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| 12 Theory slides |
| 10 Exercises - Grade E - A |
| Each lesson is meant to take 1-2 classroom sessions |
Here is some recommended reading before getting started with this lesson.
From the exploration, the following conclusions can be drawn.
To perform a translation, a vector is required. This implies that the direction of the translation plays an important role. To illustrate this statement, consider the following diagram.
Consequently, and referring to what can be inferred from the exploration applet, a third conclusion can be drawn.
The vectors AA′, BB′, and CC′ have the same direction as v.
Be aware that the three conclusions written before do not depend on the preimage. They hold true even when the preimage is a single point, a segment, a polygon, or any other figure. Then, these properties can be used to define a translation properly.
A translation is a transformation that moves every point of a figure the same distance in the same direction. More precisely, a translation along a vector v maps every point A in the plane onto its image A′ such that the following statements hold true.
As the previous exploration shows, translations preserve side lengths and angle measures. That confirms translations are rigid motions. Additionally, take note that translations map segments onto parallel segments. Consider the polygon P shown in the middle of the diagram below. The other polygons are images of P after different transformations.
What polygons are the image of P after a translation?
Only polygons P4, P6, and P14 are the image of P after a translation.
Remember that translations map segments onto parallel segments. Since P looks like an arrow pointing up, the images of P after a translation will also look like an arrow pointing up.
Since translations map segments onto parallel segments, the sides of P are parallel to the sides of its image after any translation. Notice that P looks like an arrow pointing up.
In the previous example, only the shape of polygon P was used to determine which polygons were the image of P after a translation. When the vertices are labeled, keep an eye on them. Consider the following three squares.
Therefore, S2 is not the image of PQRS after a translation. Conversely, S1 satisfies the two conditions previously written. Even more, since every vector that connects a vertex to its image have the same direction, it can be concluded that S1 is a translation of PQRS.
Translations can be performed by hand with the help of a straightedge and a compass.
To translate △ABC along v follow the four steps below.
Draw parallel lines to ℓ through each vertex.
Draw the triangle formed by the image points A′, B′, and C′.
By definition of translation, vectors AA′ and v are parallel and have the same magnitude and direction. This makes PAA′Q a parallelogram. With this in mind, the translation of △ABC can be performed as follows.
In the following applet, one of the following tasks may be required.
To translate △ABC, place points A′, B′, and C′ where they should be after the translation is applied.
When learning about rotations, it was said that the composition of two rotations could be a translation. Now, the composition of two translations will be examined.
Consider the following pair of quadrilaterals P1 and P2. Also, consider a pair of different translations. One translation along vector u=⟨5,1⟩ and the other along v=⟨-2,-4⟩.
Translating Along | Is Equivalent To |
---|---|
u=⟨5,1⟩ | Translating 5 units to the right and 1 unit up. |
v=⟨-2,-4⟩ | Translating 2 units to the left and 4 unit down. |
All the vectors drawn seem to be parallel and with the same magnitude. Even more, they all have the same direction. This could be checked by finding the component form of each vector.
Vertex | Image | Vector | Component Form |
---|---|---|---|
(-4,0) | (-1,-3) | ⟨-1−(-4),-3−0⟩ | ⟨3,-3⟩ |
(-1,1) | (2,-2) | ⟨2−(-1),-2−1⟩ | ⟨3,-3⟩ |
(-1,2) | (2,-1) | ⟨2−(-1),-1−2⟩ | ⟨3,-3⟩ |
(-3,3) | (0,0) | ⟨0−(-3),0−3⟩ | ⟨3,-3⟩ |
As the table shows, all the vectors connecting a preimage with its image have the same component form. This confirms that the vectors are parallel and have the same magnitude and direction. Consequently, a translation along ⟨3,-3⟩ maps P1 onto P2.
The two conclusions obtained in the previous example are not a coincidence. In fact, these are general results when performing a composition of translations.
Be aware that a composition of transformations might involve translations and rotations. This combination can produce interesting images.
In interior design, it is pretty common to see designs consisting of a single preimage and its images under different transformations such as translations and rotations. Below, two different kitchen tile designs are made using just four right triangles.
The translation vector tells us that we have to add 4 to the x-coordinate and 1 to the y-coordinate of A in order to move from A to B. With this information, we can write two equations. Translation:& PQ=⟨ 4, 1⟩ A ( x_A,y_A):& ( a-1,b) B ( x_B,y_B):& ( 2b+1,4+a) [-1em] Equation (I):& a-1 + 4= 2b+1 Equation (II):& b + 1= 4+a If we combine these equations, we get a system of equations which can be solved by using the Substitution Method.
Now we can determine the coordinates of A by substituting a= -4, and b= -1 into the expressions for the x- and y-coordinate of A. A( -4-1, -1) → A(-5,-1)
It is given that a line is translated using the vector ⟨ a,b⟩. Let's recall that if we translate a linear function along a vector ⟨ a, b⟩, then we should subtract a from x in the equation and add b to the entire function rule. y=m(x- a)+b+ b Let's simplify the right-hand side.
Now that we have found the equation of the translated line, we can evaluate the y-intercept by substituting 0 for x. Then solve for y.
The y-intercept of the translated line is 2b-ma.
Let's place Heichi's home at the origin of a coordinate plane and let 1 unit represent 1 mile. To go to Harvard, Heichi has to drive 120 miles east and 60 miles south. H_x:& 0 + 120 =120 H_y:& 0 - 60 =-60 This places Harvard at point H(120,- 60) in the coordinate plane.
Next up is Princeton. By using Harvard as a reference point, Heichi has to go 80 miles west and 40 miles north. Therefore, we can find the coordinates of Princeton P, by subtracting 80 from the x-coordinate and adding 40 to the y-coordinate of Harvard. P_x:& 120 - 80 =40 P_y:& -60 + 40 =-20 Now we know that the location of Princeton in our coordinate system is at P(40,- 20).
Finally, Heichi would fly 150 miles northeast from Princeton to Yale. In the diagram, this journey can be described as a right isosceles triangle.
To determine the position of Yale J, we have to find the lengths of this triangle's legs. Since this is an isosceles triangle, its legs are congruent. Furthermore, because the triangle is right, we can find the length of the legs by using the Pythagorean Theorem.
Each leg of the isosceles triangle that describes the journey from Princeton to Yale has the length 75sqrt(2).
To obtain the x-coordinate of J, we have to add 75sqrt(2) to 40. Similarly, to obtain the y-coordinate of J, we have to add 75sqrt(2) to - 20. J_x:& 40 + 75sqrt(2) J_y:& - 20 + 75sqrt(2) Now that we know the coordinates of J, we can make out another right triangle where the distance between Heichi's house and Yale is the hypotenuse.
With this information, we can solve for the distance between Heichi's home and Yale by using the Pythagorean Theorem.
The distance from Heichi's home to Yale if he were to fly directly is about 170 miles.
Let's first plot △ ABC and the midpoint D'.
Since a translation is a rigid motion, every point on the perimeter of △ ABC will be moved the same way. The midpoint on AB, is the point on △ ABC corresponding to D'. Let's find this midpoint D using the Midpoint Formula.
The midpoint of AB is at D(-4,1). Now we can determine the translation by measuring the horizontal and vertical distance between D and D'.
Let's formalize the translation. (x,y)→ (x + 8,y - 3)