The difference in length of a spring on a pogo stick from its non-compressed length when a teenager is jumping on it after θ seconds can be described by the function f of theta equals 2 times cosine theta plus radical 3 period If the angle was doubled, that is θ became 2θ, what are the solutions in the interval [0, 2π)? How do these compare to the original function?

The difference in length of a spring on a pogo stick from its noncompressed length when a teenager is jumping on it after θ seconds can be described by the func class=
The difference in length of a spring on a pogo stick from its noncompressed length when a teenager is jumping on it after θ seconds can be described by the func class=

Respuesta :

Part A.

The length of the non-compressed spring can be determined by setting

[tex]\theta=0.[/tex]

Now, evaluating the given function at θ=0, we get:

[tex]f(0)=2\cos (0)+\sqrt[]{3}.[/tex]

Recall that:

[tex]\cos 0=1.[/tex]

Therefore:

[tex]f(0)=2\cdot1+\sqrt[]{3}=2+\sqrt[]{3.}[/tex]

Now, to determine all the possible times at which the length will be equal to the non-compressed length, we set the following equation:

[tex]2\cos \theta+\sqrt[]{3}=2+\sqrt[]{3}.[/tex]

Solving the above equation for θ, we get:

[tex]\begin{gathered} 2\cos \theta=2, \\ \cos \theta=1. \end{gathered}[/tex]

The solutions to the above equation are:

[tex]\theta=2n\pi,\text{ where n is a natural number or zero.}[/tex]

Answer part A:

[tex]\theta=2n\pi,\text{ where n is a natural number or zero.}[/tex]

Part B: If we set θ to the double of itself, then, the solutions to the following equation

[tex]f(2\theta)=2+\sqrt[]{3},[/tex]

are:

[tex]2\theta=2n\pi,[/tex]

therefore:

[tex]\theta=n\pi,\text{ where n is a whole number.}[/tex]

If

[tex]\theta\in\lbrack0,2\pi),[/tex]

then

[tex]\theta=0\text{ or }\theta=\pi.[/tex]

Answer part B: The difference is that the period is half of the original period.

[tex]\theta=0\text{ or }\theta=\pi.[/tex]

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