The equations of three planes p1,p2,p3p_1, p_2, p_3 are 2x−4y+z=6,2x-4y+z=6, x+y−z=6,x+y-z=6, ax−2y−z=b,ax-2y-z=b, respectively, where aa and bb are constants. The planes p1p_1 and p2p_2 meet in a line ll.

  1. ((i))

    Find a vector equation of ll.

  2. ((ii))

    Given that the system of equations

    2x−4y+z=6,2x-4y+z=6,

    x+y−z=6,x+y-z=6,

    ax−2y−z=b,ax-2y-z=b,

    has an infinite number of solutions, find aa and bb.

  3. ((iii))

    Find, in the form r.n=pr.n = p, the equation of the plane which passes through the point (1,1,1)(1,1,1) and is perpendicular to both p1p_1 and p2p_2.

  4. ((iv))

    The plane p4p_4 meets p2p_2 in a line mm which passes through the point (3,4,1)(3,4,1) and p1,p2,p4p_1, p_2, p_4 have no point in common. Find the perpendicular distance between the lines ll and mm, giving your answer in an exact form.

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Worked solution

4((i))

1. Find the direction vector of the line $l$ by calculating the cross product of the normal vectors of $p_1$ and $p_2$.

The normal vectors of p1p_1 and p2p_2 are n1=(2−41)\mathbf{n}_1 = \begin{pmatrix} 2 \\ -4 \\ 1 \end{pmatrix} and n2=(11−1)\mathbf{n}_2 = \begin{pmatrix} 1 \\ 1 \\ -1 \end{pmatrix}.

The direction vector of the line ll is parallel to n1×n2\mathbf{n}_1 \times \mathbf{n}_2:
d=(2−41)×(11−1)=((−4)(−1)−(1)(1)(1)(1)−(2)(−1)(2)(1)−(−4)(1))=(336)\mathbf{d} = \begin{pmatrix} 2 \\ -4 \\ 1 \end{pmatrix} \times \begin{pmatrix} 1 \\ 1 \\ -1 \end{pmatrix} = \begin{pmatrix} (-4)(-1) - (1)(1) \\ (1)(1) - (2)(-1) \\ (2)(1) - (-4)(1) \end{pmatrix} = \begin{pmatrix} 3 \\ 3 \\ 6 \end{pmatrix}

This direction vector can be scaled down to (112)\begin{pmatrix} 1 \\ 1 \\ 2 \end{pmatrix}.

2. Find the coordinates of a specific point that lies on both planes.

Let z=0z = 0. The plane equations then simplify to:
2x−4y=62x - 4y = 6
x+y=6x + y = 6

From the second equation, x=6−yx = 6 - y. Substituting this into the first equation:
2(6−y)−4y=62(6 - y) - 4y = 6
12−2y−4y=612 - 2y - 4y = 6
6y=6  ⟹  y=16y = 6 \implies y = 1
Then x=6−1=5x = 6 - 1 = 5.

A common point on both planes (and therefore on ll) is (5,1,0)(5, 1, 0).

3. State the vector equation of the line $l$.

Using the point (5,1,0)(5, 1, 0) and the simplified direction vector (112)\begin{pmatrix} 1 \\ 1 \\ 2 \end{pmatrix}:
r=(510)+λ(112),λ∈R\mathbf{r} = \begin{pmatrix} 5 \\ 1 \\ 0 \end{pmatrix} + \lambda \begin{pmatrix} 1 \\ 1 \\ 2 \end{pmatrix}, \lambda \in \mathbb{R}

Answer

r=(510)+λ(112),λ∈R\mathbf{r} = \begin{pmatrix} 5 \\ 1 \\ 0 \end{pmatrix} + \lambda \begin{pmatrix} 1 \\ 1 \\ 2 \end{pmatrix}, \lambda \in \mathbb{R}

4((ii))

