Consider an ideal spring that has an unstretched length l and a spring constant k. Suppose the spring is attached to a mass m that lies on a horizontal frictionless surface. The spring-mass system is compressed a distance of x_0 from equilibrium and then released with an initial speed v_0 toward the equilibrium position.

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Answer:

Question:

What is the maximum distance the spring will be stretched

The maximum distance A the spring will be stretched is  [tex]\sqrt{x_0^2+\frac{m}{k}v_0^2 }[/tex].

Explanation:

We note that for an ideal spring

F = ma = -k·x

That is m×[tex]\ddot {x}[/tex] = - k×x

If the equation above has the following initial conditions

x(0) = -x₀

[tex]\dot x (0)[/tex] = v₀

we have [tex]x(t) =-A\cdot \cos (\sqrt{\frac{k}{m} } t+\phi )[/tex]

Where:

A = Amplitude

∅ = Phase Angle

A and ∅ are such that

[tex]x_0 = A\cdot \cos (\phi )[/tex]

[tex]x(t) =A\cdot \sqrt{\frac{k}{m} } \sin \phi = v_0[/tex]

Therefore tan ∅ = [tex]\frac{v_0}{x_0} \sqrt{\frac{m}{k} }[/tex] and

Also, the amplitude A = Maximum displacement from equilibrium or the maximum distance the spring will be stretched is given by;

A = [tex]\sqrt{x_0^2+\frac{m}{k}v_0^2 }[/tex].