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A 2-kg mass is attached to a spring with spring constant 24 N/m. The system is then immersed in a medium imparting a damping force equal to 16 times the instantaneous velocity of the mass. Find the equation of motion if it is released from rest at a point 40 cm below equilibrium.
$x(t)=0.6{e}^{\mathrm{-2}t}-0.2{e}^{\mathrm{-6}t}$
In this case, we say the system is critically damped . The general solution has the form
where ${\lambda}_{1}$ is less than zero. The motion of a critically damped system is very similar to that of an overdamped system. It does not oscillate. However, with a critically damped system, if the damping is reduced even a little, oscillatory behavior results. From a practical perspective, physical systems are almost always either overdamped or underdamped (case 3, which we consider next). It is impossible to fine-tune the characteristics of a physical system so that ${b}^{2}$ and $4mk$ are exactly equal. [link] shows what typical critically damped behavior looks like.
A 1-kg mass stretches a spring 20 cm. The system is attached to a dashpot that imparts a damping force equal to 14 times the instantaneous velocity of the mass. Find the equation of motion if the mass is released from equilibrium with an upward velocity of 3 m/sec.
We have $mg=1\left(9.8\right)=0.2k,$ so $k=49.$ Then, the differential equation is
which has general solution
Applying the initial conditions $x(0)=0$ and ${x}^{\prime}(0)=\mathrm{-3}$ gives
A 1-lb weight stretches a spring 6 in., and the system is attached to a dashpot that imparts a damping force equal to half the instantaneous velocity of the mass. Find the equation of motion if the mass is released from rest at a point 6 in. below equilibrium.
$x(t)=\frac{1}{2}{e}^{\mathrm{-8}t}+4t{e}^{\mathrm{-8}t}$
In this case, we say the system is underdamped . The general solution has the form
where $\alpha $ is less than zero. Underdamped systems do oscillate because of the sine and cosine terms in the solution. However, the exponential term dominates eventually, so the amplitude of the oscillations decreases over time. [link] shows what typical underdamped behavior looks like.
Note that for all damped systems, $\underset{t\to \infty}{\text{lim}}x(t)=0.$ The system always approaches the equilibrium position over time.
A 16-lb weight stretches a spring 3.2 ft. Assume the damping force on the system is equal to the instantaneous velocity of the mass. Find the equation of motion if the mass is released from rest at a point 9 in. below equilibrium.
We have $k=\frac{16}{3.2}=5$ and $m=\frac{16}{32}=\frac{1}{2},$ so the differential equation is
This equation has the general solution
Applying the initial conditions, $x(0)=\frac{3}{4}$ and ${x}^{\prime}(0)=0,$ we get
A 1-kg mass stretches a spring 49 cm. The system is immersed in a medium that imparts a damping force equal to four times the instantaneous velocity of the mass. Find the equation of motion if the mass is released from rest at a point 24 cm above equilibrium.
$x(t)=\mathrm{-0.24}{e}^{\mathrm{-2}t}\text{cos}\phantom{\rule{0.1em}{0ex}}\left(4t\right)-0.12{e}^{\mathrm{-2}t}\text{sin}\phantom{\rule{0.1em}{0ex}}\left(4t\right)$
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