1. Reduce the system of equations by eliminating $x$ from the second and third equations.

Let the equations be:
(1) x+y−z=6x + y - z = 6
(2) 2x−4y+z=62x - 4y + z = 6
(3) ax−2y−z=bax - 2y - z = b

We eliminate xx from equations (2) and (3) using equation (1).
Take (2) −2×- 2 \times (1):
(2x−4y+z)−2(x+y−z)=6−2(6)(2x - 4y + z) - 2(x + y - z) = 6 - 2(6)
−6y+3z=−6— (4)-6y + 3z = -6 \quad \text{--- (4)}

Take (3) −a×- a \times (1):
(ax−2y−z)−a(x+y−z)=b−6a(ax - 2y - z) - a(x + y - z) = b - 6a
(−2−a)y+(a−1)z=b−6a— (5)(-2-a)y + (a-1)z = b - 6a \quad \text{--- (5)}

2. Apply the condition for infinite solutions to find $a$.

For the 3x3 system to have an infinite number of solutions (intersecting in a line), the remaining equations after eliminating one variable must be dependent. This means equation (5) must be proportional to equation (4).

By comparing the ratio of their coefficients:
−2−a−6=a−13=b−6a−6\frac{-2-a}{-6} = \frac{a-1}{3} = \frac{b-6a}{-6}

Using the first equality to solve for aa:
−2−a−6=a−13\frac{-2-a}{-6} = \frac{a-1}{3}
−2−a=−2(a−1)-2 - a = -2(a - 1)
−2−a=−2a+2-2 - a = -2a + 2
a=4a = 4

3. Use the value of $a$ and the proportional relationship to find $b$.

Substitute a=4a = 4 into the second equality to solve for bb:
4−13=b−6(4)−6\frac{4-1}{3} = \frac{b-6(4)}{-6}
33=b−24−6\frac{3}{3} = \frac{b - 24}{-6}
1=b−24−61 = \frac{b - 24}{-6}
−6=b−24-6 = b - 24
b=18b = 18

Answer

a=4,b=18a = 4, b = 18

4((iii))

1. Find the normal vector to the plane by calculating the cross product of the normal vectors of $p_1$ and $p_2$.

Let the normal vectors of p1p_1 and p2p_2 be n1\mathbf{n}_1 and n2\mathbf{n}_2 respectively.
n1=(2−41),n2=(11−1)\mathbf{n}_1 = \begin{pmatrix} 2 \\ -4 \\ 1 \end{pmatrix}, \quad \mathbf{n}_2 = \begin{pmatrix} 1 \\ 1 \\ -1 \end{pmatrix}
Since the required plane is perpendicular to both p1p_1 and p2p_2, its normal vector n\mathbf{n} must be perpendicular to both n1\mathbf{n}_1 and n2\mathbf{n}_2, meaning it is parallel to their cross product.
n1×n2=(2−41)×(11−1)=((−4)(−1)−(1)(1)(1)(1)−(2)(−1)(2)(1)−(−4)(1))=(336)\mathbf{n}_1 \times \mathbf{n}_2 = \begin{pmatrix} 2 \\ -4 \\ 1 \end{pmatrix} \times \begin{pmatrix} 1 \\ 1 \\ -1 \end{pmatrix} = \begin{pmatrix} (-4)(-1) - (1)(1) \\ (1)(1) - (2)(-1) \\ (2)(1) - (-4)(1) \end{pmatrix} = \begin{pmatrix} 3 \\ 3 \\ 6 \end{pmatrix}
We can factor out 33 to choose a simpler normal vector for our plane, so let n=(112)\mathbf{n} = \begin{pmatrix} 1 \\ 1 \\ 2 \end{pmatrix}.

