Manipur Board 2025 Class 12 Syllabus: The syllabus is an integral part of every student’s life. The Council of Higher Secondary Education, Manipur (COHSEM) designs...
Manipur Board Class 12 Syllabus 2025: Subject-wise PDF Download
November 17, 2024Angle Between a Line and a Plane: The geometry which defines a position of a point in space by three numbers x, y and z is called three-dimensional coordinate geometry or analytical geometry. The angle between a line and a plane is the complement of the angle between the line and the normal plane.
Let us first define some key definitions like line, plane, normal to a plane and equation of a plane in different forms, which help us understand the concept angle between a line and a plane.
A surface is a plane if every point on the line joining any two arbitrary points on the surface lies on the surface. This is Euclid’s definition of a plane. The position of a plane in space can be determined in four ways.
Each of these methods can be used to find the position and hence, the equation of a plane in space.
A plane can be thought of as made of a point \(P\left( {{x_1},{y_1},{z_1}} \right)\) and all other points \(Q\) such that the segment \(PQ\) is perpendicular to a given direction \(a, b, c\) called the normal direction to the plane.
A first-degree equation in \(x, y, z\) represents a plane. The general equation of a plane is \(ax + by + cz + d = 0\)
where \(a, b\) and \(c\) are constants.
The general equation of a plane passing through a given point \(\left( {{x_1},{y_1},{z_1}} \right)\) is \(a\left( {x – {x_1}} \right) + b\left( {y – {y_1}} \right) + c\left( {z – {z_1}} \right) = 0\)
where \(a, b\) and \(c\) are constants.
Let us know about the equation of plane in normal form in the below table:
Type | Description | Equation |
Vector Form | \(\vec r \cdot \hat n = d\) | |
Cartesian Form | Let \(P(x, y, z)\) be any point on the plane | \(lx + my + nz = d\) where \(l, m,\) and \(n\) be the direction cosines of \(\hat n\). |
Note
If in the equation \(\overrightarrow r .\overrightarrow n = d,\,\overrightarrow n \) is not a unit vector, then we reduce the equation \(\vec r \cdot \vec n = d\) to normal form by dividing both sides by \(|\hat n|\), we get \(\frac{{\vec r \cdot \vec n}}{{|\hat n|}} = \frac{d}{{|\hat n|}}\)
Here is a tabular representation for deeper understanding:
Type | Description | Equation |
Vector Form | A plane passing through a point having the position vector \(\vec a\) and normal to vector \(\vec n\) | \((\vec r – \vec a)\vec n = 0\) |
Cartesian Form | \(\overrightarrow r = \left( {x\hat i + y\hat j + z\hat k} \right),\,\overrightarrow a = \left( {{x_1}\hat i + {y_1}\hat j + {z_1}\hat k} \right)\) and \(\vec n = (a\hat i + b\hat j + c\hat k)\), then \((\vec r – \vec a) = \left( {\left( {x – {x_1}} \right)\hat i + \left( {y – {y_1}} \right)\hat j + \left( {z – {z_1}} \right)\hat k} \right)\). | \(\left( {\left( {x – {x_1}} \right)\hat i + \left( {y – {y_1}} \right)\hat j + \left( {z – {z_1}} \right)\hat k} \right) \cdot (a\hat i + b\hat j + c\hat k) = 0\) \( \Rightarrow a\left( {x – {x_1}} \right) + b\left( {y – {y_1}} \right) + c\left( {z – {z_1}} \right) = 0\) |
Equation of plane passing with three given points can be described in the following manner:
Type | Description | Equation |
Vector Form | Three points \(A, B\) and \(C\) having position vectors \(a, b\) and \(c\), respectively. Let \(\vec r\) be the position vector of any point \(P\) in the plane. Hence, vector \(\overrightarrow {AP} = \vec r – \vec a,\overrightarrow {AB} = \vec b – \vec a\) and \(\overrightarrow {AC} = \vec c – \vec a\) are coplanar. | \(\left[ {\begin{array}{{20}{l}} {\vec r}&{\vec b}&{\vec c} \end{array}} \right] + \left[ {\begin{array}{{20}{l}} {\vec r}&{\vec a}&{\vec b} \end{array}} \right] + \left[ {\begin{array}{{20}{l}} {\vec r}&{\vec c}&{\vec a} \end{array}} \right] = \left[ {\begin{array}{{20}{l}} {\vec a}&{\vec b}&{\vec c} \end{array}} \right]\) |
Cartesian Form | Let the plane be passing through points \(A\left( {{x_1},{y_1},{z_1}} \right),B\left( {{x_2},{y_2},{z_2}} \right)\) and \(C\left( {{x_3},{y_3},{z_3}} \right)\). Let \(P(x,y,z)\) be any point on the plane. Then, vectors \(\overrightarrow {PA} ,\overrightarrow {BA} \) and \(\overrightarrow {CA} \) are coplanar. \( \Rightarrow [\overrightarrow {PA} \,\overrightarrow {BA} \,\overrightarrow {CA} ] = 0\) | \(\left| {x – {x_1}y – {y_1}z – {z_1}{x_2} – {x_1}{y_2} – {y_1}{z_2} – {z_1}{x_3} – {x_1}{y_3} – {y_1}{z_3} – {z_1}} \right| = 0\) |
Intercept Form | Intercepting lengths of the plane are \(a, b\) and \(c\) with \(x-\)axis, \(y-\)axis, and \(z-\)axis, respectively | \(\frac{x}{a} + \frac{y}{b} + \frac{z}{c} = 1\) |
The angle between a line and a plane is the complement of the angle between the line and the normal to the plane.
