Pipes in parallel

Dr. Huidae Cho
Department of Civil and Environmental Engineering...New Mexico State University

1   Learning objectives

  • Understand flow distribution in parallel pipe systems
  • Apply continuity and energy principles to parallel pipes
  • Compute flow split using proportional and iterative methods
  • Interpret how diameter, length, and roughness affect flow
  • Solve practical engineering problems involving parallel pipelines

Key points

  • Equal head loss governs the system
  • Flow adjusts based on hydraulic resistance

2   Concept

  • Multiple pipes connect the same upstream and downstream nodes
  • Flow splits into branches and recombines
  • Common in water distribution and bypass systems

Key points

  • Same endpoints → same energy drop
  • Flow distribution is not equal

3   Governing principles

3.1   Continuity

$$ Q = Q_1 + Q_2 + \cdots + Q_n $$

3.2   Energy (head loss equality)

$$ h_{L1} = h_{L2} = \cdots = h_{Ln} $$
  • All parallel pipes experience the same head loss

Key points

  • Equal head loss, not equal discharge

4   Head loss models

4.1   Darcy–Weisbach

$$ h_L = f \frac{L}{D} \frac{V^2}{2g} $$ $$ Q = VA $$ $$ h_L \propto \frac{L}{D^5} Q^2 $$

4.2   Hazen–Williams

$$ h_L = K Q^{1.852} $$
  • Common in water systems
  • Nonlinear relation between $h_L$ and $Q$

5   Flow distribution

$$ h_{L1}(Q_1) = h_{L2}(Q_2) $$ $$ Q = Q_1 + Q_2 $$
  • Larger, shorter, smoother pipes carry more flow
  • Smaller, longer, rougher pipes carry less flow

Key points

  • Distribution depends on resistance

6   Solution strategy

6.1   Procedure

  1. Assume $Q_1$
  2. Compute $Q_2 = Q - Q_1$
  3. Compute $h_{L1}$ and $h_{L2}$
  4. Adjust until the two head losses are equal

6.2   Numerical methods

  • Trial-and-error
  • Spreadsheet solver
  • Newton method (advanced)

Key points

  • Iteration is standard

7   Worked example 1: same material pipes

  • Same $L$, same roughness
  • $D_1 = 0.30$ m, $D_2 = 0.15$ m
  • $Q = 0.12$ m3/s

7.1   Step 1

$$ \frac{Q_1^2}{D_1^5} = \frac{Q_2^2}{D_2^5} $$

7.2   Step 2

$$ \frac{Q_1}{Q_2} = \left( \frac{D_1}{D_2} \right)^{2.5} $$ $$ \frac{Q_1}{Q_2} = 2^{2.5} \approx 5.66 $$

7.3   Step 3

$$ Q = