CM when a portion is removed. Treat removed mass as negative. Covers disc with hole, sphere with cavity.
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
If the original body has mass m1 and CM at x1, and the removed portion has mass m2 and CM at x2:
xcm=m1−m2m1x1−m2x2
The remaining mass is m1−m2 and the CM is shifted away from the removed portion.
Why this works
The original body = remaining body + removed portion.
m1x1=(m1−m2)xcm,remaining+m2x2
Solving for xcm,remaining:
xcm,remaining=m1−m2m1x1−m2x2
Example 1: Circular disc with circular hole
A uniform disc of radius R, mass M, CM at origin. A circular hole of radius R/2 is cut, with centre at (R/2,0).
Mass of removed disc: m2=M×πR2π(R/2)2=4M
CM of removed disc: x2=R/2
xcm=M−4MM⋅0−4M⋅2R=43M−MR/8=3/4−R/8=−6R
The CM shifts to x=−R/6 — away from the hole, toward the heavier side. Makes physical sense.
Example 2: Sphere with spherical cavity
A solid sphere of radius R, mass M, with a spherical cavity of radius R/2 scooped out, cavity centre at (R/2,0,0).
Mass of removed sphere: m2=M×R3(R/2)3=8M
CM of cavity: x2=R/2
xcm=M−8MM⋅0−8M⋅2R=87M−MR/16=−7/8R/16=−14R
Example 3: Square with square cutout
A uniform square plate of side 2a, mass M, CM at origin. A smaller square of side a is cut from one corner (say, at position (a/2,a/2)).
Mass of removed square: m2=4M (area ratio)
xcm=M−4MM⋅0−4M⋅2a=3M/4−Ma/8=−6a
Similarly ycm=−6a.
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.