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Q.Using a thin uniform rod, show that the centre of mass of homogenous bodies lies at their geometric centre.

Manipur CohsemCouncil of Higher Secondary Education, Manipur (Higher Secondary 1st Year) 2020Subjective· 3mImportance★★★★★
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Integrating x·dm along a thin uniform rod and dividing by the total mass gives X_cm = L/2 — the geometric midpoint — confirming that a symmetric, uniform-density body's centre of mass coincides with its geometric centre.

For a system of discrete particles, the x-coordinate of the centre of mass is

Xcm=∑mixi∑miX_{cm} = \dfrac{\sum m_i x_i}{\sum m_i}

For a continuous body, this sum becomes an integral over infinitesimally small mass elements dm:

Xcm=∫x dm∫dm=1M∫x dmX_{cm} = \dfrac{\int x\, dm}{\int dm} = \dfrac{1}{M}\int x\, dm

Setting up for a thin uniform rod:

Consider a thin, uniform rod of total mass M and length L, lying along the x-axis with one end at x=0x = 0 and the other end at x=Lx = L.

Since the rod is uniform, its mass per unit length (linear mass density) is constant:

λ=ML\lambda = \dfrac{M}{L}

Consider a small element of the rod of length dx, located at position x. Its mass is

dm=λ dx=MLdxdm = \lambda\, dx = \dfrac{M}{L}dx

Computing the centre of mass:

Xcm=1M∫0Lx⋅MLdx=1L∫0Lx dx=1L[x22]0L=1L⋅L22=L2X_{cm} = \dfrac{1}{M}\int_0^L x \cdot \dfrac{M}{L}dx = \dfrac{1}{L}\int_0^L x\, dx = \dfrac{1}{L}\left[\dfrac{x^2}{2}\right]_0^L = \dfrac{1}{L}\cdot\dfrac{L^2}{2} = \dfrac{L}{2}

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