 + y^2 = z^2 \tan^2 \alpha$ |
Equation of a cylinder (axis $z$-axis, radius $a$) | $x^2 + y^2 = a^2$ |
Shortest distance between two skew lines $\vec{r} = \vec{a_1} + \lambda \vec{b_1}$, $\vec{r} = \vec{a_2} + \mu \vec{b_2}$ | $d = \dfrac{|(\vec{a_2} - \vec{a_1}) \cdot (\vec{b_1} \times \vec{b_2})|}{|\vec{b_1} \times \vec{b_2}|}$ |
This section highlights all the important topics of Three Dimensional Geometry as per the Class 12 NCERT and JEE Main syllabus, ensuring complete coverage for board and entrance exams.
Here you’ll find the most recommended books and study materials that explain concepts clearly and provide ample practice for mastering 3D Geometry.
Book Title | Author / Publisher | Description |
---|---|---|
NCERT Mathematics Class 12 | NCERT | Official textbook covering all concepts of 3D Geometry thoroughly. |
Mathematics for Class 12 | R.D. Sharma | Detailed theory and solved problems on Three Dimensional Geometry. |
Objective Mathematics | R.S. Aggarwal | Topic-wise MCQs and practice questions aimed at board and competitive exams. |
Arihant All-In-One Mathematics | Arihant | Comprehensive theory and practice problems covering 3D geometry. |
Plane Trigonometry and Solid Geometry | S.L. Loney | Well-known classic book with exhaustive problems on 3D geometry. |
NCERT textbooks are the primary resource for building a strong foundation in Three Dimensional Geometry, with notes, step-by-step explanations and solved exercise and exemplar questions.
NCERT Maths Notes for Class 12th Chapter 11 - Three Dimensional Geometry
NCERT Maths Solutions for Class 12th Chapter 11 - Three Dimensional Geometry
NCERT Maths Exemplar Solutions for Class 12th Chapter 11 - Three Dimensional Geometry
This part focuses on subject-specific NCERT resources like exemplar problems, solutions, and notes, so as to help students build their understanding in the concept.
Subject | NCERT Notes Link | NCERT Solutions Link | NCERT Exemplar Link |
---|---|---|---|
Mathematics | NCERT notes Class 12 Maths | NCERT solutions for Class 12 Mathematics | NCERT exemplar Class 12 Maths |
Physics | NCERT notes Class 12 Physics | NCERT solutions for Class 12 Physics | NCERT exemplar Class 12 Physics |
Chemistry | NCERT notes Class 12 Chemistry | NCERT solutions for Class 12 Chemistry | NCERT exemplar Class 12 Chemistry |
This section provides a collection of practice questions to test your understanding, improve accuracy, and prepare effectively for board exams and JEE Main.
Frequently Asked Questions (FAQs)
Three Dimensional Geometry is the branch of mathematics that deals with the position of points, lines, and planes in 3D space using three coordinates. It extends coordinate geometry from a flat plane (2D) into real-world space.
In JEE Main, 3D Geometry is a scoring topic because the questions are usually formula-based and less time-consuming compared to calculus. Mastering formulas for distance, angles, and equations of lines/planes can fetch quick marks.
The angle between two planes is the same as the angle between their normal vectors. If the planes are $a_1x+b_1y+c_1z+d_1=0$ and $a_2x+b_2y+c_2z+d_2=0$, then $\cos \theta = \frac{a_1a_2+b_1b_2+c_1c_2}{\sqrt{a_1^2+b_1^2+c_1^2}\sqrt{a_2^2+b_2^2+c_2^2}}$
The direction cosine formula is $
l=\frac{ \pm a}{\sqrt{a^2+b^2+c^2}}, m=\frac{ \pm b}{\sqrt{a^2+b^2+c^2}}, n=\frac{ \pm c}{\sqrt{a^2+b^2+c^2}}
$
Any three points that do not all lie on the same line, there is a unique plane that passes through these points. Just as a line is determined by two points, a plane is determined by three.