A home interior designer is looking to design a pull-down wardrobe lift. To test his concept, the designer built a small-scale model of it, in which points are defined relative to a corner of the model at . The rods used in the model can be modelled by equations of straight lines. The main rod can be modelled by the line with equation . Another rod, line , passes through the points and .
- (a)
A supporting wire connects to a point on such that is perpendicular to . Find the position vector of .
- (b)
A retractable rod, line , is placed such that it can be modelled by reflecting about . Find a vector equation of .
- (c)
The panels of the small-scale model can be modelled by equations of planes. The main panel, plane , contains the main rod and an attachment point . A side panel, plane , can be represented by the equation .
Show that can be represented by the cartesian equation .
- (d)
A structural rod, line , needs to be placed at the intersection between and . Find a vector equation of .
- (e)
A decorative plank, plane , has equation , where . If the distance between and is exactly units, find the possible values of and .
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Worked solution
9(a)
1. Express the position vector of $F$ in terms of a parameter and find the displacement vector $\overrightarrow{BF}$.
Since lies on , let its position vector be .
The displacement vector is:
2. Apply the condition that $\overrightarrow{BF}$ is perpendicular to $l_1$ to solve for $\lambda$.
Since is perpendicular to , its scalar product with the direction vector of is .
3. Substitute the value of $\lambda$ to find the position vector of $F$.
Substitute back into the expression for :
9(b)
1. Find the position vector of $F$ on $l_1$ such that $\overrightarrow{BF}$ is perpendicular to $l_1$ (as required from part a).
Let be a point on with position vector .
Since is perpendicular to :
2. Find the position vector of $B'$, the reflection of point $B$ about $l_1$.
The point is the midpoint of the line segment connecting and its reflection .
3. State the intersection point $A$ and find the vector equation of the reflected line $l_R$.
The point matches the fixed point in the equation of (when ), meaning is the intersection point of and . Therefore, reflects to itself and lies on .
The direction vector of is given by:
The vector equation of , passing through with direction , is:
9(c)
1. Find a second direction vector on the plane by finding the displacement vector between a point on $l_1$ and $C$.
Let be a point on .
2. Calculate the cross product of the direction vector of $l_1$ and $\overrightarrow{CA}$ to find a normal vector to the plane.
Let be the direction vector of .
A simpler normal vector is .
3. Formulate the cartesian equation of the plane using the scalar product equation.
Thus, the cartesian equation is (Shown).
(Shown)
9(d)
1. Find the direction vector of the line of intersection by taking the cross product of the normal vectors of the two planes.
The normal vector of is and the normal vector of is .
The direction vector of the line of intersection is perpendicular to both normal vectors:
We can scale this vector by a factor of to obtain a simpler direction vector: .
2. Find a common point that lies on both planes.
We need to find a coordinate point that satisfies the equations of both planes:
By letting , the equations simplify to:
Substitute into the second equation:
Substituting back gives .
So, a common point on both planes is .
(Note: This is the attachment point given in part (c), which can be checked directly against the equation of .)
3. Write the vector equation of the line $l_S$.
Using the position vector of the common point and the direction vector, the vector equation of the structural rod is:
9(e)
1. Deduce the value of $\alpha$ by recognising that the planes must be parallel.
Since the distance between planes and is exactly units everywhere, the two planes must not intersect, meaning they are parallel. Thus, their normal vectors are scalar multiples of each other:
Comparing the -components or -components, we find .
Therefore, comparing the -components:
2. Formulate an equation for the distance between the parallel planes.
With , the equation of is .
Dividing by 3 gives an equation with the exact same normal vector as from part (c):
The distance between the parallel planes and is:
3. Solve for the possible values of $\beta$.
Equating the distance to and using :
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