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A 500 g air-track glider attached to a spring with spring constant 10 N/m is sitting at rest on a frictionless air track. A 250 g glider is pushed toward it from the far end of the track at a speed of 120 cm/s. It collides with and sticks to the 500 g glider. What are the amplitude and period of the subsequent oscillations?

Respuesta :

The two related concepts to solve this problem are those concerning the conservation of the Moment and the simple harmonic movement.

By conservation of the moment we can find the speed, while by the simple harmonic movement the Period.

By definition the conservation of momentum is given by

[tex]v_1m_1+v_2m_2 = (m_1+m_2)v_f[/tex]

Where,

[tex]v_{1,2}[/tex] = Velocity of each object

[tex]v_f[/tex] = Final velocity

[tex]m_{1,2}[/tex] = Mass of each object

Since the first body does not have speed, the equation would be subject to,

[tex]v_2m_2 = (m_1+m_2)v_f[/tex]

[tex]250*120=(500+250)*v_f[/tex]

[tex]v_f=40 cm/s[/tex]

From the equations of the harmonic movement we can relate the final velocity with the amplitude and angular frequency and the amplitude with the velocity. In mathematical terms,

[tex]V=Aw[/tex]

Where A is the amplitude and W is the angular frequency, which is also defined as,

[tex]w= \sqrt{(\frac{K}{m})}[/tex]

Replacing this function and clearing for the amplitude we have to,

[tex]A=V*\sqrt{\frac{m}{K}}[/tex]

[tex]A=40*\sqrt{\frac{(0.5+0.25)}{10}}[/tex]

[tex]A=10.95 cm[/tex]

Therefore the amplitude is 10.95cm

At the same time through the angular frequency we can find the period under the definition,

[tex]T =\frac{2\pi}{w}[/tex]

[tex]T =\frac{2\pi}{\sqrt{\frac{K}{m}}}[/tex]

[tex]T =2\pi*\sqrt{\frac{m}{K}}[/tex]

[tex]T=2\pi*\sqrt{0.75}{10}[/tex]

[tex]T =1.72 s[/tex]