Reflection of an Incident Ray Across a Mirror

Geometry Level 4

A mirror strip extends along the line 2 x 3 y + 15 = 0 2 x - 3 y + 15 = 0 . A light ray is directed towards the mirror from the point ( 10 , 0 ) (10, 0) . If the reflected ray passes through the point ( 10 , 10 ) (10, 10) , what is the equation of the original incident ray?

y = 5 ( x 10 ) y = -5(x - 10) y = 6 ( x 10 ) y = -6(x - 10) y = 8 ( x 10 ) y = -8(x - 10) y = 10 ( x 10 ) y = -10(x - 10)

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2 solutions

Michael Huang
Oct 21, 2017

The given problem is related to the past weekly problem .

For the ray to project from the point of collision to the target, the line passing through point ( 10 , 10 ) (10,10) must be parallel to the line of equation 2 x 3 y + 15 = 0 2x - 3y + 15 = 0 , so that the lines of equation β 1 \beta_1 and β 2 \beta_2 are equidistant from the bolded lines. Using the standard form of the linear equation A x + B y + C = 0 Ax + By + C = 0 , A A and B B are same for both equations β 1 \beta_1 and β 2 \beta_2 . The only values that are different involve the C C variable, which shifts the equation vertically with respect to B B . With that being said,

  • Equation β 1 \beta_1 passing through ( 10 , 10 ) (10,10) is 2 x 3 y + 10 = 0 2x - 3y + 10 = 0 .
  • Because of A , B , C A,B,C -linearity, Equation β 2 \beta_2 is 2 x 3 y + 15 + ( 15 10 ) = 2 x 3 y + 20 = 0 2x - 3y + 15 + (15 - 10) = 2x - 3y + 20 = 0 .

Mirroring point ( 10 , 10 ) (10,10) past the bolded line shows that the line of equation α 2 \alpha_2 is perpendicular to these 3 lines. So equation α 2 \alpha_2 is 3 x + 2 y + 50 = 0 3x + 2y + 50 = 0 , which passes through point ( 10 , 10 ) (10,10) . With equations α 2 \alpha_2 and β 2 \beta_2 , we can determine their point of arrival, which is the intersection point ( 110 13 , 160 13 ) \left(\frac{110}{13}, \frac{160}{13}\right) .

So the answer is y = 8 ( x 10 ) \boxed{y = -8(x - 10)} , which is easily found by computing the equation passing through ( 10 , 0 ) (10,0) and the image point.

Hosam Hajjir
Oct 22, 2017

Let P = ( 10 , 0 ) P = (10, 0) and Q = ( 10 , 10 ) Q = (10, 10) . Since Q Q lies on the reflected ray, then its reflection across the mirror lies on the extension of the original ray (behind the mirror). So, the only thing to this problem is to find the image Q Q' under reflection across the given line. There is a standard formula for this computation, and it is as follows. Let the mirror line equation be M ( r r 0 ) = 0 M \cdot (r - r_0 ) = 0 where r , r 0 r , r_0 , and M M are two-dimensional vectors, with r = ( x , y ) T r = (x, y)^T , r 0 = ( x 0 , y 0 ) T r_0 = (x_0, y_0)^T is any point that lies on the mirror line, and M M is the normal to the line. For the given equation, M = ( 2 , 3 ) T M = (2, -3)^T , and we can take r 0 = ( 0 , 5 ) T r_0 = (0, 5)^T . Now the formula for finding the image of point Q Q is:

Q = r 0 + ( I 2 M M T M T M ) ( Q r 0 ) Q' = r_0 + (I - 2 \dfrac{M M^T}{ M^T M } ) (Q - r_0 )

where I I is the 2 × 2 2 \times 2 identity matrix. Using the given value of the vector M M , we obtain

M T M = ( 2 , 3 ) ( 2 , 3 ) T = 13 M^T M = (2, -3) (2, -3)^T = 13 , and

M M T = [ 2 3 ] [ 2 3 ] = [ 4 6 6 9 ] M M^T = \begin{bmatrix} 2 \\ -3 \end{bmatrix} \begin{bmatrix} 2 && -3 \end{bmatrix} = \begin{bmatrix} 4 && -6 \\ -6 && 9 \end{bmatrix}

