Characterization of a plane in the space

α\alphaα

is a plane in the space and we’ve been told in school that its equation in canonical form is:

ax+by+cz+d=0
ax+by+cz+d=0
ax+by+cz+d=0

But this doesn’t tell us nothing about the plane characteristics and no-one explained us how th…


This content originally appeared on DEV Community and was authored by ccarcaci

α\alphaα is a plane in the space and we've been told in school that its equation in canonical form is:

ax+by+cz+d=0 ax+by+cz+d=0 ax+by+cz+d=0

But this doesn't tell us nothing about the plane characteristics and no-one explained us how this equation is formed.

Plane formation

A plane in the space could be identified by a point and 2 non-parallel vectors.

P=(x0,y0,z0)∈αu‾,v‾∈α P=(x_0,y_0,z_0)\in \alpha \\ \\ \underline{u},\underline{v}\in \alpha P=(x0​,y0​,z0​)∈αu​,v​∈α

u‾,v‾\underline{u},\underline{v}u​,v​ have magnitude, direction, and orientation. It's possible to write:

u‾=PQv‾=PR \underline{u}=PQ \\ \underline{v}=PR u​=PQv​=PR

Every other point XXX that belongs to α\alphaα could be written as a linear combination of these elements starting from the origin:

OX=OP+s∗u‾+t∗v‾X=(x,y,z)∈αs∈Rt∈R OX=OP+s*\underline{u}+t*\underline{v} \\ X=(x,y,z)\in\alpha \\ s\in R \\ t\in R OX=OP+s∗u​+t∗v​X=(x,y,z)∈αs∈Rt∈R

This clarifies why it is possible to say:

A plane in the space could be identified by a point and 2 non-parallel vectors.

Parametric equations

XXX can be described by its parametric equations:

x=x0+m1∗s+m2∗ty=y0+n1∗s+n2∗tz=z0+p1∗s+p2∗tu‾=(m1,n1,p1)v‾=(m2,n2,p2) x=x_0+m_1*s+m_2*t \\ y=y_0+n_1*s+n_2*t \\ z=z_0+p_1*s+p_2*t \\ \underline{u}=(m_1,n_1,p_1) \\ \underline{v}=(m_2,n_2,p_2) x=x0​+m1​∗s+m2​∗ty=y0​+n1​∗s+n2​∗tz=z0​+p1​∗s+p2​∗tu​=(m1​,n1​,p1​)v​=(m2​,n2​,p2​)

The goal is to solve this system over sss and ttt reducing it to a linear equation that is satisfied for the points belongings to the plane.

A bit of math

t=x−x0−m1∗sm2t=y−y0−n1∗sn2t=z−z0−p1∗sp2 t=\frac{x-x_0-m_1*s}{m_2} \\ t=\frac{y-y_0-n_1*s}{n_2} \\ t=\frac{z-z_0-p_1*s}{p_2} t=m2​x−x0​−m1​∗s​t=n2​y−y0​−n1​∗s​t=p2​z−z0​−p1​∗s​

Equal over ttt :

x−x0−m1∗sm2=y−y0−n1∗sn2x−x0−m1∗sm2=z−z0−p1∗sp2 \frac{x-x_0-m_1*s}{m_2}=\frac{y-y_0-n_1*s}{n_2} \\ \frac{x-x_0-m_1*s}{m_2}=\frac{z-z_0-p_1*s}{p_2} m2​x−x0​−m1​∗s​=n2​y−y0​−n1​∗s​m2​x−x0​−m1​∗s​=p2​z−z0​−p1​∗s​

