Applications of Integration: Center of Mass, Mean Value, and Root Mean Square

Center of Mass

Center of Mass for Discrete Masses

  • Consider a mechanical system with nn discrete masses located at positions along an axis.
  • Index each mass with i=1i = 1 to nn.
  • The ithi^{th} body has mass m<em>im<em>i and is located at position x</em>ix</em>i with respect to the origin.
  • The location of the center of mass xˉ\bar{x} is calculated as:
    xˉ=<em>i=1nx</em>im<em>i</em>i=1nmi\bar{x} = \frac{\sum<em>{i=1}^{n} x</em>i m<em>i}{\sum</em>{i=1}^{n} m_i}
Example: Discrete Masses
  • Four masses are located at positions -2, -1, 1, and 2.
  • The masses are 2, 1, 2, and 3, respectively.
  • Calculate the center of mass:
    xˉ=<em>i=14x</em>im<em>i</em>i=14m<em>i\bar{x} = \frac{\sum<em>{i=1}^{4} x</em>i m<em>i}{\sum</em>{i=1}^{4} m<em>i}xˉ=x</em>1m<em>1+x</em>2m<em>2+x</em>3m<em>3+x</em>4m<em>4m</em>1+m<em>2+m</em>3+m4\bar{x} = \frac{x</em>1m<em>1 + x</em>2m<em>2 + x</em>3m<em>3 + x</em>4m<em>4}{m</em>1 + m<em>2 + m</em>3 + m_4}
    xˉ=(2)(2)+(1)(1)+(1)(2)+(2)(3)2+1+2+3\bar{x} = \frac{(-2)(2) + (-1)(1) + (1)(2) + (2)(3)}{2 + 1 + 2 + 3}
    xˉ=41+2+68\bar{x} = \frac{-4 - 1 + 2 + 6}{8}
    xˉ=38\bar{x} = \frac{3}{8}

Center of Mass for Continuous Systems

  • For a one-dimensional object with linear density ρ(x)\rho(x), where ρ(x)\rho(x) gives the density at each point xx from the origin.
  • Assume the density function is defined from x=ax = a to x=bx = b.
  • Divide the interval [a,b][a, b] into nn equal subintervals of length Δx=ban\Delta x = \frac{b - a}{n}.
  • Approximate the mass in each subinterval as ρ(xi)Δx\rho(x_i) \Delta x.
  • Approximate the center of mass as:
    xˉ<em>i=1nx</em>iρ(x<em>i)Δx</em>i=1nρ(xi)Δx\bar{x} \approx \frac{\sum<em>{i=1}^{n} x</em>i \rho(x<em>i) \Delta x}{\sum</em>{i=1}^{n} \rho(x_i) \Delta x}
  • The exact center of mass is found by taking the limit as nn \to \infty:
    xˉ=<em>abxρ(x)dx</em>abρ(x)dx\bar{x} = \frac{\int<em>{a}^{b} x \rho(x) dx}{\int</em>{a}^{b} \rho(x) dx}
Example: Continuous System
  • Find the center of mass of an object with linear density ρ(x)=ax2\rho(x) = ax^2, where a > 0 and 0xL0 \le x \le L.
  • Apply the formula:
    xˉ=<em>0Lx(ax2)dx</em>0Lax2dx\bar{x} = \frac{\int<em>{0}^{L} x(ax^2) dx}{\int</em>{0}^{L} ax^2 dx}
    xˉ=a<em>0Lx3dxa</em>0Lx2dx\bar{x} = \frac{a \int<em>{0}^{L} x^3 dx}{a \int</em>{0}^{L} x^2 dx}
    xˉ=<em>0Lx3dx</em>0Lx2dx\bar{x} = \frac{\int<em>{0}^{L} x^3 dx}{\int</em>{0}^{L} x^2 dx}
    xˉ=x44<em>0Lx33</em>0L\bar{x} = \frac{\frac{x^4}{4} \Big|<em>0^L}{\frac{x^3}{3} \Big|</em>0^L}
    xˉ=L44L33\bar{x} = \frac{\frac{L^4}{4}}{\frac{L^3}{3}}
    xˉ=34L\bar{x} = \frac{3}{4}L

