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Mathematics · Ch 6 — Applications of Vector Algebra

Distance of a Point from a Plane

6.8.12

Distance of a Point from a Plane

Theorem 6.20 (vector form). The perpendicular distance from a point with position vector u⃗\vec u to the plane r⃗⋅n⃗=p\vec r\cdot\vec n=p is

δ=∣u⃗⋅n⃗−p∣∣n⃗∣.\delta=\frac{|\vec u\cdot\vec n-p|}{|\vec n|}.

Proof sketch. Drop the perpendicular from A(u⃗)A(\vec u) to the plane, meeting it at FF; the line AFAF is r⃗=u⃗+tn⃗\vec r=\vec u+t\vec n (parallel to the normal). Substituting into the plane's equation gives the parameter t1t_1 at FF, namely t1=p−u⃗⋅n⃗∣n⃗∣2t_1=\dfrac{p-\vec u\cdot\vec n}{|\vec n|^2}; then FA⃗=−t1n⃗\vec{FA}=-t_1\vec n has length δ=∣t1∣∣n⃗∣=∣u⃗⋅n⃗−p∣∣n⃗∣\delta=|t_1||\vec n|=\dfrac{|\vec u\cdot\vec n-p|}{|\vec n|}. The position vector of the foot FF itself is r⃗1=u⃗+t1n⃗=u⃗+p−u⃗⋅n⃗∣n⃗∣2n⃗\vec r_1=\vec u+t_1\vec n=\vec u+\dfrac{p-\vec u\cdot\vec n}{|\vec n|^2}\vec n.

(b) Cartesian form. For a point (x1,y1,z1)(x_1,y_1,z_1) and plane ax+by+cz=pax+by+cz=p:

δ=∣ax1+by1+cz1−p∣a2+b2+c2.\delta=\frac{|ax_1+by_1+cz_1-p|}{\sqrt{a^2+b^2+c^2}}. …