ttt is gone, let's target sss

x−x0m2−m1m2∗s=y−y0n2−n1n2∗sx−x0m2−m1m2∗s=z−z0p2−p1p2∗s \frac{x-x_0}{m_2}-\frac{m_1}{m_2}*s=\frac{y-y_0}{n_2}-\frac{n_1}{n_2}*s \\ \frac{x-x_0}{m_2}-\frac{m_1}{m_2}*s=\frac{z-z_0}{p_2}-\frac{p_1}{p_2}*s m2​x−x0​​−m2​m1​​∗s=n2​y−y0​​−n2​n1​​∗sm2​x−x0​​−m2​m1​​∗s=p2​z−z0​​−p2​p1​​∗s
x−x0m2−y−y0n2=(m1m2−n1n2)∗sx−x0m2−z−z0p2=(m1m2−p1p2)∗s \frac{x-x_0}{m_2}-\frac{y-y_0}{n_2}=(\frac{m_1}{m_2}-\frac{n_1}{n_2})*s \\ \frac{x-x_0}{m_2}-\frac{z-z_0}{p_2}=(\frac{m_1}{m_2}-\frac{p_1}{p_2})*s m2​x−x0​​−n2​y−y0​​=(m2​m1​​−n2​n1​​)∗sm2​x−x0​​−p2​z−z0​​=(m2​m1​​−p2​p1​​)∗s
A=x−x0m2B=y−y0n2C=m1m2D=n1n2E=z−z0p2F=p1p2 A=\frac{x-x_0}{m_2} \\ B=\frac{y-y_0}{n_2} \\ C=\frac{m_1}{m_2} \\ D=\frac{n_1}{n_2} \\ E=\frac{z-z_0}{p_2} \\ F=\frac{p_1}{p_2} A=m2​x−x0​​B=n2​y−y0​​C=m2​m1​​D=n2​n1​​E=p2​z−z0​​F=p2​p1​​
A−B=s∗(C−D)A−E=s∗(C−F) A-B=s*(C-D) \\ A-E=s*(C-F) A−B=s∗(C−D)A−E=s∗(C−F)
s=A−BC−Ds=A−EC−F s=\frac{A-B}{C-D} \\ s=\frac{A-E}{C-F} s=C−DA−B​s=C−FA−E​
(A−B)(C−F)=(A−E)(C−D)AC−AF−BC+BF=AC−AD−CE+DE−AF−BC+BF=−AD−CD+DEAF−AD+BC−BF−CE+DE=0A∗(F−D)+B∗(C−F)+E∗(D−C)=0 (A-B)(C-F)=(A-E)(C-D) \\ AC-AF-BC+BF=AC-AD-CE+DE \\ -AF-BC+BF=-AD-CD+DE \\ AF-AD+BC-BF-CE+DE=0 \\ A*(F-D)+B*(C-F)+E*(D-C)=0 (A−B)(C−F)=(A−E)(C−D)AC−AF−BC+BF=AC−AD−CE+DE−AF−BC+BF=−AD−CD+DEAF−AD+BC−BF−CE+DE=0A∗(F−D)+B∗(C−F)+E∗(D−C)=0
x−x0m2(p1p2−n1n2)+y−y0n2(m1m2−p1p2+z−z0p2∗(n1n2−m1m2)=0 \frac{x-x_0}{m_2}(\frac{p_1}{p_2}-\frac{n_1}{n_2})+\frac{y-y_0}{n_2}(\frac{m_1}{m_2}-\frac{p_1}{p_2}+\frac{z-z_0}{p_2}*(\frac{n_1}{n_2}-\frac{m_1}{m_2})=0 m2​x−x0​​(p2​p1​​−n2​n1​​)+n2​y−y0​​(m2​m1​​−p2​p1​​+p2​z−z0​​∗(n2​n1​​−m2​m1​​)=0
a=p1p2−n1n2m2b=m1m2−p1p2n2c=n1n2−m1m2p2 a=\frac{\frac{p_1}{p_2}-\frac{n_1}{n_2}}{m_2} \\ b=\frac{\frac{m_1}{m_2}-\frac{p_1}{p_2}}{n_2} \\ c=\frac{\frac{n_1}{n_2}-\frac{m_1}{m_2}}{p_2} a=m2​p2​p1​​−n2​n1​​​b=n2​m2​m1​​−p2​p1​​​c=p2​n2​n1​​−m2​m1​​​
a∗(x−x0)+b∗(y−y0)+c∗(z−z0)=0ax+by+cz−ax0−by0−cz0=0d=−ax0−by0−cz0ax+by+cz+d=0 a*(x-x_0)+b*(y-y_0)+c*(z-z_0)=0 \\ ax+by+cz-ax_0-by_0-cz_0=0 \\ d=-ax_0-by_0-cz_0 \\ ax+by+cz+d=0 a∗(x−x0​)+b∗(y−y0​)+c∗(z−z0​)=0ax+by+cz−ax0​−by0​−cz0​=0d=−ax0​−by0​−cz0​ax+by+cz+d=0
w‾=(a,b,c) \underline{w}=(a,b,c) w​=(a,b,c)

