** Observe Properties through Symmetry **** ** positiveeast.org Topical Outline | Geometry Outline | MathBits" Teacher Reresources **Terms of Use Contact Person:** Donna Roberts

Properties of

**parallelograms**can be observed via symmetry.

*Definition:*A

**parallelogram**is a quadrilateral through two sets of opposite sides parallel. Definitions need no further observations, as they are stated facts.

A parallelogram has **rotational symmetry** when rotated 180º about its center. A parallelogram has no reflectional symmetry.

Rotational symmetry will map These sides coincide after the rotation, so we can observe that

*AD = CB*and

*AB = CD.*

**The opposite sides are congruent.**

You are watching: Does a rhombus have rotational symmetry

You are watching: Does a rhombus have rotational symmetry

This rotation will also map

*∠A*onto

*∠C*and

*∠B*onto

*∠D*, showing the

**opposite angles congruent.**

If we draw the diagonals, intersecting at P, rotational symmetry will mans Theses segments will coincide after the rotation, showing us that DP = BP and AP = CP, which implies congruent segments. Segment bisectors create congruent segments, so we see the diagonals bisecting each other. | |

If we draw a single diagonal (either one), we can observe that the rotational symmetry will map Δ ADC onto ΔCBA. This shows the diagonal creating two congruent triangles. |

Properties of rectangles can be observed through symmetry. Definition: A rectangle is a parallelogram with four right angles. A rectangle has Reflectional symmetry, (over the line of reflection shown), will map A onto B, and D onto C (as well as B onto A and C onto D). Since reflection is a rigid transformation, we know that lengths are preserved. If we now draw the diagonal from A to C, we know that the length of the diagonal will be preserved after the reflection. Since the reflection maps , we can see the diagonals congruent. Properties of a rhombus can be observed through symmetry. Definition: A rhombus is a parallelogram with four congruent sides. Reflectional symmetry, over the diagonal from Since reflection is a rigid transformation, the reflections in the diagonals from B, D and E are equidistant from A and C. Also, points A, C and E are equidistant from B and D. By definition of perpendicular bisectors, we know . The diagonals are perpendicular. Properties of squares can be observed via symmetry. Definition: A square is a paralleloglamb with four right angles and four congruent sides. A square has Since a square is a parallelogram, a rectangle, and a rhombus, our symmetry observations for a square will be the same as those we have already seen. A trapezoid has no reflectional symmetry and no rotational symmetry. We cannot make monitorings based upon symmetry. Definition: A trapezoid is a quadrilateral with at least one pair of parallel sides. Properties of isosceles trapezoids can be observed via symmetry. Definition: An isosceles trapezoid is a trapezoid with congruent base angles. A isosceles trapezoid has reflectional symmetry when reflected over the line through the midpoints of its bases. An isosceles trapezoid with only one pair of parallel sides has no rotational symmetry. Reflectional symmetry, (over the line of reflection shown), will map A onto B, and D onto C (as well as B onto A and C onto D). Since reflection is a rigid transformation, we know that lengths are preserved. Leg coincides with leg . The legs are congruent. During this reflection, which also preserves angle measure, ∠A will map onto ∠B and ∠D will map onto ∠C, making the base angles congruent. If we now draw the diagonal from A to C,we know that the length of the diagonal will be preserved after the reflection.Since the reflection mapns ,we can see the diagonals congruent. Properties of kites can be observed with symmetry. Definition: A kite is a quadrilateral with two distinct pairs of adjacent sides congruent. A kite has reflectional symmetry when reflected over its diagonal which connects the common endpoints of its congruent adjacent sides. Reflectional symmetry, (over the line of reflection shown), will map A onto C, B onto B and D onto C (as well as C onto A). Since reflection is a rigid transformation, we know that angle measures are preserved. ∠A is mapped onto ∠C and m∠A = m∠C. One pair of opposite ∠s congruent. In addition, One diagonal bisects the angles. We can also observe that the reflectional symmetry will map Δ If we draw the second diagonal from One diagonal bisects the other. Note: The diagonal DOING the bisecting is the diagonal which is also the line of reflection. Topical Outline | Geometry Outline | positiveeast.org | MathBits" Teacher Resources Terms of Use |