The plane p1p_1 has equation x−y+z=0x - y + z = 0 and the plane p2p_2 has equation x+y+z=2x + y + z = 2.

  1. (a)

    Find the acute angle between planes p1p_1 and p2p_2.

  2. (b)

    Find the vector equation of the line of intersection of planes p1p_1 and p2p_2.

  3. (c)

    With reference to the origin OO, the points AA and BB are such that OA→=−2i+j−k\overrightarrow{OA} = -2\mathbf{i} + \mathbf{j} - \mathbf{k} and OB→=i+j\overrightarrow{OB} = \mathbf{i} + \mathbf{j}. The line ll has equation r=−2i+j−k+μ(i−k)\mathbf{r} = -2\mathbf{i} + \mathbf{j} - \mathbf{k} + \mu(\mathbf{i} - \mathbf{k}), where μ\mu is a parameter.

    Find the shortest distance between line ll and the line with cartesian equation x−3=−z+2x - 3 = -z + 2, y=1y = 1.

  4. (d)

    The point CC lies on ll such that angle ABC=90∘ABC = 90^\circ. Find the position vector of point CC.

  5. (e)

    Find the position vector of the foot of perpendicular from point AA to p2p_2.

  6. (f)

    A plane p3p_3 is equidistant to both point AA and plane p2p_2. Find the cartesian equation of plane p3p_3.

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Worked solution

10(a)

1. Identify the normal vectors from the cartesian equations of the planes.

From the equations x−y+z=0x - y + z = 0 and x+y+z=2x + y + z = 2, the normal vectors to planes p1p_1 and p2p_2 are respectively:
n1=(1−11)\mathbf{n}_1 = \begin{pmatrix} 1 \\ -1 \\ 1 \end{pmatrix} and n2=(111)\mathbf{n}_2 = \begin{pmatrix} 1 \\ 1 \\ 1 \end{pmatrix}

2. Use the scalar product to find the acute angle between the normal vectors.

Let θ\theta be the acute angle between the planes.
cos⁡θ=∣n1⋅n2∣∣n1∣∣n2∣\cos \theta = \frac{| \mathbf{n}_1 \cdot \mathbf{n}_2 |}{|\mathbf{n}_1| |\mathbf{n}_2|}
cos⁡θ=∣(1)(1)+(−1)(1)+(1)(1)∣12+(−1)2+1212+12+12\cos \theta = \frac{|(1)(1) + (-1)(1) + (1)(1)|}{\sqrt{1^2+(-1)^2+1^2} \sqrt{1^2+1^2+1^2}}
cos⁡θ=133=13\cos \theta = \frac{1}{\sqrt{3}\sqrt{3}} = \frac{1}{3}
θ=cos⁡−1(13)≈70.5287∘≈70.5∘ (1 d.p.)\theta = \cos^{-1}\left(\frac{1}{3}\right) \approx 70.5287^\circ \approx 70.5^\circ \text{ (1 d.p.)}

Answer

70.5∘70.5^\circ

10(b)

1. Find the direction vector of the line of intersection using the cross product of the planes' normal vectors.

n1=(1−11),n2=(111)\mathbf{n}_1 = \begin{pmatrix} 1 \\ -1 \\ 1 \end{pmatrix}, \quad \mathbf{n}_2 = \begin{pmatrix} 1 \\ 1 \\ 1 \end{pmatrix}

The direction vector d\mathbf{d} of the line of intersection is given by n1×n2\mathbf{n}_1 \times \mathbf{n}_2:
d=(1−11)×(111)=((−1)(1)−(1)(1)(1)(1)−(1)(1)(1)(1)−(−1)(1))=(−202)\mathbf{d} = \begin{pmatrix} 1 \\ -1 \\ 1 \end{pmatrix} \times \begin{pmatrix} 1 \\ 1 \\ 1 \end{pmatrix} = \begin{pmatrix} (-1)(1) - (1)(1) \\ (1)(1) - (1)(1) \\ (1)(1) - (-1)(1) \end{pmatrix} = \begin{pmatrix} -2 \\ 0 \\ 2 \end{pmatrix}

Taking a simpler parallel vector (by dividing by 2), we use d=(−101)\mathbf{d} = \begin{pmatrix} -1 \\ 0 \\ 1 \end{pmatrix}.

2. Find a point that lies on both planes to serve as the position vector for the line.

Let z=0z = 0. The Cartesian equations of the planes become:
x−y=0  ⟹  x=yx - y = 0 \implies x = y
x+y=2x + y = 2

Substituting x=yx = y into the second equation:
2y=2  ⟹  y=1 and x=12y = 2 \implies y = 1 \text{ and } x = 1

A common point on the line is (1,1,0)(1, 1, 0), so the position vector is a=(110)\mathbf{a} = \begin{pmatrix} 1 \\ 1 \\ 0 \end{pmatrix}.