Therefore,

I 2 M M T M T M = [ 1 0 0 1 ] 2 13 [ 4 6 6 9 ] = 1 13 [ 5 12 12 5 ] I - 2 \dfrac{M M^T}{ M^T M } = \begin{bmatrix} 1 && 0 \\ 0 && 1 \end{bmatrix} - \dfrac{2}{13}\begin{bmatrix} 4 && -6 \\ -6 && 9 \end{bmatrix} = \dfrac{1}{13} \begin{bmatrix} 5 && 12 \\ 12 && -5 \end{bmatrix}

Therefore,

Q = ( 0 , 5 ) T + 1 13 [ 5 12 12 5 ] ( ( 10 , 10 ) ( 0 , 5 ) ) T Q' = (0, 5)^T + \dfrac{1}{13} \begin{bmatrix} 5 && 12 \\ 12 && -5 \end{bmatrix} ( (10, 10) - (0, 5) )^T

Performing the above computation, results in,

Q = ( 110 13 , 160 13 ) Q' = ( \dfrac{110}{13}, \dfrac{160}{13} )

What is left is to find an equation of the line passing through P P and Q Q' . The slope is given by

m = ( 160 13 0 ) 110 13 10 = 160 20 = 8 m = \dfrac{ ( \dfrac{160}{13} - 0 ) } { \dfrac{110}{13} - 10 } = \dfrac{ 160 }{-20}= -8

Therefore, the equation of the line (using point-slope formulation) is y = 8 ( x 10 ) y = -8 (x - 10) .

Yet another way to do this problem is to write the incident ray line in parametric form as follows

r = P + t d r = P + t d

where d d is a direction vector, and t t is an arbitrary real parameter, then the reflected ray will have the equation

r = r 0 + ( I 2 M M T M T M ) ( r r 0 ) r' = r_0 + (I - 2 \dfrac{M M^T}{ M^T M } ) (r - r_0)

Substituting r = P + t d r = P + t d

r = r 0 + ( I 2 M M T M T M ) ( P r 0 + t d ) r' = r_0 + (I - 2 \dfrac{M M^T}{ M^T M } ) ( P - r_0 + t d)

Since Q lies on the reflected ray, then

Q = r 0 + ( I 2 M M T M T M ) ( P r 0 + t d ) Q = r_0 + (I - 2 \dfrac{M M^T}{ M^T M } ) (P - r_0 + t d)

for some t. Noting that the inverse of ( I 2 M M T M T M ) (I - 2 \dfrac{M M^T}{ M^T M } ) is itself, it follows that

( I 2 M M T M T M ) ( Q r 0 ) ( P r 0 ) = t d (I - 2 \dfrac{M M^T}{ M^T M } ) (Q - r_0) - (P - r_0) = t d

From which the direction of d can be determined..

Evaluating the expression above, results in

1 13 [ 5 12 12 5 ] ( ( 10 , 10 ) ( 0 , 5 ) ) ( ( 10 , 0 ) ( 0 , 5 ) ) = t d \dfrac{1}{13} \begin{bmatrix} 5 && 12 \\ 12 && -5 \end{bmatrix} ( (10,10) - (0, 5) ) - ( (10, 0) - (0, 5) ) = t d

( 20 13 , 160 13 ) = t d ( \dfrac{-20}{13} , \dfrac{160}{13} ) = t d

Therefore, vector d d can be taken as ( 1 , 8 ) (-1, 8) . And the equation of the incident ray becomes,

r = ( 10 , 0 ) + t ( 1 , 8 ) r = (10, 0) + t (-1, 8)

Pre-multiplying by an orthogonal vector to ( 1 , 8 ) (-1,8) , for example , ( 8 , 1 ) (8, 1 ) , results in the algebraic equation of the line,

( 8 , 1 ) T r = 8 x + y = 80 (8, 1)^T r = 8 x + y = 80 , hence y = 8 x + 80 = 8 ( x 10 ) y = -8 x + 80 = -8 (x - 10) .

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