Let \(\alpha \) be the plane and \(L\) the line which is not parallel to \(\alpha \). Let the line \(L\) make an angle \(\theta \left( {0 < \theta < \frac{\pi }{2}} \right)\) with the plane \(\alpha \). Then \(\left( {\frac{\pi }{2} – \theta } \right)\) is the acute angle between the normal to the plane and the line \(L\).
Let the given line be \(\vec r = \vec a + \lambda \vec b\) and the given plane be \(\vec r \cdot \vec n = d\).
If \(\phi \) is the angle between the given line (parallel to \(\vec b\)) and the normal to the plane. So, \(\vec n \cdot \vec b = |\vec n||\vec b|\cos \phi = nb\cos \phi \)
If \(\theta \) is the angle between the line and plane, then \(\theta = \left( {\frac{\pi }{2} – \emptyset } \right) = \left( {\frac{\pi }{2} – \left( {\frac{{\vec n \cdot \vec b}}{{nb}}} \right)} \right) = \left( {\frac{{\vec n \cdot \vec b}}{{nb}}} \right)\).
Let the given line be \(\frac{{x – {x_1}}}{l} = \frac{{y – {y_1}}}{m} = \frac{{z – {z_1}}}{n}\) and the given plane be \(ax + by + cz + d = 0\).
The direction ratios of the line are \(l, m, n\). The equation of the plane is given to be \(ax + by + cz + d = 0\) so that the direction ratios of the normal to the plane are \(a, b, c\). Suppose that \(\theta \) be the angle between the line and the plane where \(\theta \) is an acute angle. Then \(\left( {\frac{\pi }{2} – \theta } \right)\) is the acute angle between the given line and the normal to the given plane.
Hence, \(\cos \left( {\frac{\pi }{2} – \theta } \right) = \frac{{|al + bm + cn|}}{{\sqrt {{l^2} + {m^2} + {n^2}} \sqrt {{a^2} + {b^2} + {c^2}} }}\)
\( \Rightarrow \sin \theta = \frac{{|al + bm + cn|}}{{\sqrt {{l^2} + {m^2} + {n^2}} \sqrt {{a^2} + {b^2} + {c^2}} }}\)
\( \Rightarrow \theta = \left[ {\frac{{|al + bm + cn|}}{{\sqrt {{l^2} + {m^2} + {n^2}} \sqrt {{a^2} + {b^2} + {c^2}} }}} \right]\) ; where \(\left( {0 < \theta < \frac{\pi }{2}} \right)\).
Which gives the required angle between the line and the plane.
The following are few conditions of parallelism and Perpendicularity:
If a line is parallel to the plane, then normal to the plane is perpendicular to the given line (i.e. \(\theta = 0\))
\( \Rightarrow al + bm + cn = 0\)
Also, since \(\left( {{x_1},{y_1},{z_1}} \right)\) does not lie in the plane \(ax + by + cz + d = 0\).
\(\therefore \,\,a{x_1} + b{y_1} + c{z_1} + d \ne 0\)
If a line is perpendicular to the plane (i.e. \(\theta = \frac{\pi }{2}\)) then the line is parallel to the normal to the plane. But the direction ratios of the line are \(l, m, n\) and the direction ratios of the normal to the plane are \(a, b, c\). Hence \(\frac{l}{a} = \frac{m}{b} = \frac{n}{c}\) is required conditions for perpendicular.