3. State the vector equation of the line.

The equation of the line is r=a+λd\mathbf{r} = \mathbf{a} + \lambda \mathbf{d}, where λ∈R\lambda \in \mathbb{R}.
r=(110)+λ(−101),λ∈R\mathbf{r} = \begin{pmatrix} 1 \\ 1 \\ 0 \end{pmatrix} + \lambda \begin{pmatrix} -1 \\ 0 \\ 1 \end{pmatrix}, \quad \lambda \in \mathbb{R}

Answer

r=(110)+λ(−101),λ∈R\mathbf{r} = \begin{pmatrix} 1 \\ 1 \\ 0 \end{pmatrix} + \lambda \begin{pmatrix} -1 \\ 0 \\ 1 \end{pmatrix}, \quad \lambda \in \mathbb{R}

10(c)

1. Express the equation of the second line in vector form and observe it is parallel to $l$.

Let the second line be l2l_2. Its cartesian equation is given by x−3=z−2−1x - 3 = \frac{z - 2}{-1}, y=1y = 1.
By converting this to vector form, a point on l2l_2 is P(3,1,2)P(3, 1, 2) and its direction vector is d2=(10−1)\mathbf{d}_2 = \begin{pmatrix} 1 \\ 0 \\ -1 \end{pmatrix}.
The line ll has equation r=(−21−1)+μ(10−1)\mathbf{r} = \begin{pmatrix} -2 \\ 1 \\ -1 \end{pmatrix} + \mu \begin{pmatrix} 1 \\ 0 \\ -1 \end{pmatrix}.
Since the direction vectors are identical, line ll and line l2l_2 are parallel.

2. Calculate the displacement vector between points on the two lines and its cross product with the direction vector.

Let A(−2,1,−1)A(-2, 1, -1) be the point on ll corresponding to position vector OA→\overrightarrow{OA}.
The displacement vector from AA to PP is:
AP→=OP→−OA→=(312)−(−21−1)=(503)\overrightarrow{AP} = \overrightarrow{OP} - \overrightarrow{OA} = \begin{pmatrix} 3 \\ 1 \\ 2 \end{pmatrix} - \begin{pmatrix} -2 \\ 1 \\ -1 \end{pmatrix} = \begin{pmatrix} 5 \\ 0 \\ 3 \end{pmatrix}
The cross product of AP→\overrightarrow{AP} with the direction vector d=i−k\mathbf{d} = \mathbf{i} - \mathbf{k} is:
AP→×d=(503)×(10−1)=((0)(−1)−(3)(0)(3)(1)−(5)(−1)(5)(0)−(0)(1))=(080)\overrightarrow{AP} \times \mathbf{d} = \begin{pmatrix} 5 \\ 0 \\ 3 \end{pmatrix} \times \begin{pmatrix} 1 \\ 0 \\ -1 \end{pmatrix} = \begin{pmatrix} (0)(-1) - (3)(0) \\ (3)(1) - (5)(-1) \\ (5)(0) - (0)(1) \end{pmatrix} = \begin{pmatrix} 0 \\ 8 \\ 0 \end{pmatrix}

3. Evaluate the shortest distance using the perpendicular distance formula.

The shortest distance between the two parallel lines is the perpendicular distance from point PP on l2l_2 to line ll:
Distance=∣AP→×d∣∣d∣=02+82+0212+02+(−1)2=82=42\text{Distance} = \frac{|\overrightarrow{AP} \times \mathbf{d}|}{|\mathbf{d}|} = \frac{\sqrt{0^2 + 8^2 + 0^2}}{\sqrt{1^2 + 0^2 + (-1)^2}} = \frac{8}{\sqrt{2}} = 4\sqrt{2}

Answer

424\sqrt{2}

10(d)

1. Express the position vector of $C$ and the displacement vectors $\overrightarrow{BA}$ and $\overrightarrow{BC}$ in terms of $\mu$.

