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Mathematics · Ch 6 — Applications of Vector Algebra

Equation of a Plane in Normal Form

6.8.1

Equation of a Plane in Normal Form

Theorem 6.15 (Normal form). The plane at perpendicular distance p≥0p\ge0 from the origin, with unit normal vector d^\hat d, has vector equation

r⃗⋅d^=p.\vec r\cdot\hat d=p.

Proof. Let AA be the foot of the perpendicular from OO to the plane, so OA⃗=pd^\vec{OA}=p\hat d. For any point PP (position vector r⃗\vec r) on the plane, AP⃗=r⃗−pd^\vec{AP}=\vec r-p\hat d is perpendicular to OA⃗=pd^\vec{OA}=p\hat d, so (r⃗−pd^)⋅pd^=0(\vec r-p\hat d)\cdot p\hat d=0, i.e. (r⃗−pd^)⋅d^=0(\vec r-p\hat d)\cdot\hat d=0 (dividing by pp, assuming p≠0p\ne0), giving r⃗⋅d^=p\vec r\cdot\hat d=p.

(b) Cartesian normal form. Writing d^=li^+mj^+nk^\hat d=l\hat i+m\hat j+n\hat k (direction cosines l,m,nl,m,n) and r⃗=xi^+yj^+zk^\vec r=x\hat i+y\hat j+z\hat k, the equation becomes

lx+my+nz=p.lx+my+nz=p.

Remark.

(i) If the plane passes through the origin, p=0p=0, giving lx+my+nz=0lx+my+nz=0. …