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The centre of mass is a point in an object where its entire weight seems to be concentrated. You can think of it as the balancing point of the object. If you tried to balance the object on your finger, it would stay balanced only if your finger was right under the centre of mass. This concept is very useful in physics, especially when we deal with objects that have odd shapes or are made of different parts.
Instead of calculating how every small part of the object moves, we can treat the whole object as if all its mass is located at the centre of mass. This makes solving problems much easier. In this lesson, we’ll learn how to find the centre of mass for a semicircular disc — a shape that’s like a full circle cut in half.
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Assume the mass of the semicircular disc to be M and its radius to be R. The density or mass per unit area of the disc is then given by
σ = M/(πR2/2) = 2M/πR2
Consider a small element in the shape of a ring with radius r and thickness dr. The area of this element can be calculated as
Area = πrdr (since (dr)2 is very small and can be neglected)
The mass of this elementary ring, dM, can be calculated as
dM = (πrdr)(2M/πR2) = (2Mr/R2)dr
Let's denote the coordinates of the centre of mass of this element as (x,y). Due to the symmetry of the disc, x = 0 and y = 2r/π.
Now, let's denote the coordinates of the centre of mass of the semicircular disc as xcm and ycm.
From symmetry, we can conclude that xcm = 0. The y-coordinate can be calculated as
ycm = (1/M)∫ydM
Substituting the value of y and dM into the equation, we get
\(\begin{array}{l}y_{cm} = \frac{1}{M}\int_{0}^{R}\left ( \frac{2r}{\pi } \right ) \frac{2Mr}{R^{2}}dr\end{array} \)
After solving the integral, we find
yCM = (4/πR2)(R3/3) = 4R/3π
In conclusion, the centre of mass of a semicircular disc of radius R and mass M is located at the coordinates (0, 4R/3π).
A semicircular disc is shaped like half of a full circle. If you draw a vertical line down from the middle of the flat edge (diameter), you will notice that both sides of the disc are mirror images of each other. This vertical line is called the y-axis.
Because of this symmetry, the centre of mass must lie somewhere on this y-axis. This is because the left and right parts of the disc are equal, so the centre of mass can’t be off to one side.
Since the shape is symmetrical from left to right, we don’t need to worry about the x-direction (horizontal direction). The x-coordinate of the centre of mass is always zero. So we only need to find its vertical position (the y-coordinate) along the y-axis.
The centre of mass of a semicircular disc is not on the flat edge (diameter) and not at the centre of the full circle either. Instead, it lies a little below the centre of the diameter, inside the curved area of the disc.
So if you tried to balance the disc at this point, it would stay balanced. This is because it lies within the body of the disc, not outside or on the edge.
The exact position of the centre of mass along the y-axis depends on the size of the disc — in other words, its radius (R).
Mathematically, this position is found using a special formula:
y = 4R ÷ (3π)
This means the centre of mass is closer to the flat edge than to the curved edge, and the bigger the radius, the farther down the centre of mass lies.
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