Since CC lies on ll, its position vector OC→\overrightarrow{OC} is:
OC→=(−2+μ1−1−μ)\overrightarrow{OC} = \begin{pmatrix} -2 + \mu \\ 1 \\ -1 - \mu \end{pmatrix}
Next, we find the displacement vectors BA→\overrightarrow{BA} and BC→\overrightarrow{BC}:
BA→=OA→−OB→=(−21−1)−(110)=(−30−1)\overrightarrow{BA} = \overrightarrow{OA} - \overrightarrow{OB} = \begin{pmatrix} -2 \\ 1 \\ -1 \end{pmatrix} - \begin{pmatrix} 1 \\ 1 \\ 0 \end{pmatrix} = \begin{pmatrix} -3 \\ 0 \\ -1 \end{pmatrix}
BC→=OC→−OB→=(−2+μ1−1−μ)−(110)=(−3+μ0−1−μ)\overrightarrow{BC} = \overrightarrow{OC} - \overrightarrow{OB} = \begin{pmatrix} -2 + \mu \\ 1 \\ -1 - \mu \end{pmatrix} - \begin{pmatrix} 1 \\ 1 \\ 0 \end{pmatrix} = \begin{pmatrix} -3 + \mu \\ 0 \\ -1 - \mu \end{pmatrix}

2. Set up the scalar product equation for the perpendicular vectors and solve for $\mu$.

Since angle ABC=90∘ABC = 90^\circ, the vectors BA→\overrightarrow{BA} and BC→\overrightarrow{BC} are perpendicular, which means their scalar product is zero:
BA→⋅BC→=0\overrightarrow{BA} \cdot \overrightarrow{BC} = 0
(−30−1)⋅(−3+μ0−1−μ)=0\begin{pmatrix} -3 \\ 0 \\ -1 \end{pmatrix} \cdot \begin{pmatrix} -3 + \mu \\ 0 \\ -1 - \mu \end{pmatrix} = 0
−3(−3+μ)+0(0)−1(−1−μ)=0-3(-3 + \mu) + 0(0) - 1(-1 - \mu) = 0
9−3μ+1+μ=09 - 3\mu + 1 + \mu = 0
10−2μ=0  ⟹  μ=510 - 2\mu = 0 \implies \mu = 5

3. Substitute $\mu$ back into $\overrightarrow{OC}$ to find the position vector of point $C$.

Substitute μ=5\mu = 5 into the expression for OC→\overrightarrow{OC}:
OC→=(−2+51−1−5)=(31−6)\overrightarrow{OC} = \begin{pmatrix} -2 + 5 \\ 1 \\ -1 - 5 \end{pmatrix} = \begin{pmatrix} 3 \\ 1 \\ -6 \end{pmatrix}
So, the position vector of point CC is 3i+j−6k3\mathbf{i} + \mathbf{j} - 6\mathbf{k}.

Answer

3i+j−6k3\mathbf{i} + \mathbf{j} - 6\mathbf{k}

10(e)

1. Formulate the vector equation of the line passing through $A$ and perpendicular to plane $p_2$.

Let the line be lAFl_{AF}. Since it is perpendicular to p2p_2, its direction vector is the normal vector of p2p_2, which is n=(111)\mathbf{n} = \begin{pmatrix} 1 \\ 1 \\ 1 \end{pmatrix}.

The vector equation of the line is:
lAF:r=(−21−1)+λ(111), where λ∈Rl_{AF}: \mathbf{r} = \begin{pmatrix} -2 \\ 1 \\ -1 \end{pmatrix} + \lambda \begin{pmatrix} 1 \\ 1 \\ 1 \end{pmatrix}, \text{ where } \lambda \in \mathbb{R}

2. Substitute the line equation into the plane equation to find the value of the parameter $\lambda$ at the intersection.

The equation of p2p_2 is r⋅(111)=2\mathbf{r} \cdot \begin{pmatrix} 1 \\ 1 \\ 1 \end{pmatrix} = 2. Substitute lAFl_{AF} into p2p_2:
[(−21−1)+λ(111)]⋅(111)=2\left[ \begin{pmatrix} -2 \\ 1 \\ -1 \end{pmatrix} + \lambda \begin{pmatrix} 1 \\ 1 \\ 1 \end{pmatrix} \right] \cdot \begin{pmatrix} 1 \\ 1 \\ 1 \end{pmatrix} = 2
(−21−1)⋅(111)+λ(111)⋅(111)=2\begin{pmatrix} -2 \\ 1 \\ -1 \end{pmatrix} \cdot \begin{pmatrix} 1 \\ 1 \\ 1 \end{pmatrix} + \lambda \begin{pmatrix} 1 \\ 1 \\ 1 \end{pmatrix} \cdot \begin{pmatrix} 1 \\ 1 \\ 1 \end{pmatrix} = 2
(−2+1−1)+λ(1+1+1)=2(-2 + 1 - 1) + \lambda(1 + 1 + 1) = 2
−2+3λ=2-2 + 3\lambda = 2
3λ=4  ⟹  λ=433\lambda = 4 \implies \lambda = \frac{4}{3}

