The mass per unit length of a non-uniform rod of length L varies as m=20x. Where will be the centre of mass of the rod?

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Published July 24, 2025
Physics
Mechanics
System of Particles
Center of Mass

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Detailed Explanation

Overview of Steps and Why We Choose Them

  1. Model the Density: The problem directly tells us the linear mass density (mass per unit length) as λ(x)=20x\lambda(x) = 20x. This is our starting point.
  2. Find Total Mass (MM): We must know the rod’s entire mass to normalise our centre-of-mass formula. We integrate λ(x)\lambda(x) over the whole length.
  3. Set Up the Centre-of-Mass Integral: The definition of centre of mass for a 1-D object is xcm=1M0Lxdmx_{cm} = \frac{1}{M} \int_{0}^{L} x \, dm. Because dm=λ(x)dxdm = \lambda(x)\,dx, we substitute.
  4. Carry Out the Integrals: Compute the total mass integral and the numerator integral, then divide.
  5. Interpret the Result: State the answer in simple words: how far from the chosen origin.

Detailed Walk-Through

1. Linear Mass Density

The rod is not uniform; its density depends on position xx (measured from the lighter end):

λ(x)=20x(kg per metre, if units are SI)\lambda(x) = 20x \quad \left(\text{kg per metre, if units are SI}\right)

2. Total Mass MM

M=0Lλ(x)dx=0L20xdx=20[x22]0L=10L2M = \int_{0}^{L} \lambda(x)\,dx = \int_{0}^{L} 20x\,dx = 20\left[\frac{x^{2}}{2}\right]_{0}^{L} = 10L^{2}

3. Centre-of-Mass Formula

xcm=1M0Lxdm=1M0Lxλ(x)dxx_{cm} = \frac{1}{M} \int_{0}^{L} x \, dm = \frac{1}{M} \int_{0}^{L} x\,\lambda(x)\,dx

Substitute λ(x)=20x\lambda(x)=20x:

0Lx(20x)dx=200Lx2dx\int_{0}^{L} x\,(20x)\,dx = 20\int_{0}^{L} x^{2}\,dx

4. Compute the Numerator Integral

200Lx2dx=20[x33]0L=203L320\int_{0}^{L} x^{2}\,dx = 20\left[\frac{x^{3}}{3}\right]_{0}^{L} = \frac{20}{3}L^{3}

5. Divide to Get xcmx_{cm}

xcm=1M(203L3)=110L2203L3=23L\begin{aligned} x_{cm} &= \frac{1}{M}\left(\frac{20}{3}L^{3}\right)\\[4pt] &= \frac{1}{10L^{2}} \cdot \frac{20}{3}L^{3}\\[4pt] &= \frac{2}{3}L \end{aligned}

So the centre of mass is located at 23L\boxed{\tfrac{2}{3}L} measured from x=0x=0 (the lighter end).

Simple Explanation (ELI5)

Think of the rod like a stick that gets heavier as you go from the left end to the right end.

  • The rule that tells us how heavy each tiny piece is says:
    • For every 1-metre step to the right, that little piece is 20 times heavier than if we were at the very start!
  • To find the balancing point (centre of mass), we do the same thing you do when you try to balance a seesaw: you imagine all the tiny children (little masses) sitting along the rod and ask, "Where should the pivot be so the seesaw stays level?"
  • Math lets us add up every tiny piece’s weight and its position. When we do that careful adding, the balancing point comes out at two-thirds of the rod’s length from the lighter end.

So if the rod is LL metres long, the centre of mass is at 23L\frac{2}{3}L from the end where x=0x=0 (the lighter end).

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Step-by-Step Solution

Step-by-Step Solution

  1. Given: Linear mass density λ(x)=20x\lambda(x) = 20x for 0xL0 \le x \le L.

  2. Total Mass

M=0L20xdx=10L2M = \int_{0}^{L} 20x\,dx = 10L^{2}
  1. Centre of Mass Formula
xcm=1M0Lxλ(x)dxx_{cm} = \frac{1}{M} \int_{0}^{L} x\,\lambda(x)\,dx
  1. Compute Numerator
0Lx(20x)dx=200Lx2dx=203L3\int_{0}^{L} x\,(20x)\,dx = 20\int_{0}^{L} x^{2}\,dx = \frac{20}{3}L^{3}
  1. Divide
xcm=110L2×203L3=23L\begin{aligned} x_{cm} &= \frac{1}{10L^{2}} \times \frac{20}{3}L^{3}\\[4pt] &= \frac{2}{3}L \end{aligned}
  1. Answer: The centre of mass is 2L3\boxed{\dfrac{2L}{3}} from the end where x=0x=0 (the lighter end).

Examples

Example 1

Balancing a hammer: the heavy head shifts the centre of mass toward the head, similar to the non-uniform rod.

Example 2

Designing tapered light poles: engineers calculate centre of mass to ensure the base can handle wind loads.

Example 3

Loading cargo on a ship: distribution of weight is critical so the ship’s centre of mass stays low and centred.

Example 4

Placing batteries in an RC car: heavier components are arranged so the centre of mass improves cornering stability.

Visual Representation

References

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