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Mathematics · Ch 6 — Line and Plane

Equation of Plane Passing through a Point and Perpendicular to a Vector

6.4.1

Equation of Plane Passing through a Point and Perpendicular to a Vector

Theorem 6.8 (vector form). The plane through the point A(a⃗)A(\vec a) that is perpendicular to a fixed non-zero vector n⃗\vec n has the equation r⃗⋅n⃗=a⃗⋅n⃗\vec r \cdot \vec n = \vec a \cdot \vec n, where P(r⃗)P(\vec r) denotes an arbitrary point of the plane.

Why this is true: if P(r⃗)P(\vec r) lies on the plane, the chord AP→\overrightarrow{AP} lies entirely in the plane, so it must be perpendicular to the normal n⃗\vec n. Writing this perpendicularity as a dot product, AP→⋅n⃗=0\overrightarrow{AP}\cdot\vec n = 0. Since AP→=r⃗−a⃗\overrightarrow{AP} = \vec r - \vec a, this becomes (r⃗−a⃗)⋅n⃗=0(\vec r - \vec a)\cdot \vec n = 0, and expanding the dot product over the subtraction gives r⃗⋅n⃗−a⃗⋅n⃗=0\vec r \cdot \vec n - \vec a \cdot \vec n = 0, i.e. r⃗⋅n⃗=a⃗⋅n⃗\vec r\cdot\vec n = \vec a \cdot \vec n. This is called the vector equation of a plane in scalar product form (Fig. 6.8 shows the point AA, a general point PP on the plane, the chord AP→\overrightarrow{AP} lying flat in the plane, and n⃗\vec n standing perpendicular to it). If the fixed number a⃗⋅n⃗\vec a \cdot \vec n is called dd, the equation shortens further to r⃗⋅n⃗=d\vec r \cdot \vec n = d.

Theorem 6.9 (Cartesian form). If A(x1,y1,z1)A(x_1, y_1, z_1) is a point of the plane and a,b,ca, b, c are the direction ratios of the normal, the same idea translated into coordinates gives a(x−x1)+b(y−y1)+c(z−z1)=0a(x - x_1) + b(y - y_1) + c(z - z_1) = 0. Here P(x,y,z)P(x, y, z) is a general point of the plane, so x−x1,y−y1,z−z1x - x_1, y - y_1, z - z_1 are the direction ratios of AP→\overrightarrow{AP}; because AP→\overrightarrow{AP} is perpendicular to the normal, the sum of the products of corresponding direction ratios must vanish, which is exactly this equation. Multiplying out gives the familiar linear form ax+by+cz+d=0ax + by + cz + d = 0.

Ex.(1): the plane through the point with position vector 2i^+3j^+4k^2\hat i + 3\hat j + 4\hat k that is perpendicular to 2i^+j^−2k^2\hat i + \hat j - 2\hat k. Here a⃗⋅n⃗=(2)(2)+(3)(1)+(4)(−2)=4+3−8=−1\vec a \cdot \vec n = (2)(2) + (3)(1) + (4)(-2) = 4 + 3 - 8 = -1, so by Theorem 6.8 the required equation is r⃗⋅(2i^+j^−2k^)=−1\vec r \cdot (2\hat i + \hat j - 2\hat k) = -1.

Ex.(2): the plane through A(1,2,3)A(1, 2, 3) whose normal has direction ratios 3,2,53, 2, 5. By Theorem 6.9, 3(x−1)+2(y−2)+5(z−3)=03(x-1) + 2(y-2) + 5(z-3) = 0, which simplifies to 3x+2y+5z−22=03x + 2y + 5z - 22 = 0. …

Figure 6.8Fig. 6.8 — Plane through the point A(ā) perpendicular to the normal vector n̄; a point P(r̄) lies in the plane
Fig. 6.8 — Fig. 6.8 — Plane through the point A(ā) perpendicular to the normal vector n̄; a point P(r̄) lies in the plane

Drawn by us to help you understand the concept clearly, and verified to make sure it's accurate. For exams, practice from your textbook's own diagram.

What this figure shows. A shaded parallelogram-shaped plane carries a marked point A with position vector a-bar and a second point P with position vector r-bar on the same plane, connected by a dotted segment labelled AP. A vertical arrow labelled n-bar rises from the plane at A, meeting the plane at a right angle (shown by the small square corner mark) to show that the fixed vector n-bar is normal to the plane while AP lies flat within it, which is exactly the perpendicularity AP . n-bar = 0 that the proof of Theorem 6.8 turns in …