3. Calculate the position vector of the foot of the perpendicular.

Substitute λ=43\lambda = \frac{4}{3} back into the equation of the line lAFl_{AF} to find the position vector of the foot of the perpendicular, FF:
OF→=(−21−1)+43(111)=(−2+4/31+4/3−1+4/3)=(−2/37/31/3)\overrightarrow{OF} = \begin{pmatrix} -2 \\ 1 \\ -1 \end{pmatrix} + \frac{4}{3} \begin{pmatrix} 1 \\ 1 \\ 1 \end{pmatrix} = \begin{pmatrix} -2 + 4/3 \\ 1 + 4/3 \\ -1 + 4/3 \end{pmatrix} = \begin{pmatrix} -2/3 \\ 7/3 \\ 1/3 \end{pmatrix}

Expressing in terms of i\mathbf{i}, j\mathbf{j}, and k\mathbf{k}:
OF→=−23i+73j+13k\overrightarrow{OF} = -\frac{2}{3}\mathbf{i} + \frac{7}{3}\mathbf{j} + \frac{1}{3}\mathbf{k}

Answer

−23i+73j+13k-\frac{2}{3}\mathbf{i} + \frac{7}{3}\mathbf{j} + \frac{1}{3}\mathbf{k}

10(f)

1. Find the position vector of the foot of perpendicular $F$ from $A$ to $p_2$ (expected from part e).

Let the normal to plane p2p_2 be n=(111)\mathbf{n} = \begin{pmatrix} 1 \\ 1 \\ 1 \end{pmatrix}.
The equation of the line passing through AA and perpendicular to p2p_2 is:
r=(−21−1)+λ(111)\mathbf{r} = \begin{pmatrix} -2 \\ 1 \\ -1 \end{pmatrix} + \lambda \begin{pmatrix} 1 \\ 1 \\ 1 \end{pmatrix}
Substitute this into the equation of p2p_2 (x+y+z=2x + y + z = 2) to find the intersection:
(−2+λ)+(1+λ)+(−1+λ)=2(-2 + \lambda) + (1 + \lambda) + (-1 + \lambda) = 2
3λ−2=2  ⟹  λ=433\lambda - 2 = 2 \implies \lambda = \frac{4}{3}
The position vector of the foot of perpendicular FF is:
OF→=(−21−1)+43(111)=(−2/37/31/3)\overrightarrow{OF} = \begin{pmatrix} -2 \\ 1 \\ -1 \end{pmatrix} + \frac{4}{3} \begin{pmatrix} 1 \\ 1 \\ 1 \end{pmatrix} = \begin{pmatrix} -2/3 \\ 7/3 \\ 1/3 \end{pmatrix}
(Note: This calculation is typically completed in part (e) and can be carried forward directly).

2. Determine the equation of $p_3$ by finding the midpoint between $A$ and $F$.

For plane p3p_3 to be equidistant to point AA and plane p2p_2 with a strictly non-zero distance, it must be parallel to p2p_2 and pass through the midpoint MM of AA and FF.
The position vector of MM is:
OM→=OA→+OF→2=12[(−21−1)+(−2/37/31/3)]=(−4/35/3−1/3)\overrightarrow{OM} = \frac{\overrightarrow{OA} + \overrightarrow{OF}}{2} = \frac{1}{2} \left[ \begin{pmatrix} -2 \\ 1 \\ -1 \end{pmatrix} + \begin{pmatrix} -2/3 \\ 7/3 \\ 1/3 \end{pmatrix} \right] = \begin{pmatrix} -4/3 \\ 5/3 \\ -1/3 \end{pmatrix}
Since p3p_3 is parallel to p2p_2, its normal vector is also n=(111)\mathbf{n} = \begin{pmatrix} 1 \\ 1 \\ 1 \end{pmatrix}.
The scalar product equation of p3p_3 is r⋅n=OM→⋅n\mathbf{r} \cdot \mathbf{n} = \overrightarrow{OM} \cdot \mathbf{n}:
r⋅(111)=(−4/35/3−1/3)⋅(111)=−43+53−13=0\mathbf{r} \cdot \begin{pmatrix} 1 \\ 1 \\ 1 \end{pmatrix} = \begin{pmatrix} -4/3 \\ 5/3 \\ -1/3 \end{pmatrix} \cdot \begin{pmatrix} 1 \\ 1 \\ 1 \end{pmatrix} = -\frac{4}{3} + \frac{5}{3} - \frac{1}{3} = 0
Thus, the cartesian equation of p3p_3 is x+y+z=0x + y + z = 0.

Answer

x+y+z=0x + y + z = 0

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