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Mathematics · Ch 6 — Line and Plane

The Normal Form of Equation of Plane

6.4.4

The Normal Form of Equation of Plane

Theorem 6.12 (normal form). If pp is the (non-negative) distance of a plane from the origin and n^\hat n is the unit vector along the perpendicular dropped from the origin onto the plane, the plane's equation is simply r⃗⋅n^=p\vec r \cdot \hat n = p.

Why this is true: let NN be the foot of that perpendicular, so ON→=p\overrightarrow{ON} = p in length; since n^\hat n is the unit vector along ON→\overrightarrow{ON}, this means ON→=pn^\overrightarrow{ON} = p\hat n. For any point P(r⃗)P(\vec r) of the plane, NP→\overrightarrow{NP} lies in the plane and is therefore perpendicular to n^\hat n (the perpendicular to the plane), so NP→⋅n^=0\overrightarrow{NP}\cdot\hat n = 0. Writing NP→=r⃗−pn^\overrightarrow{NP} = \vec r - p\hat n turns this into (r⃗−pn^)⋅n^=0(\vec r - p\hat n)\cdot\hat n = 0, i.e. r⃗⋅n^−p(n^⋅n^)=0\vec r\cdot\hat n - p(\hat n\cdot\hat n) = 0; since n^\hat n is a unit vector, n^⋅n^=1\hat n\cdot\hat n = 1, leaving r⃗⋅n^=p\vec r\cdot \hat n = p (Fig. 6.11 shows the axes, the foot NN, the segment ONON of length pp, the unit vector n^\hat n along it, and a general point PP of the plane with position vector r⃗\vec r).

Several useful facts follow immediately. If l,m,nl, m, n are the direction cosines of the normal, then n^=li^+mj^+nk^\hat n = l\hat i + m\hat j + n\hat k, and the coordinates of the foot NN itself are (pl,pm,pn)(pl, pm, pn) — a shortcut used repeatedly below. In Cartesian coordinates the normal form reads lx+my+nz=plx + my + nz = p. Finally, because a unit normal can point either way, there are always two planes at a given distance pp from the origin with the same underlying normal direction, namely r⃗⋅n^=±p\vec r\cdot\hat n = \pm p.

Ex.(7): the plane at distance 66 from the origin, normal to 2i^−j^+2k^2\hat i - \hat j + 2\hat k. Here ∣n⃗∣=4+1+4=3|\vec n| = \sqrt{4+1+4} = 3, so n^=13(2i^−j^+2k^)\hat n = \tfrac{1}{3}(2\hat i - \hat j + 2\hat k), and r⃗⋅n^=p\vec r\cdot\hat n = p becomes r⃗⋅13(2i^−j^+2k^)=6\vec r\cdot\tfrac{1}{3}(2\hat i-\hat j+2\hat k)=6, i.e. r⃗⋅(2i^−j^+2k^)=18\vec r\cdot(2\hat i - \hat j + 2\hat k) = 18.

Ex.(8): the perpendicular distance of the origin from x−3y+4z−6=0x - 3y + 4z - 6 = 0. The normal has direction ratios 1,−3,41, -3, 4, so ∣n⃗∣=1+9+16=26|\vec n| = \sqrt{1+9+16}=\sqrt{26}; dividing through converts x−3y+4z=6x-3y+4z=6 to normal form 126x−326y+426z=626\tfrac{1}{\sqrt{26}}x - \tfrac{3}{\sqrt{26}}y + \tfrac{4}{\sqrt{26}}z = \tfrac{6}{\sqrt{26}}, so the distance is 626\tfrac{6}{\sqrt{26}}. …

Figure 6.11Fig. 6.11 — Normal form of the equation of a plane: ON ⟂ plane (foot N, length p), unit normal n̂, and r̄ = OP to a point P on the plane
Fig. 6.11 — Fig. 6.11 — Normal form of the equation of a plane: ON ⟂ plane (foot N, length p), unit normal n̂, and r̄ = OP to a point P on 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 3-D sketch shows the coordinate axes X, Y, Z meeting at the origin O, with a shaded plane cutting across the picture; N is the foot of the perpendicular dropped from O onto the plane, and P is a general point of the plane. The segment ON is labelled with its length p, the unit vector n-hat is drawn along ON with a right-angle mark showing NP perpendicular to n-hat, and the position vector r-bar of P is drawn from O to P, together giving the picture behind the normal-form equation r …