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Show that the equation pi a v = (4)/(3) pi a3 ( - ') g is dimensionally homogeneous.

Physics

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i. An equation is considered homogeneous if the dimensions of all terms on both sides of the equation are identical. This means that if you express each physical quantity in terms of its fundamental dimensions (mass [M][M], length [L][L], and time [T][T]), the resulting dimensional formula must be the same for every term in the equation.

ii. To show that the equation ηπav=43πa3(ρ−ρ′)g\eta \pi a v = \frac{4}{3} \pi a^3 (\rho - \rho') g is homogeneous, we need to determine the dimensions of each term on both sides.

  1. Identify the dimensions of each variable.

    • η\eta (coefficient of viscosity): [ML−1T−1][M L^{-1} T^{-1}] (given as kg m−1s−1\text{kg m}^{-1} \text{s}^{-1})
    • aa (radius): [L][L]
    • vv (speed): [LT−1][L T^{-1}]
    • ρ\rho (density): [ML−3][M L^{-3}]
    • ρ′\rho' (density): [ML−3][M L^{-3}]
    • gg (acceleration due to gravity): [LT−2][L T^{-2}]
    • π\pi and 43\frac{4}{3} are dimensionless constants.
  2. Calculate the dimension of the Left Hand Side (LHS).

    The LHS is ηπav\eta \pi a v.

    Dimension(LHS)=Dimension(η)×Dimension(a)×Dimension(v)\text{Dimension(LHS)} = \text{Dimension}(\eta) \times \text{Dimension}(a) \times \text{Dimension}(v) Dimension(LHS)=[ML−1T−1]×[L]×[LT−1]\text{Dimension(LHS)} = [M L^{-1} T^{-1}] \times [L] \times [L T^{-1}] Dimension(LHS)=[ML−1+1+1T−1−1]\text{Dimension(LHS)} = [M L^{-1+1+1} T^{-1-1}] Dimension(LHS)=[MLT−2]\text{Dimension(LHS)} = [M L T^{-2}]
  3. Calculate the dimension of the Right Hand Side (RHS).

    The RHS is 43πa3(ρ−ρ′)g\frac{4}{3} \pi a^3 (\rho - \rho') g.
    First, for terms to be subtracted, they must have the same dimensions. Since ρ\rho and ρ′\rho' are both densities, their dimensions are the same:

    Dimension(ρ−ρ′)=[ML−3]\text{Dimension}(\rho - \rho') = [M L^{-3}]

    Now, substitute all dimensions into the RHS expression:

    Dimension(RHS)=Dimension(a3)×Dimension(ρ−ρ′)×Dimension(g)\text{Dimension(RHS)} = \text{Dimension}(a^3) \times \text{Dimension}(\rho - \rho') \times \text{Dimension}(g) Dimension(RHS)=[L3]×[ML−3]×[LT−2]\text{Dimension(RHS)} = [L^3] \times [M L^{-3}] \times [L T^{-2}] Dimension(RHS)=[ML3−3+1T−2]\text{Dimension(RHS)} = [M L^{3-3+1} T^{-2}] Dimension(RHS)=[MLT−2]\text{Dimension(RHS)} = [M L T^{-2}]
  4. Compare the dimensions of the LHS and RHS.

    We found that:

    Dimension(LHS)=[MLT−2]\text{Dimension(LHS)} = [M L T^{-2}] Dimension(RHS)=[MLT−2]\text{Dimension(RHS)} = [M L T^{-2}]

    Since the dimensions of both sides of the equation are identical, the equation is dimensionally homogeneous.

    The equation ηπav=43πa3(ρ−ρ′)g\eta \pi a v = \frac{4}{3} \pi a^3 (\rho - \rho') g is indeed homogeneous.

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