To find the point of intersection of the line \(\frac{{x – {x_1}}}{l} = \frac{{y – {y_1}}}{m} = \frac{{z – {z_1}}}{n}\) and the plane be \(ax + by + cz + d = 0\)
Let \(\frac{{x – {x_1}}}{l} = \frac{{y – {y_1}}}{m} = \frac{{z – {z_1}}}{n} = k\)
\( \Rightarrow x = {x_1} + lk,y = {y_1} + mk,z = {z_1} + nk\,\,\,\,\,…(1)\)
If the point \((x, y, z)\) lies on the plane \(ax + by + cz = d\), then \(a\left( {{x_1} + lk} \right) + b\left( {{y_1} + mk} \right) + c\left( {{z_1} + nk} \right) + d = 0\)
\( \Rightarrow k = \frac{{a{x_1} + b{y_1} + c{z_1} + d}}{{al + bm + cn}}\)
Putting the value of \(k\) in \((1)\) we get the coordinates of the point of intersection. Here we suppose that the line is not parallel to the plane so that \(al + bm + cn \ne 0\).
Here are a few solved examples that can give better insight:
Q.1. Find the angle between the line \(\vec r = (\hat i + 2\hat j – \hat k) + \lambda (\hat i – \hat j + \hat k)\) and the plane \(\vec r \cdot (2\hat i – \hat j + \hat k) = 4\).
Ans: We know that \(\theta \) is the angle between the line be \(\vec r = \vec a + \lambda \vec b\) and plane be \(\vec r \cdot \vec n = d\), then \(\sin \theta = \left| {\frac{{\vec n \cdot \vec b}}{{|n||b|}}} \right|\)
Therefore, if \(\theta \) is the angle between \(\vec r = (\hat i + 2\hat j – \hat k) + \lambda (\hat i – \hat j + \hat k)\) and \(\vec r.(2\hat i – \hat j+ \hat k) = 4\).
Here, \(\vec b = (\hat i – \hat j + \hat k)\), and \(\vec n = (2\hat i – \hat j + \hat k)\)
Then, \(\sin \theta = \frac{{(\hat i – \hat j + \hat k) \cdot (2\hat i – \hat j + \hat k)}}{{|\hat i – \hat j + \hat k||2\hat i – \hat j + \hat k|}} = \frac{{2 + 1 + 1}}{{\sqrt {1 + 1 + 1} \sqrt {4 + 1 + 1} }} = \frac{4}{{\sqrt 3 \sqrt 6 }} = \frac{4}{{3\sqrt 2 }}\)
\( \Rightarrow \theta = \frac{4}{{3\sqrt 2 }}\)
Hence, the angle between \(\vec r = (\hat i + 2\hat j – \hat k) + \lambda (\hat i – \hat j + \hat k)\) and \(\vec r \cdot (2\hat i – \hat j + \hat k) = 4\) is \(\frac{4}{{3\sqrt 2 }}\).
Q.2. Find the angle between the line \(\frac{{x + 1}}{2} = \frac{y}{3} = \frac{{z – 3}}{6}\) and the plane \(3x + y + z = 7\).
Ans: Let \(\theta \) be the angle between the line and the plane. Then \(\left( {\frac{\pi }{2} – \theta } \right)\) will be the angle between the line and the normal to the plane.
\(\cos \left( {\frac{\pi }{2} – \theta } \right) = \sin (\theta ) = \frac{{|al + bm + cn|}}{{\sqrt {{l^2} + {m^2} + {n^2}} \sqrt {{a^2} + {b^2} + {c^2}} }}\)
\(\sin (\theta ) = \frac{{2 \times 3 + 3 \times 1 + 6 \times 1}}{{\sqrt {{2^2} + {3^2} + {6^2}} \sqrt {{3^2} + {1^2} + {1^2}} }}\)
\(\sin (\theta ) = \frac{{6 + 3 + 6}}{{\sqrt {49} \sqrt {11} }} = \frac{{15}}{{7\sqrt {11} }}\)
Therefore, \(\theta = \frac{{15}}{{7\sqrt {11} }}\).
Q.3. Find the angle between the line \(\frac{{x + 2}}{3} = \frac{y}{4} = \frac{{z – 2}}{3}\) and the plane \(4x + 2y + 2z = 9\).
Ans: Let \(\theta \) be the angle between the line and the plane. Then \(\left( {\frac{\pi }{2} – \theta } \right)\) will be the angle between the line and the normal to the plane.
