Differences
This shows you the differences between two versions of the page.
Both sides previous revision Previous revision Next revision | Previous revision | ||
183_notes:examples:energy_in_a_spring-mass_system [2014/10/28 07:00] – pwirving | 183_notes:examples:energy_in_a_spring-mass_system [2014/10/28 13:07] (current) – pwirving | ||
---|---|---|---|
Line 8: | Line 8: | ||
+ | === Facts === | ||
- | === Facts === | + | Mass of 0.2kg |
+ | |||
+ | Mass attached to horizontal spring | ||
+ | |||
+ | Horizontal spring stiffness | ||
+ | |||
+ | The initial states for both parts of the problem are separated into part a and part b. | ||
a: | a: | ||
Line 29: | Line 36: | ||
+ | Amplitude (maximum stretch) of the oscillation | ||
+ | |||
+ | Maximum speed of the block | ||
Line 34: | Line 44: | ||
+ | Friction is negligible. | ||
=== Representations === | === Representations === | ||
+ | |||
System: Mass and spring | System: Mass and spring | ||
Surroundings: | Surroundings: | ||
+ | |||
+ | $E_{f} = E_{i} + W$ The energy principle. | ||
+ | |||
+ | $K = \dfrac{1}{2}mv^2$ | ||
+ | |||
+ | $U_{spring} = \dfrac{1}{2}k_{s}s^2$ | ||
=== Solution === | === Solution === | ||
+ | |||
a: | a: | ||
Line 50: | Line 69: | ||
$E_{f} = E_{i} + W$ | $E_{f} = E_{i} + W$ | ||
+ | |||
+ | The initial energy and the final energy can be expressed as the addition of kinetic and potential parts. | ||
$K_{f} + U_{f} = K_{i} + U_{i} + W$ | $K_{f} + U_{f} = K_{i} + U_{i} + W$ | ||
- | $K_{f}$ and $W$ cancel out. | + | We know that no work is done by the surroundings because the point where the wall force is applied does not move. |
+ | |||
+ | We also know that when the stretch is maximum, the block is momentarily at rest (the turning point). | ||
+ | |||
+ | With this information we know that $K_{f}$ and $W$ are zero. | ||
$0 + \dfrac{1}{2}k_{s}s^2_{f} = \dfrac{1}{2}mv^2_{i} + \dfrac{1}{2}k_{s}s^2_{i}$ | $0 + \dfrac{1}{2}k_{s}s^2_{f} = \dfrac{1}{2}mv^2_{i} + \dfrac{1}{2}k_{s}s^2_{i}$ | ||
+ | |||
+ | The amplitude corresponds to the stretch $s_{f}$. We want to rearrange the equations to isolate $s_{f}$. | ||
$\dfrac{1}{2}k_{s}s^2_{f} = \dfrac{1}{2}(0.2 kg)(0.5 m/s)^2 + \dfrac{1}{2}(12 N/m)(0.03 m)^2$ | $\dfrac{1}{2}k_{s}s^2_{f} = \dfrac{1}{2}(0.2 kg)(0.5 m/s)^2 + \dfrac{1}{2}(12 N/m)(0.03 m)^2$ | ||
+ | |||
+ | We can further simplify the equation by substituting values in for the variables. | ||
$\dfrac{1}{2}k_{s}s^2_{f} = 0.03 J$ | $\dfrac{1}{2}k_{s}s^2_{f} = 0.03 J$ | ||
+ | |||
+ | Solve for $s_{f}$. | ||
$s_{f} = \sqrt {2(0.03 J)/(12 N/m)} = 0.07 m$ | $s_{f} = \sqrt {2(0.03 J)/(12 N/m)} = 0.07 m$ | ||
Line 67: | Line 98: | ||
b: | b: | ||
+ | |||
+ | $v_{max}$ is maximum when its final state is when $s_{f} = 0$ which is when the block has only kinetic energy. | ||
+ | |||
+ | The total initial energy when there is only kinetic energy is equal to the total final energy when there is only potential energy. | ||
$K_f + 0 = 0.03 J$ | $K_f + 0 = 0.03 J$ | ||
+ | |||
+ | Substitute in $\dfrac{1}{2}mv^2$ | ||
$\dfrac{1}{2}mv^2_{f} = 0.03 J$ | $\dfrac{1}{2}mv^2_{f} = 0.03 J$ | ||
+ | |||
+ | Isolate $v_{max}$ to solve for the maximum velocity. | ||
$v_{max} = \sqrt {2(0.03 J)/(0.2 kg)} = 0.55 m/s$ | $v_{max} = \sqrt {2(0.03 J)/(0.2 kg)} = 0.55 m/s$ |