Mean Value of a Function

  • The mean value of a function f(x)f(x) over an interval [a,b][a, b] is needed to find a varying quantity.
  • Approximate the mean value by subdividing the interval into nn equal parts and averaging the function values at each point x<em>ix<em>i: 1n</em>i=1nf(xi)\frac{1}{n} \sum</em>{i=1}^{n} f(x_i)
  • Since Δx=ban\Delta x = \frac{b - a}{n}, we have n=baΔxn = \frac{b - a}{\Delta x}.
  • The mean value can be approximated as:
    1ba<em>i=1nf(x</em>i)Δx\frac{1}{b-a} \sum<em>{i=1}^{n} f(x</em>i) \Delta x
  • The exact mean value fˉ\bar{f} is:
    fˉ=lim<em>n1ba</em>i=1nf(x<em>i)Δx=1ba</em>abf(x)dx\bar{f} = \lim<em>{n \to \infty} \frac{1}{b-a} \sum</em>{i=1}^{n} f(x<em>i) \Delta x = \frac{1}{b-a} \int</em>{a}^{b} f(x) dx
  • Geometrically, the area under the curve of f(x)f(x) between aa and bb is equal to the area of a rectangle with height fˉ\bar{f} and width (ba)(b - a).
Example 1: Mean Value
  • Find the mean value of f(x)=x2f(x) = x^2 over the interval [0,1][0, 1]:
    fˉ=110<em>01x2dx\bar{f} = \frac{1}{1 - 0} \int<em>{0}^{1} x^2 dxfˉ=</em>01x2dx\bar{f} = \int</em>{0}^{1} x^2 dx
    fˉ=x3301\bar{f} = \frac{x^3}{3} \Big|_0^1
    fˉ=13\bar{f} = \frac{1}{3}
Example 2: Mean Value
  • Find the mean value of f(x)=sin(πx)f(x) = \sin(\pi x) over the interval [1,1][-1, 1]:
  • The function is odd-symmetric, meaning f(x)=f(x)f(-x) = -f(x).
  • The area under the curve cancels out, so the mean value should be zero.
    fˉ=11(1)<em>11sin(πx)dx\bar{f} = \frac{1}{1 - (-1)} \int<em>{-1}^{1} \sin(\pi x) dxfˉ=12</em>11sin(πx)dx\bar{f} = \frac{1}{2} \int</em>{-1}^{1} \sin(\pi x) dx
    fˉ=12[cos(πx)π]11\bar{f} = \frac{1}{2} \left[ -\frac{\cos(\pi x)}{\pi} \right]_{-1}^{1}
    fˉ=12π[cos(π)+cos(π)]\bar{f} = \frac{1}{2\pi} [-\cos(\pi) + \cos(-\pi)]
    fˉ=12π[(1)+(1)]=0\bar{f} = \frac{1}{2\pi} [-(-1) + (-1)] = 0

Root Mean Square Value

  • The mean value of a function is sometimes useless (e.g., when the function is anti-symmetric over the interval of integration).

  • The root mean square (RMS) value is introduced for a function f(x)f(x) defined on an interval [a,b][a, b] to obtain more information when the average is uninformative.

  • The RMS value is defined as the square root of the mean value of the square of the function:
    RMS=Mean Value of f(x)2RMS = \sqrt{\text{Mean Value of } f(x)^2}

    RMS=1baab[f(x)]2dxRMS = \sqrt{\frac{1}{b-a} \int_{a}^{b} [f(x)]^2 dx}

Example: Root Mean Square Value
  • Calculate the RMS value for the function f(x)=2cos(x)f(x) = 2\cos(x) over the interval [0,2π][0, 2\pi]:

    RMS=12π0<em>02π(2cos(x))2dxRMS = \sqrt{\frac{1}{2\pi - 0} \int<em>{0}^{2\pi} (2\cos(x))^2 dx}RMS=12π</em>02π4cos2(x)dxRMS = \sqrt{\frac{1}{2\pi} \int</em>{0}^{2\pi} 4\cos^2(x) dx}
    RMS=42π02πcos2(x)dxRMS = \sqrt{\frac{4}{2\pi} \int_{0}^{2\pi} \cos^2(x) dx}

  • Use the power reduction formula: cos2(x)=1+cos(2x)2\cos^2(x) = \frac{1 + \cos(2x)}{2}
    RMS=42π<em>02π1+cos(2x)2dxRMS = \sqrt{\frac{4}{2\pi} \int<em>{0}^{2\pi} \frac{1 + \cos(2x)}{2} dx}RMS=44π</em>02π(1+cos(2x))dxRMS = \sqrt{\frac{4}{4\pi} \int</em>{0}^{2\pi} (1 + \cos(2x)) dx}
    RMS=1π[x+sin(2x)2]02πRMS = \sqrt{\frac{1}{\pi} \left[ x + \frac{\sin(2x)}{2} \right]_{0}^{2\pi}}
    RMS=1π(2π+000)RMS = \sqrt{\frac{1}{\pi} (2\pi + 0 - 0 - 0)}
    RMS=2ππRMS = \sqrt{\frac{2\pi}{\pi}}
    RMS=2RMS = \sqrt{2}