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Formulas/physics/Centre Of Mass/Negative Mass Method — Excluded Portion

Negative Mass Method — Excluded Portion

CM when a portion is removed. Treat removed mass as negative. Covers disc with hole, sphere with cavity.
Class 11Class JEE
Derivation

The idea

When a portion is cut out of a uniform body, the remaining body can be thought of as:

original body+negative mass at the location of the removed portion\text{original body} + \text{negative mass at the location of the removed portion}

If the original body has mass m1m_1 and CM at x1x_1, and the removed portion has mass m2m_2 and CM at x2x_2:

xcm=m1x1m2x2m1m2x_{cm} = \frac{m_1 x_1 - m_2 x_2}{m_1 - m_2}

The remaining mass is m1m2m_1 - m_2 and the CM is shifted away from the removed portion.

Why this works

The original body = remaining body + removed portion.

m1x1=(m1m2)xcm,remaining+m2x2m_1 x_1 = (m_1 - m_2) x_{cm,remaining} + m_2 x_2

Solving for xcm,remainingx_{cm,remaining}:

xcm,remaining=m1x1m2x2m1m2x_{cm,remaining} = \frac{m_1 x_1 - m_2 x_2}{m_1 - m_2}

Example 1: Circular disc with circular hole

A uniform disc of radius RR, mass MM, CM at origin. A circular hole of radius R/2R/2 is cut, with centre at (R/2,0)(R/2, 0).

Mass of removed disc: m2=M×π(R/2)2πR2=M4m_2 = M \times \frac{\pi(R/2)^2}{\pi R^2} = \frac{M}{4}

CM of removed disc: x2=R/2x_2 = R/2

xcm=M0M4R2MM4=MR/83M4=R/83/4=R6x_{cm} = \frac{M \cdot 0 - \frac{M}{4} \cdot \frac{R}{2}}{M - \frac{M}{4}} = \frac{-MR/8}{\frac{3M}{4}} = \frac{-R/8}{3/4} = -\frac{R}{6}

The CM shifts to x=R/6x = -R/6 — away from the hole, toward the heavier side. Makes physical sense.

Example 2: Sphere with spherical cavity

A solid sphere of radius RR, mass MM, with a spherical cavity of radius R/2R/2 scooped out, cavity centre at (R/2,0,0)(R/2, 0, 0).

Mass of removed sphere: m2=M×(R/2)3R3=M8m_2 = M \times \frac{(R/2)^3}{R^3} = \frac{M}{8}

CM of cavity: x2=R/2x_2 = R/2

xcm=M0M8R2MM8=MR/167M8=R/167/8=R14x_{cm} = \frac{M \cdot 0 - \frac{M}{8} \cdot \frac{R}{2}}{M - \frac{M}{8}} = \frac{-MR/16}{\frac{7M}{8}} = -\frac{R/16}{7/8} = -\frac{R}{14}

Example 3: Square with square cutout

A uniform square plate of side 2a2a, mass MM, CM at origin. A smaller square of side aa is cut from one corner (say, at position (a/2,a/2)(a/2, a/2)).

Mass of removed square: m2=M4m_2 = \frac{M}{4} (area ratio)

xcm=M0M4a2MM4=Ma/83M/4=a6x_{cm} = \frac{M \cdot 0 - \frac{M}{4} \cdot \frac{a}{2}}{M - \frac{M}{4}} = \frac{-Ma/8}{3M/4} = -\frac{a}{6}

Similarly ycm=a6y_{cm} = -\frac{a}{6}.

The CM always shifts away from the removed portion

This is intuitive: removing mass from one side makes the body heavier on the other side, shifting the CM toward the remaining material.

Remember
For mass ratios: if the body is uniform, $\frac{m_2}{m_1} = \frac{\text{area}_2}{\text{area}_1}$ (2D) or $\frac{\text{volume}_2}{\text{volume}_1}$ (3D). You don't need the actual density — only the ratios matter.