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Mathematics · Ch 6 — Line and Plane

The Vector Equation of the Plane Passing through Point A(a-bar) and Parallel to b-bar and c-bar

6.4.2

The Vector Equation of the Plane Passing through Point A(a-bar) and Parallel to b-bar and c-bar

Theorem 6.10. The plane through the point A(a⃗)A(\vec a) that is parallel to two given non-zero, non-parallel vectors b⃗\vec b and c⃗\vec c has the equation (r⃗−a⃗)⋅(b⃗×c⃗)=0\left(\vec r - \vec a\right)\cdot\left(\vec b\times\vec c\right) = 0, equivalently r⃗⋅(b⃗×c⃗)=a⃗⋅(b⃗×c⃗)\vec r\cdot(\vec b\times\vec c) = \vec a\cdot(\vec b\times\vec c).

Why this is true: because b⃗\vec b and c⃗\vec c both lie parallel to the plane (rather than in some other orientation), their cross product b⃗×c⃗\vec b\times\vec c is perpendicular to both of them and therefore perpendicular to the whole plane — it is a normal vector, even though b⃗\vec b and c⃗\vec c individually are not. For a general point P(r⃗)P(\vec r) of the plane, AP→\overrightarrow{AP} lies in the plane, so AP→\overrightarrow{AP} must be perpendicular to b⃗×c⃗\vec b\times\vec c: AP→⋅(b⃗×c⃗)=0\overrightarrow{AP}\cdot(\vec b\times\vec c) = 0. Substituting AP→=r⃗−a⃗\overrightarrow{AP} = \vec r - \vec a gives the stated equation (Fig. 6.9 shows b⃗\vec b and c⃗\vec c as two arrows lying flat in the plane from AA, and b⃗×c⃗\vec b \times \vec c standing up perpendicular to the plane).

A useful alternative comes from noticing that AP→\overrightarrow{AP}, b⃗\vec b and c⃗\vec c are all parallel to the same plane, so they are coplanar; hence AP→\overrightarrow{AP} can always be written as a linear combination AP→=λb⃗+μc⃗\overrightarrow{AP} = \lambda\vec b + \mu\vec c for some scalars λ,μ\lambda, \mu. This gives r⃗−a⃗=λb⃗+μc⃗\vec r - \vec a = \lambda\vec b + \mu\vec c, i.e. r⃗=a⃗+λb⃗+μc⃗\vec r = \vec a + \lambda\vec b + \mu\vec c — the vector equation of a plane in parametric form, with λ\lambda and μ\mu free real parameters that sweep out every point of the plane.

Ex.(4): the plane through A(−1,2,−5)A(-1, 2, -5) parallel to b⃗=4i^−j^+3k^\vec b = 4\hat i - \hat j + 3\hat k and c⃗=i^+j^−k^\vec c = \hat i + \hat j - \hat k. Here a⃗=−i^+2j^−5k^\vec a = -\hat i + 2\hat j - 5\hat k, and b⃗×c⃗=∣i^j^k^4−1311−1∣=−2i^+7j^+5k^\vec b \times \vec c = \begin{vmatrix}\hat i & \hat j & \hat k \\ 4 & -1 & 3 \\ 1 & 1 & -1\end{vmatrix} = -2\hat i + 7\hat j + 5\hat k. Then a⃗⋅(b⃗×c⃗)=(−1)(−2)+(2)(7)+(−5)(5)=2+14−25=−9\vec a\cdot(\vec b\times\vec c) = (-1)(-2) + (2)(7) + (-5)(5) = 2 + 14 - 25 = -9, so the plane's equation is r⃗⋅(−2i^+7j^+5k^)=−9\vec r\cdot(-2\hat i + 7\hat j + 5\hat k) = -9. …

Figure 6.9Fig. 6.9 — Vector equation of a plane through A(ā) with normal n̄, using position vectors ā = OA and r̄ = OP
Fig. 6.9 — Fig. 6.9 — Vector equation of a plane through A(ā) with normal n̄, using position vectors ā = OA and r̄ = OP

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 plane shows point A (with position vector a-bar) as the vertex of two arrows drawn inside the plane, labelled b-bar and c-bar, meeting at a right angle mark, with a second point P (position vector r-bar) on the plane joined to A by a dotted segment marked AP. Directly above A, a vertical arrow labelled b-bar x c-bar rises perpendicular to the plane, illustrating that although b-bar and c-bar themselves only lie in the plane (they do not have to be perpendicular to each other), their cross product is the true normal direction used to test …