Transformed Parabola

Geometry Level pending

A parabola in the x y xy plane is given by v = 1 4 u 2 v = \dfrac{1}{4} u^2 , where the coordinates ( x , y ) (x, y) are related to the ( u , v ) (u,v) coordinates by

[ x y ] = R [ u v ] + [ 5 2 ] \begin{bmatrix} x \\ y \end{bmatrix} = R \begin{bmatrix} u \\ v \end{bmatrix} + \begin{bmatrix} 5 \\ 2 \end{bmatrix}

and R R is the 2 × 2 2 \times 2 rotation matrix by 3 0 30^\circ counter clockwise, i.e.

R = [ cos 3 0 sin 3 0 sin 3 0 cos 3 0 ] R =\begin{bmatrix} \cos 30^\circ && -\sin 30^\circ \\ \sin 30^\circ && \cos 30^\circ \end{bmatrix}

Now, you apply the following transformation to the points on the parabola.

If p p is a point on the parabola, you define its image p p' as follows:

p = A p + b p' = A p + b

where

A = [ 1 3 0 2 ] , b = [ 1 4 ] A = \begin{bmatrix} 1 && -3 \\ 0 && 2 \end{bmatrix} , \hspace{24pt} b = \begin{bmatrix} 1 \\ - 4 \end{bmatrix}

Given that the image of the parabola is another parabola, find the vertex of the new parabola and the direction of its axis. Let r 0 = ( r 0 x , r 0 y ) r_0 = (r_{0x}, r_{0y} ) be the vertex and u = ( cos θ , sin θ ) u = ( \cos \theta , \sin \theta ) ( θ \theta in radians, 0 θ < 2 π 0 \le \theta \lt 2 \pi ) be the unit vector along the axis pointing in the direction that the parabola opens up. Further, and just as important, by attaching a suitable reference coordinate frame O x y O' x' y' to the new parabola, where O O' is at the vertex, its equation can be written as

y = a x 2 y' = a {x'}^2

with a > 0 a \gt 0

Find 4 ( r 0 x r 0 y ) + θ + a 4(r_{0x} - r_{0y}) + \theta + a


The answer is 7.5986.

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1 solution

Hosam Hajjir
May 2, 2021

Here's an outline of one possible solution method that depends on parametric equations.

The coordinate vector in the u v uv reference frame is given parametrically by ( t , 1 4 t 2 ) = t ( 1 , 0 ) + t 2 ( 0 , 1 4 ) (t, \dfrac{1}{4} t^2) = t (1, 0) + t^2 (0, \dfrac{1}{4})

Hence the coordinate vector in the x y xy plane is given by

p = ( x , y ) = R ( u , v ) + ( 5 , 2 ) = R ( t ( 1 , 0 ) + t 2 ( 0 , 1 4 ) ) + ( 5 , 2 ) p = (x, y) = R (u,v) + (5, 2) = R ( t (1, 0) + t^2 (0, \dfrac{1}{4} ) )+ (5, 2)

Note that ordered pairs are actually 2 × 1 2 \times 1 column vectors. Next apply the transformation to obtain

p = A p + b = A ( t R ( 1 , 0 ) + t 2 R ( 0 , 1 4 ) + ( 5 , 2 ) ) + b p' = A p + b = A ( t R (1, 0) + t^2 R (0, \dfrac{1}{4} ) + (5, 2) ) + b

and this can be written as

p = v 0 + v 1 t + v 2 t 2 ( 1 ) p' = v_0 + v_1 t + v_2 t^2 \hspace{12pt} (1) ,

with v 0 = A ( 5 , 2 ) + b , v 1 = A R ( 1 , 0 ) , v 2 = A R ( 0 , 1 4 ) v_0 = A (5, 2) + b , v_1 = A R (1, 0) , v_2 = A R (0, \dfrac{1}{4} )

Equation ( 1 ) (1) can be written as

p = u 0 + c 1 u 1 ( t + t 0 ) + c 2 u 2 ( t + t 0 ) 2 ( 2 ) p' = u_0 + c_1 u_1 (t + t_0) + c_2 u_2 (t + t_0)^2 \hspace{12pt} (2)

where u 1 u_1 and u 2 u_2 are unit vectors and mutually perpendicular to each other.

Expanding ( 2 ) (2) and equating similar terms, results in,

v 0 = u 0 + c 1 u 1 t 0 + c 2 u 2 t 0 2 ( 3 ) v_0 = u_0 + c_1 u_1 t_0 + c_2 u_2 t_0^2 \hspace{16pt} (3)

v 1 = c 1 u 1 + 2 c 2 u 2 t 0 ( 4 ) v_1 = c_1 u_1 + 2 c_2 u_2 t_0 \hspace{16pt} (4)

v 2 = c 2 u 2 ( 5 ) v_2 = c_2 u_2 \hspace{16pt} (5)

Equation ( 5 ) (5) determines u 2 u_2 and c 2 c_2 , as c 2 = v 2 c_2 = | v_2 | , and u 2 = v 2 / c 2 u_2 = v_2 / c_2

This also determines u 1 u_1 as a unit vector that is perpendicular to u 2 u_2 .

Next, from equation ( 4 ) (4) , by dot multiplying both sides with u 1 u_1 , we obtain

v 1 u 1 = c 1 v_1 \cdot u_1 = c_1

and by dot multiplying both sides with u 2 u_2 , we obtain

v 1 u 2 = 2 c 2 t 0 v_1 \cdot u_2 = 2 c_2 t_0

hence c 1 c_1 and t 0 t_0 are now determined. Finally u 0 u_0 can be computed from equation ( 3 ) (3) .

The vertex is u 0 u_0 , θ \theta is the angle of u 2 u_2 , and a = c 2 c 1 2 a = \dfrac{c_2}{{c_1}^2}

Performing these calculations gives us r 0 = u 0 = ( 0.105328239 , 0.437689286 ) r_0 = u_0 = (0.105328239,-0.437689286 ) , u 2 = ( 0.872850734 , 0.487987291 ) u_2 = (-0.872850734, 0.487987291) , and a = 2.794707525 a = 2.794707525

Hence, θ = 2.631810294 \theta = 2.631810294 , and 4 ( r 0 x r 0 y ) + θ + a = 7.598587919 7.5986 4(r_{0x} - r_{0y} ) + \theta + a = 7.598587919 \approx \boxed{7.5986 }

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