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183_notes:examples:the_jumper [2014/10/07 05:05] – pwirving | 183_notes:examples:the_jumper [2014/10/11 06:07] – pwirving | ||
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Surroundings: | Surroundings: | ||
- | {{course_planning: | + | $$\Delta E_{system} = W_{surroundings}$$ |
+ | |||
+ | {{course_planning: | ||
=== Solution === | === Solution === | ||
+ | |||
+ | The first step is defining the system and surroundings which we have done in representations section, with the jumper, cord and Earth parts of the system and the surroundings being nothing. | ||
+ | |||
+ | Energy of the system is equal to the work done by the surroundings. | ||
$$\Delta E_{system} = W_{surroundings}$$ | $$\Delta E_{system} = W_{surroundings}$$ | ||
+ | |||
+ | In the initial state of the problem the sum of the kinetic and potential energies is equal to zero since there is no work done by the surroundings. | ||
$$\Delta K_{jumper} + \Delta U_{grav} + \Delta U_{spring} = W_{surroundings} = 0$$ | $$\Delta K_{jumper} + \Delta U_{grav} + \Delta U_{spring} = W_{surroundings} = 0$$ | ||
- | $$\Delta K_{jumper}$$ is 0 because jumper is motionless before + after jump | + | $$\Delta K_{jumper}$$ |
- | $$W_{surroundings}$$ no work | + | $W_{surroundings}$ |
+ | |||
+ | Let gravitational potential energy equal to potential energy of a spring so that you can solve for k_{s} | ||
$$\Delta U_{grav} = -\Delta U_{spring}$$ | $$\Delta U_{grav} = -\Delta U_{spring}$$ | ||
+ | |||
+ | Sub in formulas for gravitational potential energy and potential energy into equation. | ||
$$mg(y_{f}-y_{i}) = \dfrac{1}{2}ks({s_{f}}^2 - {s_{i}}^2)$$ | $$mg(y_{f}-y_{i}) = \dfrac{1}{2}ks({s_{f}}^2 - {s_{i}}^2)$$ | ||
- | $${s_{i}}^2 = 0$$ no stretch | + | ${s_{i}}^2 = 0$ There is no stretch |
+ | |||
+ | You can cancel out s_{i}. | ||
$$m_{j}(y_{f}-y_{i}) = -\dfrac{1}{2}ks({s_{f}}^2)$$ | $$m_{j}(y_{f}-y_{i}) = -\dfrac{1}{2}ks({s_{f}}^2)$$ | ||
+ | |||
+ | Rearrange the equation to solve for k_{s}: | ||
+ | |||
+ | $$k_{s} = \dfrac{-2m_{j}g(y_{f}-y_{i})}{{s_{f}}^2} >0$$ | ||
+ | |||
+ | We expect k_{s} to be greater than 0 which makes sense because $(y_{f}-y_{i}) < 0$ due to the person dropping 30m from its initial height. | ||
+ | |||
+ | $s_{f} = L - L_{0}$ | ||
+ | |||
+ | You were told in the question that when not stretched the cord is 10m and the stretched length is 30m. | ||
+ | |||
+ | $$k_{s} = \dfrac{-2(200kg)(9.81m/ | ||
+ | |||
+ | Substitute in for various variables to solve for k_{s} | ||
+ | |||
+ | $$k_{s} = 294N/m$$ | ||