This is the directional vector of the plane, orthogonal to it.

Geometry

To prove that w‾\underline{w}w​ is orthogonal to the plane, it should be orthogonal to both u‾\underline{u}u​ and v‾\underline{v}v​ .

The scalar product should be 0:

w‾⋅u‾=0w‾⋅v‾=0 \underline{w}\cdot\underline{u}=0 \\ \underline{w}\cdot\underline{v}=0 w​⋅u​=0w​⋅v​=0
w‾⋅u‾=a∗m1+b∗n1+c∗p1=p1p2−n1n2m2∗m1+m1m2−p1p2n2∗n1+n1n2−m1m2p2∗p1 \underline{w}\cdot\underline{u}=a*m_1+b*n_1+c*p_1=\frac{\frac{p_1}{p_2}-\frac{n_1}{n_2}}{m_2}*m_1+\frac{\frac{m_1}{m_2}-\frac{p_1}{p_2}}{n_2}*n_1+\frac{\frac{n_1}{n_2}-\frac{m_1}{m_2}}{p_2}*p_1 w​⋅u​=a∗m1​+b∗n1​+c∗p1​=m2​p2​p1​​−n2​n1​​​∗m1​+n2​m2​m1​​−p2​p1​​​∗n1​+p2​n2​n1​​−m2​m1​​​∗p1​
w‾⋅u‾=p1p2m1m2−n1n2m1m2+m1m2n1n2−p1p2n1n2+n1n2p1p2−m1m2p1p2=0 \underline{w}\cdot\underline{u}=\frac{p_1}{p_2}\frac{m_1}{m_2}-\frac{n_1}{n_2}\frac{m_1}{m_2}+\frac{m_1}{m_2}\frac{n_1}{n_2}-\frac{p_1}{p_2}\frac{n_1}{n_2}+\frac{n_1}{n_2}\frac{p_1}{p_2}-\frac{m_1}{m_2}\frac{p_1}{p_2}=0 w​⋅u​=p2​p1​​m2​m1​​−n2​n1​​m2​m1​​+m2​m1​​n2​n1​​−p2​p1​​n2​n1​​+n2​n1​​p2​p1​​−m2​m1​​p2​p1​​=0
w‾⋅v‾=a∗m2+b∗n2+c∗p2=p1p2−n1n2m2∗m2+m1m2−p1p2n2∗n2+n1n2−m1m2p2∗p2=0 \underline{w}\cdot\underline{v}=a*m_2+b*n_2+c*p_2=\frac{\frac{p_1}{p_2}-\frac{n_1}{n_2}}{m_2}*m_2+\frac{\frac{m_1}{m_2}-\frac{p_1}{p_2}}{n_2}*n_2+\frac{\frac{n_1}{n_2}-\frac{m_1}{m_2}}{p_2}*p_2=0 w​⋅v​=a∗m2​+b∗n2​+c∗p2​=m2​p2​p1​​−n2​n1​​​∗m2​+n2​m2​m1​​−p2​p1​​​∗n2​+p2​n2​n1​​−m2​m1​​​∗p2​=0


This content originally appeared on DEV Community and was authored by ccarcaci


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