Porisma

Meet a line and a plane

Decide whether a line crosses, misses or lies in a plane, then find its angle.

Classify a line and a plane

Test the line direction against the plane normal first. A nonzero dot product gives one intersection. A zero dot product needs a second test: substitute a point from the line to distinguish containment from a disjoint parallel line.

Let the line be r=a+λm\mathbf r=\mathbf a+\lambda\mathbf m and the plane r⋅n=d\mathbf r\cdot\mathbf n=d, with m≠0\mathbf m\ne\mathbf0 and n≠0\mathbf n\ne\mathbf0.

m⋅n≠0\mathbf m\cdot\mathbf n\ne0

Point test: No additional test needed

Relationship: One crossing

Common points: Exactly one

m⋅n=0\mathbf m\cdot\mathbf n=0

Point test:

a⋅n≠d\mathbf a\cdot\mathbf n\ne d

Relationship: Parallel and disjoint

Common points: None

m⋅n=0\mathbf m\cdot\mathbf n=0

Point test:

a⋅n=d\mathbf a\cdot\mathbf n=d

Relationship: Line lies in plane

Common points: Infinitely many

Solve the one-crossing case

For the one-crossing case, follow the source’s three steps. First write the intersection position as OP→=a+λm\overrightarrow{OP}=\mathbf a+\lambda\mathbf m. Then substitute it into the plane:

(a+λm)⋅n=d,a⋅n+λ(m⋅n)=d,λ=d−a⋅nm⋅n.\begin{aligned}(\mathbf a+\lambda\mathbf m)\cdot\mathbf n&=d,\\\mathbf a\cdot\mathbf n+\lambda(\mathbf m\cdot\mathbf n)&=d,\\\lambda&=\frac{d-\mathbf a\cdot\mathbf n}{\mathbf m\cdot\mathbf n}.\end{aligned}

Finally substitute this parameter back into the line to obtain P. The source summary’s last instruction says “find Π\Pi”; the required result is the intersection point P, not the plane.

Interpret a zero direction test

When m⋅n=0\mathbf m\cdot\mathbf n=0, do not divide by it. Substitution instead gives either a contradiction (no intersection) or an identity (every line point is in the plane). The source uses “parallel” for both an in-plane direction and a disjoint parallel line; the point test distinguishes those cases. A nonparallel line cannot be disjoint from an infinite plane in three-dimensional Euclidean space.

Derive the angle between a line and a plane

The source defines α\alpha using the acute angle between the line and its projection in the plane. For nonzero direction m\mathbf m and normal n\mathbf n, first find the directed-vector angle θ∈[0,π]\theta\in[0,\pi]:

cos⁡θ=m⋅n∣m∣∣n∣.\cos\theta=\frac{\mathbf m\cdot\mathbf n}{|\mathbf m||\mathbf n|}.

The source refers back to its earlier vector-angle section 12.2. It gives two cases, each with a complement method and a trigonometric derivation.

Acute θ\theta. Here α=π/2−θ\alpha=\pi/2-\theta. Using cos⁡(π/2−α)=sin⁡α\cos(\pi/2-\alpha)=\sin\alpha gives

sin⁡α=m⋅n∣m∣∣n∣.\sin\alpha=\frac{\mathbf m\cdot\mathbf n}{|\mathbf m||\mathbf n|}.

Obtuse θ\theta. Here α=θ−π/2\alpha=\theta-\pi/2. Expand the cosine of a sum:

cos⁡(π/2+α)=cos⁡(π/2)cos⁡α−sin⁡(π/2)sin⁡α=−sin⁡α.\begin{aligned}\cos(\pi/2+\alpha)&=\cos(\pi/2)\cos\alpha-\sin(\pi/2)\sin\alpha\\&=-\sin\alpha.\end{aligned}

Thus −sin⁡α=(m⋅n)/(∣m∣∣n∣)-\sin\alpha=(\mathbf m\cdot\mathbf n)/(|\mathbf m||\mathbf n|), and the negative dot product must be negated before taking the nonnegative line–plane angle. Both cases combine as

α=sin⁡−1 ⁣(∣m⋅n∣∣m∣∣n∣).\alpha=\sin^{-1}\!\left(\frac{|\mathbf m\cdot\mathbf n|}{|\mathbf m||\mathbf n|}\right).

Reversing either vector does not change the geometric line–plane angle. The source’s word “acute” describes its general examples; the formula also includes the boundary cases α=0\alpha=0 for a direction parallel to the plane and α=π/2\alpha=\pi/2 for a perpendicular line. In the latter case the projected direction is zero, so the projection-angle description is understood by this perpendicular convention. Neither zero vector defines the required direction or normal.

Explain the three possible intersection equations

For Π:x+2y+2z=6\Pi:x+2y+2z=6, classify the lines l1:r=(0,0,0)+t(2,−1,0)l_1:\mathbf r=(0,0,0)+t(2,-1,0), l2:r=(6,0,0)+t(2,−1,0)l_2:\mathbf r=(6,0,0)+t(2,-1,0) and l3:r=(0,0,0)+t(1,0,0)l_3:\mathbf r=(0,0,0)+t(1,0,0). Predict the outcome using direction and point tests, then interpret the equation obtained by substitution.

After your attempt: compare the reasoning

With normal n=(1,2,2)\mathbf n=(1,2,2), the first two directions have dot product zero with the normal.

The origin is off the plane, so l1l_1 is parallel and disjoint: substitution gives 0=60=6.

The base point (6,0,0)(6,0,0) is in the plane, so all of l2l_2 lies in it: substitution gives 6=66=6.

For l3l_3, the direction dot product is 1, so there is one crossing. Substitution gives t=6t=6, at (6,0,0)(6,0,0).

An inconsistent equation, an identity and a unique parameter correspond to different geometric situations.

Compare a line angle with its normal angle

A line has direction m=(1,0,3)\mathbf m=(1,0,\sqrt3) and a plane has normal n=(0,0,1)\mathbf n=(0,0,1). Find their angle. Repeat for line directions (1,0,0)(1,0,0) and (0,0,1)(0,0,1). Explain why blindly reporting the angle to the normal would exchange the two boundary cases.

After your attempt: compare the reasoning

For (1,0,3)(1,0,\sqrt3) the normal angle is 30∘30^\circ, so the line–plane angle is 60∘60^\circ.

The dot-product cosine gives the angle to the normal; take its complement for the plane.

For (1,0,0)(1,0,0) the normal angle is 90∘90^\circ but the line–plane angle is 0∘0^\circ; for (0,0,1)(0,0,1) the normal angle is 0∘0^\circ but the line–plane angle is 90∘90^\circ.

Use sin⁡α=∣m⋅n∣/(∣m∣∣n∣)\sin\alpha=|\mathbf m\cdot\mathbf n|/(|\mathbf m||\mathbf n|) for the line–plane angle.

A direction test alone says nothing about whether a parallel line is contained in the plane.

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