\(\cos \left( {\frac{\pi }{2} – \theta } \right) = \sin (\theta ) = \frac{{|al + bm + cn|}}{{\sqrt {{l^2} + {m^2} + {n^2}} \sqrt {{a^2} + {b^2} + {c^2}} }}\)
\(\sin (\theta ) = \frac{{3 \times 4 + 4 \times 2 + 3 \times 2}}{{\sqrt {{3^2} + {4^2} + {3^2}} \sqrt {{4^2} + {2^2} + {2^2}} }}\)
\(\sin (\theta ) = \frac{{12 + 8 + 6}}{{\sqrt {34} \sqrt {24} }} = \frac{{26}}{{4\sqrt {51} }} = \frac{{13}}{{2\sqrt {51} }}\)
Therefore, \(\theta = \frac{{13}}{{2\sqrt {51} }}\).
Q.4. Find the angle between the line \(\vec r = (2\hat i + \hat j – 3\hat k) + \lambda (2\hat i – 2\hat j + 3\hat k)\) and the plane \(\vec r \cdot (3\hat i – 2\hat j + 2\hat k) = 5\).
Ans: We know that \(\theta \) is the angle between the line be \(\overrightarrow r = \overrightarrow a + \lambda \overrightarrow b \) and plane be \(\vec r \cdot \vec n = d\), then \(\sin \theta = \left| {\frac{{\vec n \cdot \vec b}}{{|n||b|}}} \right|\)
Therefore, if \(\theta \) is the angle between the line \(\vec r = (2\hat i + \hat j – 3\hat k) + \lambda (2\hat i – 2\hat j + 3\hat k)\) and the plane \(\vec r \cdot (3\hat i – 2\hat j + 2\hat k) = 5\).
Here, \(\vec b = (2\hat i – 2\hat j + 3\hat k)\), and \(\vec n = (3\hat i – 2\hat j + 2\hat k)\)
Then, \(\sin \theta = \frac{{(3\hat i – 2\hat j + 2\hat k) \cdot (2\hat i – 2\hat j + 3\hat k)}}{{|3\hat i – 2\hat j + 2\hat k||2\hat i – 2\hat j + 3\hat k|}} = \frac{{6 + 4 + 6}}{{\sqrt {9 + 4 + 4} \sqrt {4 + 4 + 9} }} = \frac{{16}}{{\sqrt {17} \sqrt {17} }} = \frac{{16}}{{17}}\)
\( \Rightarrow \theta = \frac{{16}}{{17}}\)
Hence, the angle the between \(\vec r = (2\hat i + \hat j – 3\hat k) + \lambda (2\hat i – 2\hat j + 3\hat k)\) and the plane \(\vec r.(3\hat i – 2\hat j + 2\hat k) = 5\) is \(\frac{{16}}{{17}}\).
Q.5. Find the angle between the line \(\vec r = (\hat i + \hat k) + \lambda (\hat j + \hat k)\) and the plane \(\vec r \cdot (2\hat i – \hat j ) = 3\).
Ans: We know that \(\theta \) is the angle between the line be \(\vec r = \vec a + \lambda \vec b\) and plane be \(\vec r \cdot \vec n = d\), then \(\sin \theta = \left| {\frac{{\vec n \cdot \vec b}}{{|n||b|}}} \right|\)
Therefore, if \(\theta \) is the angle between the line \(\vec r = (\hat i + \hat k) + \lambda (\hat j + \hat k)\) and the plane \(\vec r.(2\hat i – \hat j ) = 3\).
Here, \(\vec b = (\hat j + \hat k)\), and \(\vec n = (2\hat i – \hat j )\)
Then, \(\sin \theta = \frac{{(2\hat i – \hat j) \cdot (\hat j + \hat k)}}{{|(2\hat i – \hat j)||(\hat j + \hat k)|}} = \frac{{0 – 1 + 0}}{{\sqrt {4 + 1} \sqrt {1 + 1} }} = \frac{{ – 1}}{{\sqrt 5 \sqrt 2 }} = \frac{{ – 1}}{{\sqrt {10} }}\)
\( \Rightarrow \theta = \left( {\frac{{ – 1}}{{\sqrt {10} }}} \right)\)
Hence, the angle between the line \(\vec r = (\hat i + \hat k) + \lambda (\hat j + \hat k)\) and the plane \(\vec r \cdot (2\hat i – \hat j ) = 3\) is \(\left( {\frac{{ – 1}}{{\sqrt {10} }}} \right)\).
