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NCERT Exemplar · Q16

Q.The centre of mass of an extended body on the surface of the earth and its centre of gravity (Note: more than one of the given options may be correct.)

(a) are always at the same point for any size of the body.
(b) are always at the same point only for spherical bodies.
(c) can never be at the same point.
(d) is close to each other for objects, say of sizes less than 100 m.
(e) both can change if the object is taken deep inside the earth.
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Centre of mass is a geometric property; centre of gravity depends on the local gravitational field. For small objects on Earth's surface the two nearly coincide, but they separate for large bodies or when the field varies significantly. Options (D) and (E) are correct.

Why centre of mass and centre of gravity differ

The centre of mass is purely geometric: it is the weighted average position of all the mass elements in a body, independent of any external field. If you have mass elements mim_i at positions r⃗i\vec{r}_i, then

r⃗CM=∑mir⃗i∑mi.\vec{r}_{\text{CM}} = \frac{\sum m_i \vec{r}_i}{\sum m_i}.

The centre of gravity, on the other hand, is the point where the total gravitational force (weight) can be considered to act. It is the weighted average of positions using weight as the weighting factor:

r⃗CG=∑migir⃗i∑migi,\vec{r}_{\text{CG}} = \frac{\sum m_i g_i \vec{r}_i}{\sum m_i g_i},

where gig_i is the local acceleration due to gravity at position r⃗i\vec{r}_i.

If gravity is uniform—the same magnitude and direction everywhere in the body—then gi=gg_i = g factors out and the two definitions become identical. But Earth's gravity is not perfectly uniform: it decreases with altitude (or increases with depth, up to a point), and its direction is always radial toward Earth's centre. For an extended body these variations matter.


Examining each option

1. Option (A): "are always at the same point for any size of the body"

This would require gravity to be uniform across the entire body, regardless of size. On Earth's surface, gg varies with height as

g(h)≈g0(1−2hRE),g(h) \approx g_0 \left(1 - \frac{2h}{R_E}\right),

where RE≈6400 kmR_E \approx 6400\,\text{km}. For a tall building (say 100 m), the variation is about 2×1006.4×106≈3×10−5\frac{2 \times 100}{6.4 \times 10^6} \approx 3 \times 10^{-5}, or 0.003%. This is negligible, so CM and CG nearly coincide.

But for a very large object—imagine a body stretching hundreds of kilometres vertically—the top experiences noticeably weaker gravity than the bottom. The centre of gravity shifts downward (toward the stronger field) relative to the centre of mass.

Option (A) is false.


2. Option (B): "are always at the same point only for spherical bodies"

Spherical symmetry of the body does not guarantee uniform gravity within the body. A large sphere on Earth's surface still has its top farther from Earth's centre than its bottom, so gg varies across it. The statement confuses the symmetry of the object with the uniformity of the external field.

Option (B) is false.


3. Option (C): "can never be at the same point"

In the limit of a point mass, or for any body small enough that gg is effectively constant across it, CM and CG coincide to any measurable precision. So "never" is too strong.

Option (C) is false.


4. Option (D): "is close to each other for objects, say of sizes less than 100 m"

For a 100 m tall object, the fractional change in gg from bottom to top is

Δgg≈2hRE=2006.4×106≈3×10−5.\frac{\Delta g}{g} \approx \frac{2h}{R_E} = \frac{200}{6.4 \times 10^6} \approx 3 \times 10^{-5}.

This tiny variation means the centre of gravity is displaced from the centre of mass by a distance of order h×10−5∼1 mmh \times 10^{-5} \sim 1\,\text{mm}—utterly negligible for any practical purpose. The two points are indeed "close."

Tip

For everyday objects (buildings, vehicles, even large ships), treating CM and CG as the same point introduces errors far smaller than measurement uncertainty.

Option (D) is correct.


5. Option (E): "both can change if the object is taken deep inside the earth"

The centre of mass is an intrinsic property of the body's mass distribution; moving the body does not change it (assuming the body is rigid). …

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