The effective mass of the spring in spring-mass system is m/3.
1. Assume the Spring's Total Mass m and Length L:
Let the spring be uniformly distributed with mass m and length L. The linear mass density λ of the spring is:
$ \lambda =\frac{m}{L}$
2. Position and Velocity of Elements:
Each point on the spring moves with a different velocity during oscillations. If we assume simple harmonic motion, the velocity at a point x along the spring can be written as proportional to x.
So, if v is the velocity at the end of the spring, then the velocity of an element at position x along the spring is:
$v(x)=\frac{x}{L}.v$
3. Infinitesimal Mass Element dm:
For an infinitesimal element of length dx at position x, the mass dm is:
$dm=\lambda dx=\frac{m}{L}dx$
4. Infinitesimal Kinetic Energy:
The kinetic energy of this infinitesimal element is:
$dK=\frac{1}{2}dmv(x)^{2}=\frac{1}{2}\frac{m}{L}dx(\frac{x}{L}v)^{2}$
$dK=\frac{1}{2}\frac{m}{L}\frac{x^{2}}{L^{2}}v^{2}dx=\frac{m}{2}\frac{v^{2}}{L^{3}}x^{2}dx$
5. Total Kinetic Energy of the Spring:
Integrate dK from x = 0 to x = L to find the total kinetic energy K:
$K=\int_{0}^{L}\frac{mv^{2}}{2L^{3}}x^{2}dx$
$K=\frac{mv^{2}}{2L^{3}}\frac{L^{3}}{3}=\frac{mv^{2}}{6}$
6. Define Effective Mass:
The kinetic energy of the spring can be equated to the kinetic energy of a point mass m<sub> eff </sub> moving with velocity v:
$\frac{1}{2}m_{eff}v^{2}=\frac{mv^{2}}{6}$
$m_{eff}=\frac{m}{3}$
Thus, the effective mass of the spring is indeed $\frac{m}{3}$.
No comments:
Post a Comment