Spring Potential Energy: Difference between revisions
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===Difficult=== | ===Difficult=== | ||
A package of mass 9 kg sits on an airless asteroid with mass 8.0x10<sup>20</ | A package of mass 9 kg sits on an airless asteroid with mass 8.0x10<sup>20</sup> kg and radius 8.7x10<sup>5</sup> m. Your goal is to launch the package so that it will never come back and when it is very far away it will have a speed of 226 m/s. You have a spring whose stiffness is 2.8x10<sup>5</sup> N/m. How much must you compress the spring? | ||
The initial condition for escape from the asteroid is: | The initial condition for escape from the asteroid is: | ||
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Potential energy of the spring equals the total energy in the system. | Potential energy of the spring equals the total energy in the system. | ||
<sup>1</sup>⁄<sub> | <sup>1</sup>⁄<sub>2</sub>k<sub>s</sub>s<sup>2</sup =<sup>1</sup>⁄<sub>(2</sub>mv<sub>esc<sup>2</sup> +(-G<sup>Mm</sup>⁄<sub>R</sub | ||
s<sup>2</ | s<sup>2</sup> = <sup>m</sup>⁄<sub>(k<sub>s</sub>(<sup>2GM</sup>⁄<sub>(k<sub>R</sub> +v<sup>2</sup> | ||
==Connectedness== | ==Connectedness== |
Revision as of 21:14, 5 December 2015
Work in progress by scarswell3 This topic covers Spring Potential Energy.
The Main Idea
Elastic Potential Energy is the energy stored in elastic materials due to their deformation. Often this refers to the stretching or compressing of a spring.
A Mathematical Model
The formula for Ideal Spring Energy is:
Us=1⁄2kss2
where:
ks= spring constant
s2= stretch measured from the equilibrium point;
A Computational Model
An oscillating spring can be modeled by the following:
from __future__ import division from visual import * from visual.graph import * scene.width=600 scene.height = 760 g = 9.8 mball = .2 Lo = 0.3 ks = 12 deltat = 1e-3 t = 0 ceiling = box(pos=(0,0,0), size = (0.5, 0.01, 0.2)) ball = sphere(pos=(0,-0.3,0), radius=0.025, color=color.yellow) spring = helix(pos=ceiling.pos, color=color.green, thickness=.005, coils=10, radius=0.01) spring.axis = ball.pos - ceiling.pos vball = vector(0.02,0,0) ball.p = mball*vball scene.autoscale = 0 scene.center = vector(0,-Lo,0) while t < 10: rate(1000) L_vector = (mag(ball.pos) - Lo)* ball.pos.norm() Fspring = -ks * L_vector Fgrav = vector(0,-mball * g,0) Fnet = Fspring + Fgrav ball.p = ball.p + Fnet * deltat ball.pos = ball.pos + (ball.p/mball) * deltat spring.axis = ball.pos-ceiling.pos t = t + deltat
Examples
Be sure to show all steps in your solution and include diagrams whenever possible
Simple
If a spring's spring constant is 200 N/m and it is stretched 1.5 meters from rest, what is the potential spring energy?
ks= 200 N/m
s= 1.5 m
Us=(0.5)kss2
Us= (0.5)(200 N/m)(1.5 m)2
Us= 225 J
Middling
A horizontal spring with stiffness 0.6 N/m has a relaxed length of 10 cm. A mass of 25 g is attached and you stretch the spring to a length of 20 cm. The mass is released and moves with little friction. What is the speed of the mass at the moment when the spring returns to its relaxed length of 10cm?
ks= 0.6 N/m
s= 0.1 m
Us=(.5)kss2= (.5)(0.6 N/m)(0.1 m)2
Us= 0.003 J
Potential Energy is Converted into Kinetic Energy (K):
Us= K
Us=(0.5)mv2
0.003 J=(0.5)(0.025 kg)v2
v2=(0.003 J)⁄((0.5)(0.025 kg)
v2=0.24 J/kg*s
v=0.49 m/s
Difficult
A package of mass 9 kg sits on an airless asteroid with mass 8.0x1020 kg and radius 8.7x105 m. Your goal is to launch the package so that it will never come back and when it is very far away it will have a speed of 226 m/s. You have a spring whose stiffness is 2.8x105 N/m. How much must you compress the spring?
The initial condition for escape from the asteroid is:
Ki+Ui =1⁄(2mvesc2 +(-GMm⁄(R=0
Potential energy of the spring equals the total energy in the system.
1⁄2kss2</sup =1⁄(2mvesc2 +(-GMm⁄R</sub
s2 = m⁄(ks(2GM⁄(kR +v2
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