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### Course: Algebra 2 > Unit 12

Lesson 2: Interpreting features of functions# Symmetry of algebraic models

Learn how to interpret the symmetry of a graph in the context of an applied problem.

## Introduction

In this article, we will learn how to interpret the symmetry of a graph in the context of an applied problem.

But first, let's refresh our memories regarding the symmetry of functions.

## Symmetry of functions

Now, let's take a look at an example.

## Example 1

The energy stored in a spring, $E(x)$ , in joules, is a function of the spring's displacement, $x$ , in meters, from its relaxed state, with a positive $x$ indicating a stretched spring and a negative $x$ indicating a compressed spring. The graph of $y=E(x)$ is shown below.

What can we learn about the context from the symmetry of its graph?

## The symmetry of function $E$

Let's apply what we know about symmetry to function $E$ .

If you reflect the graph of function $E$ over the $y$ -axis, it lands on itself.

So, function $E$ is an even function. Algebraically, this means that $E(-x)=E(x)$ for all $x$ .

## Interpreting symmetrical features

What does “$E(-x)=E(x)$ for all $x$ ” mean?

Because the statement is true for $x$ 's, we can say that $E(-x)=E(x)$ is true when $x=2$ , $x=4$ , $x=10$ , etc. Let's start by thinking about what the statement means for a specific $x$ value, in this case when $x=2$ .

*all*When $x=2$ , this statement becomes $E(-2)=E(2)$ .

Focusing on what each variable represents can help with this interpretation. Remember that a

*positive*input indicates a*stretch*of the spring and a*negative*input indicates a*compression*of the spring, and that an output represents the energy stored in the spring.In this light, we see that ${E}({-2})={E}({2})$ means that a ${\text{spring compressed by}2\text{meters}}$ contains the same amount of${\text{energy}}$ as ${\text{the same spring stretched by}2\text{meters}}$ .

We are now ready to interpret the more general statement, $E(-x)=E(x)$ , which is our ultimate goal.

Using the above examples for guidance, we see that $E(-x)=E(x)$ means that a spring compressed by $x$ meters contains the same amount of energy as a spring stretched by $x$ meters.

In other words:

*A spring compressed by a certain amount stores the same amount of energy as a spring that has been stretched by that same amount*.### Reflection question

Let's try another example.

## Example 2

Pranav normally uses $20$ kilograms of wood per day in his wood stove to keep his house at $25$ degrees Celsius. He tries adjusting the amount of wood, $w$ , he burns to see how the temperature changes. Specifically, a positive $w$ indicates an addition of $w$ kilograms of wood and a negative $w$ indicates a reduction of $w$ kilograms of wood. The graph of $y=T(w)$ is shown below, where $T(w)$ indicates the change in the temperature of Pranav's house.

## The symmetry of function $T$

The graph of function $T$ is symmetric with respect to the origin.

So, function $T$ is an odd function. Algebraically, this means that $T(-w)=-T(w)$ for all $w$ .

## Interpreting symmetrical features

To interpret the symmetry in this situation, we want to translate the mathematical statement “for any $w$ -value, $T(-w)=-T(w)$ ” in terms of the context.

Again, let's start by thinking about the meaning of this for a particular $w$ value. Then, we can go back and generalize.

To help with this, remember that a

*positive*input indicates an*addition*of wood and a*negative*input indicates a*reduction*of wood, and that the function outputs a temperature change.So we see that ${T}({-1})=-{T}({1})$ means that the ${\text{temperature change}}$ that results from burning ${1\text{less kilogram of wood}}$ is opposite that of what results from burning ${1\text{more kilogram of wood}}$ .

We are now ready to generalize and interpret the symmetry statement for a general $w$ .

In other words:

*Increasing and decreasing the wood burned by a certain amount have exactly opposite effects on the temperature of the house.*### Reflection question

## Drawing a conclusion

In general, to interpret the meaning of the symmetry in the graph of a function, it is helpful to do the following:

Step $1$ : Decide if the function is even or odd and determine what this means algebraically.

Step $2$ : Understand what each variable represents in terms of the context.

Step $3$ : Come up with a statement that uses the meaning of the variables and compares the output values for opposite input values.

## Try it yourself

Trudy is learning to drive a new kind of vehicle. The speed of the vehicle is determined by the position of a rotating knob. The vehicle's speed, $V(x)$ , in miles per hour, is a function of the knob position, $x$ . Note that $x>0$ means the knob is turned $x$ units clockwise and $x<0$ means the knob is turned $x$ units counter-clockwise.

The graph of $y=V(x)$ is shown below.

## Want to join the conversation?

- I answered the last question right, but I still don't understand why option A is wrong. "Adjacent knob positions result in speeds that are different by 1/2 miles per hour.". That seems correct to me. Both lines increase at that rate for each adjacent knob position, i.e., 1,2,3, etc. So what is wrong with that option?(15 votes)
- The phrasing of the question is a bit tricky. It doesn't ask which statement is true, it asks which statement "best interprets the symmetry".

The statement you selected may be true, but it doesn't say anything about the symmetry of the graph.

The statement that "Rotating the knob clockwise and counter-clockwise by the same amount results in equal vehicle speeds" is not only true, but also explains what it means for this graph to be symmetrical.(58 votes)

- proof: any function can be written as sum of an even function and an odd function.(8 votes)
- Nice problem!

For any function f(x), with a domain of all real numbers, define the functions

g(x)=(f(x)+f(-x))/2

h(x)=(f(x)-f(-x))/2.

We have

g(x)+h(x)

=(f(x)+f(-x)+f(x)-f(-x))/2

=2f(x)/2

=f(x).

So f(x) is the sum of g(x) and h(x).

The function g(x) is even because

g(-x)=(f(-x)+f(x))/2

=(f(x)+f(-x))/2

=g(x).

The function h(x) is odd because

h(-x)=(f(-x)-f(x))/2

=-(f(x)-f(-x))/2

=-h(x).

Since f(x) is any arbitrary function, we conclude that any function, with a domain of all real numbers, can be written as the sum of an even function and an odd function.(17 votes)

- Is there function that is both even or odd?(5 votes)
- Yes, f(x) = 0 is both even and odd.(12 votes)

- Can f(x)=-f(x), except when f(x)=0(4 votes)
- Your statement does not make sense.

f(x) = -f(x) would mean that each input "x" creates two output values y and -y and those two values are equal. The only situtation where y and -y would be equal is when y=0. You have excluded that value.

Another issue with the statement is that a function can only generate one output for each input. Your statement is trying to indicate that there are two outputs for one input generated by the function. That would never happen.(5 votes)

- So what would F(x)=-F(x) be?

Even or neither.(3 votes)- The only value which is its own negative is zero. So only F(x) = 0 would satisfy that constraint.

Now if F(x) = 0, then F(-x) = 0 also. So your function would be both odd and even.(4 votes)

- While I understand that the point of the last section of the article is to illustrate the behavior of even functions, one could "assume" that "adjacent knob positions" means adjacent integer values, e.g. there's some sort of detent at each integer value. In that case, the first statement, "Adjacent knob positions result in speeds that are different by 1/2 mile per hour", would also be correct.(3 votes)