Respuesta :
Answer:
Approximately [tex]6.5 \times 10^{2}\; {\rm N\cdot m^{-1}}[/tex] (assuming that [tex]g = 9.8\; {\rm m\cdot s^{-2}}[/tex] and that the spring is ideal.)
Explanation:
If the elastic cable is ideal, Hooke's Law would apply. Let [tex]k[/tex] denote the spring constant of the cable. At a displacement of [tex]x[/tex] from the equilibrium position of the spring, the elastic potential energy stored in the cables would be [tex](1/2)\, k\, x^{2}[/tex].
In this question, the initial displacement from the equilibrium position was [tex]x = 30.0\; {\rm m}[/tex]. Assuming that there is no energy loss, all the elastic energy stored in the cables would be turned into gravitational potential energy ([tex]{\rm GPE}[/tex])
Let [tex]m[/tex] denote the mass of the passenger and the chair, combined. Let [tex]g[/tex] denote the gravitational field strength. If the altitude gain of the passenger and the chair is [tex]h[/tex], the [tex]{\rm GPE}[/tex] of the passenger and the chair combined would be [tex]m\, g\, h[/tex].
The entirety of the [tex]{\rm GPE}[/tex] of the passenger and the chair was converted from the elastic potential energy initially stored in the cables. There was no energy lost. Therefore, the following would be an equality:
[tex]\displaystyle \frac{1}{2}\, k \, x^{2} = m\, g\, h[/tex].
It is given that [tex]x = 12.0\; {\rm m}[/tex], [tex]m = 1.6 \times 10^{2}\; {\rm kg}[/tex], and [tex]h = 30.0\; {\rm m}[/tex] (relative to the starting position of the passenger and the chair, with the cables already stretched.) Assuming that [tex]g = 9.8\; {\rm m\cdot s^{-2}}[/tex], substitute in the values and solve for the spring constant [tex]k[/tex]:
[tex]\begin{aligned}k &= \frac{2\, m\, g\, h}{x^{2}} \\ &= \frac{2 \times 1.6\times 10^{2}\; {\rm kg} \times 9.8\; {\rm m\cdot s^{-2}} \times 30.0\; {\rm m}}{(12.0\; {\rm m})^{2}} \\ &\approx 6.5 \times 10^{2}\; {\rm kg \cdot s^{-2}} \\ &= 6.5 \times 10^{2}\; {\rm (kg \cdot m \cdot s^{-2}) \cdot m^{-1}} \\ &= 6.5\times 10^{2}\; {\rm N \cdot m^{-1}}\end{aligned}[/tex].