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1. a) State the conditions which are necessary for a physical equation to be correct.

A physical equation must satisfy two main conditions to be considered correct:

  • Dimensional Homogeneity: The dimensions of all terms on both sides of the equation must be identical. This means that the units on the left-hand side must match the units on the right-hand side.
  • Numerical Correctness: The equation must be numerically accurate, meaning the constants and relationships within the equation must be verified by experimental data or derived from established physical principles.

1. b) Show that this equation is homogeneous.

The given equation is for the rate of flow of a liquid:

Vt=πPr48ηL\frac{V}{t} = \frac{\pi P r^4}{8 \eta L}

To show that this equation is homogeneous, we need to verify that the dimensions of the Left Hand Side (LHS) are equal to the dimensions of the Right Hand Side (RHS).

  • Step 1: Identify the dimensions of each variable.

    • Volume (VV): [L3][L^3]
    • Time (tt): [T][T]
    • Pressure (PP): Force per unit area. Force has dimensions [MLT−2][MLT^{-2}], and area has dimensions [L2][L^2]. So, [P]=[MLT−2][L2]=[ML−1T−2][P] = \frac{[MLT^{-2}]}{[L^2]} = [ML^{-1}T^{-2}]
    • Radius (rr): [L][L]
    • Length (LL): [L][L]
    • Coefficient of viscosity (η\eta): Given in units of Nsm−2N s m^{-2}. NN (Newton) is a unit of force, so [N]=[MLT−2][N] = [MLT^{-2}]. ss (second) is a unit of time, so [s]=[T][s] = [T]. m−2m^{-2} (meter squared inverse) is a unit of length squared inverse, so [m−2]=[L−2][m^{-2}] = [L^{-2}]. So, [η]=[MLT−2]⋅[T]⋅[L−2]=[ML−1T−1][\eta] = [MLT^{-2}] \cdot [T] \cdot [L^{-2}] = [ML^{-1}T^{-1}]
    • π\pi and 8 are dimensionless constants.
  • Step 2: Determine the dimensions of the Left Hand Side (LHS). The LHS is Vt\frac{V}{t}.

    Dimensions of LHS=[L3][T]=[L3T−1]\text{Dimensions of LHS} = \frac{[L^3]}{[T]} = [L^3T^{-1}]
  • Step 3: Determine the dimensions of the Right Hand Side (RHS). The RHS is πPr48ηL\frac{\pi P r^4}{8 \eta L}. We ignore the dimensionless constants π\pi and 8. First, find the dimensions of the numerator Pr4P r^4:

    [Pr4]=[ML−1T−2]⋅[L4]=[ML(−1+4)T−2]=[ML3T−2][P r^4] = [ML^{-1}T^{-2}] \cdot [L^4] = [ML^{(-1+4)}T^{-2}] = [ML^3T^{-2}]

    Next, find the dimensions of the denominator ηL\eta L:

    [ηL]=[ML−1T−1]⋅[L]=[ML(−1+1)T−1]=[MT−1][\eta L] = [ML^{-1}T^{-1}] \cdot [L] = [ML^{(-1+1)}T^{-1}] = [MT^{-1}]

    Now, combine these to find the dimensions of the RHS:

    Dimensions of RHS=[ML3T−2][MT−1]\text{Dimensions of RHS} = \frac{[ML^3T^{-2}]}{[MT^{-1}]} =[M(1−1)L3T(−2−(−1))]= [M^{(1-1)} L^3 T^{(-2 - (-1))}] =[M0L3T(−2+1)]= [M^0 L^3 T^{(-2+1)}] =[L3T−1]= [L^3T^{-1}]
  • Step 4: Compare the dimensions of the LHS and RHS. Dimensions of LHS = [L3T−1][L^3T^{-1}] Dimensions of RHS = [L3T−1][L^3T^{-1}] Since the dimensions of both sides of the equation are identical, the equation is dimensionally homogeneous.

The equation is homogeneous.

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