Derive by the method of dimensions, an expression for the maximum velocity u for fluid flow through a circular tube. Assume that u depends on (i) the radius of the tube R, (ii) vis... Derive by the method of dimensions, an expression for the maximum velocity u for fluid flow through a circular tube. Assume that u depends on (i) the radius of the tube R, (ii) viscosity of the fluid η, (iii) pressure gradient (P/ℓ), ℓ is the length of the tube.

Question image

Understand the Problem

The question is asking us to derive an expression for maximum velocity in fluid flow through a circular tube using dimensional analysis, considering factors like tube radius, fluid viscosity, and pressure gradient.

Answer

$$ u = k \cdot \frac{P}{\ell \eta} $$
Answer for screen readers

The derived expression for maximum velocity is: $$ u = k \cdot \frac{P}{\ell \eta} $$

Steps to Solve

  1. Identify the Variables Define the variables that affect the maximum velocity $u$:
  • Tube radius $R$ (length)
  • Viscosity of the fluid $\eta$ (mass/time length)
  • Pressure gradient $\frac{P}{\ell}$ (force/length$^2$)
  1. Write the Dimensional Formulae Establish the dimensional formula for each variable:
  • Viscosity $\eta$ has dimensions $[M][L]^{-1}[T]^{-1}$
  • Pressure gradient $\frac{P}{\ell}$ has dimensions $[M][L]^{-1}[T]^{-2}$
  • Tube radius $R$ has dimensions $[L]$
  1. Establish the Relationship Using Dimensional Analysis Assume that maximum velocity $u$ can be expressed as: $$ u = k \cdot R^x \cdot \eta^y \cdot \left(\frac{P}{\ell}\right)^z $$ where $k$ is a constant.

  2. Determine the Dimensions of the Left Side The left side, maximum velocity $u$, has dimensions $[L][T]^{-1}$.

  3. Write the Dimensional Relationship Substituting the dimensions into the equation gives: $$ [L][T]^{-1} = k \cdot [L]^x \cdot [M][L]^{-1}[T]^{-1}^y \cdot [M][L]^{-1}[T]^{-2}^z $$

  4. Simplify the Right Side This results in: $$ [M]^{y+z} [L]^{x-y-1-z} [T]^{-y-2z} $$

  5. Equate Powers of Dimensions Set powers of each dimension equal to those on the left side:

  • For $M$: $y + z = 0$
  • For $L$: $x - y - 1 - z = 1$
  • For $T$: $-y - 2z = -1$
  1. Solve the Equations From $y + z = 0$, we can write $z = -y$.

Substituting into the other equations:

  • $x - y + 1 + y = 1 \implies x + 1 = 1 \implies x = 0$
  • $-y - 2(-y) = -1 \implies -y + 2y = -1 \implies y = -1$

Thus, $z = 1$.

  1. Final Expression The derived expression for maximum velocity is: $$ u = k \cdot \frac{P}{\ell} \cdot R^{0} \cdot \eta^{-1} $$ Hence, we simplify to: $$ u = k \cdot \frac{P}{\ell \eta} $$

The derived expression for maximum velocity is: $$ u = k \cdot \frac{P}{\ell \eta} $$

More Information

This result indicates that the maximum velocity in fluid flow through a circular tube is proportional to the pressure gradient and inversely proportional to the viscosity of the fluid. The constant $k$ depends on factors not specified in the problem.

Tips

  • Miscounting the dimensions when equating powers of $M$, $L$, and $T$.
  • Ignoring the dependency of other parameters when deriving the relationships; ensure all given factors are considered.

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