The angle between a line and a plane is the complement of the angle between the line and the normal plane. If \(\theta \) is the angle between the line \(\vec r = \vec a + \lambda \vec b\) and plane \(\vec r.\vec n = d\), then \(\theta = \left( {\frac{{\vec n \cdot \vec b}}{{nb}}} \right)\). Let \(\theta \) be the angle between the line \(\frac{{x – {x_1}}}{l} = \frac{{y – {y_1}}}{m} = \frac{{z – {z_1}}}{n}\) and the given plane \(ax + by + cz + d = 0\) then \(\theta = \left[ {\frac{{|al + bm + cn|}}{{\sqrt {{l^2} + {m^2} + {n^2}} \sqrt {{a^2} + {b^2} + {c^2}} }}} \right]\) ; where \(\left( {0 < \theta < \frac{\pi }{2}} \right)\). If the line is parallel to the normal of the plane, then the line is perpendicular to the plane. If the line is parallel to the given plane, then normal to the plane is perpendicular to the given line i.e. \(al + bm + cn = 0\).
Students must be having many questions regarding Angle Between a Line and a Plane. Here are a few commonly asked questions and answers:
Q.1. How to find the acute angle between a line and a plane?
Ans: The angle between a line and a plane is the complement of the angle between the line and the normal to the plane. Let \(\alpha \) be the plane and \(L\) the line which is not parallel to \(\alpha \). Let the line \(L\) make an angle \(\theta \left( {0 < \theta < \frac{\pi }{2}} \right)\) with the plane \(\alpha \). Then \(\left( {\frac{\pi }{2} – \theta } \right)\) is the acute angle between the normal to the plane and the line \(L\).
Q.2. Find the angle between a line and a plane?
Ans: Let the given line be \(\vec r = \vec a + \lambda \vec b\) and the given plane be \(\vec r \cdot \vec n = d\) and \(\theta \) is the angle between the line and plane, then \(\theta = \left( {\frac{\pi }{2} – \left( {\frac{{\vec n \cdot \vec b}}{{nb}}} \right)} \right) = \left( {\frac{{\vec n \cdot \vec b}}{{nb}}} \right)\)
Q.3. How do you find the angle between a line and a plane?
Ans: Let the given line be \(\vec r = \vec a + \lambda \vec b\) and the given plane be \(\vec r \cdot \vec n = d\).
If \(\phi \) is the angle between the given line (parallel to \(\vec b\)) and the normal to the plane. So, \(\vec n \cdot \vec b = |\vec n||\vec b|\cos \phi = nb\cos \phi \)
\( \Rightarrow \cos \phi = \frac{{\vec n \cdot \vec b}}{{nb}} \Rightarrow \left( {\frac{{\vec n \cdot \vec b}}{{nb}}} \right)\)
Q.4. How to find the angle between a line and a plane?
Ans: Let the given line be \(\frac{{x – {x_1}}}{l} = \frac{{y – {y_1}}}{m} = \frac{{z – {z_1}}}{n}\) and the given plane be \(ax + by + cz + d = 0\). If \(\phi \) is the angle between the given line and the normal to the plane then \(\emptyset = \left[ {\frac{{|al + bm + cn|}}{{\sqrt {{l^2} + {m^2} + {n^2}} \sqrt {{a^2} + {b^2} + {c^2}} }}} \right]\)
Q.5. What is the formula for the angle between a line and a plane?
Ans: Let the given line be \(\vec r = \vec a + \lambda \vec b\) and the given plane be \(\vec r \cdot \vec n = d\).
If \(\phi \) is the angle between the given line (parallel to \(\vec b\)) and the normal to the plane. So, \(\vec n \cdot \vec b = |\vec n||\vec b|\cos \phi = nb\cos \phi \)
\( \Rightarrow \cos \phi = \frac{{\vec n \cdot \vec b}}{{nb}}\)
\(\therefore \left( {\frac{{\vec n \cdot \vec b}}{{nb}}} \right)\)
or
Let the given line be \(\frac{{x – {x_1}}}{l} = \frac{{y – {y_1}}}{m} = \frac{{z – {z_1}}}{n}\) and the given plane be \(ax + by + cz + d = 0\). If \(\phi \) is the angle between the given line and the normal to the plane then \(\emptyset = \left[ {\frac{{|al + bm + cn|}}{{\sqrt {{l^2} + {m^2} + {n^2}} \sqrt {{a^2} + {b^2} + {c^2}} }}} \right]\)