2. Use the given point to find the scalar constant $p$ and write the final equation of the plane.

The required plane passes through the point with position vector a=(111)\mathbf{a} = \begin{pmatrix} 1 \\ 1 \\ 1 \end{pmatrix}.
The equation of the plane in scalar product form is r⋅n=a⋅n\mathbf{r} \cdot \mathbf{n} = \mathbf{a} \cdot \mathbf{n}.
r⋅(112)=(111)⋅(112)\mathbf{r} \cdot \begin{pmatrix} 1 \\ 1 \\ 2 \end{pmatrix} = \begin{pmatrix} 1 \\ 1 \\ 1 \end{pmatrix} \cdot \begin{pmatrix} 1 \\ 1 \\ 2 \end{pmatrix}
r⋅(112)=(1)(1)+(1)(1)+(1)(2)=4\mathbf{r} \cdot \begin{pmatrix} 1 \\ 1 \\ 2 \end{pmatrix} = (1)(1) + (1)(1) + (1)(2) = 4

Answer

r⋅(112)=4\mathbf{r} \cdot \begin{pmatrix} 1 \\ 1 \\ 2 \end{pmatrix} = 4

4((iv))

1. Deduce the geometrical relationship between lines $l$ and $m$.

Since ll is the intersection of p1p_1 and p2p_2, and mm is the intersection of p4p_4 and p2p_2, both lines ll and mm lie completely in the plane p2p_2.
If ll and mm were to intersect at a point, this point would lie in p1p_1, p2p_2, and p4p_4. However, we are given that p1,p2,p_1, p_2, and p4p_4 have no point in common.
Therefore, ll and mm cannot intersect. Since they are coplanar and non-intersecting, they must be parallel lines (l∥ml \parallel m).

2. Find a displacement vector between a point on $l$ and the given point on $m$.

From part (i), the equation of line ll is r=(510)+λ(112)\mathbf{r} = \begin{pmatrix} 5 \\ 1 \\ 0 \end{pmatrix} + \lambda \begin{pmatrix} 1 \\ 1 \\ 2 \end{pmatrix}.
Let B(5,1,0)B(5, 1, 0) be a point on ll. The direction vector of ll (and therefore mm) is d=(112)\mathbf{d} = \begin{pmatrix} 1 \\ 1 \\ 2 \end{pmatrix}.
Let A(3,4,1)A(3, 4, 1) be the given point on mm.
The displacement vector from BB to AA is:
BA⃗=(341)−(510)=(−231)\vec{BA} = \begin{pmatrix} 3 \\ 4 \\ 1 \end{pmatrix} - \begin{pmatrix} 5 \\ 1 \\ 0 \end{pmatrix} = \begin{pmatrix} -2 \\ 3 \\ 1 \end{pmatrix}

3. Calculate the perpendicular distance between the parallel lines $l$ and $m$.

The perpendicular distance dd from point AA to line ll is given by d=∣BA⃗×d∣∣d∣d = \frac{|\vec{BA} \times \mathbf{d}|}{|\mathbf{d}|}.
BA⃗×d=(−231)×(112)=((3)(2)−(1)(1)(1)(1)−(−2)(2)(−2)(1)−(3)(1))=(55−5)\vec{BA} \times \mathbf{d} = \begin{pmatrix} -2 \\ 3 \\ 1 \end{pmatrix} \times \begin{pmatrix} 1 \\ 1 \\ 2 \end{pmatrix} = \begin{pmatrix} (3)(2) - (1)(1) \\ (1)(1) - (-2)(2) \\ (-2)(1) - (3)(1) \end{pmatrix} = \begin{pmatrix} 5 \\ 5 \\ -5 \end{pmatrix}
d=52+52+(−5)212+12+22=756=536=52=522d = \frac{\sqrt{5^2 + 5^2 + (-5)^2}}{\sqrt{1^2 + 1^2 + 2^2}} = \frac{\sqrt{75}}{\sqrt{6}} = \frac{5\sqrt{3}}{\sqrt{6}} = \frac{5}{\sqrt{2}} = \frac{5\sqrt{2}}{2}

Answer

522\frac{5\sqrt{2}}{2}

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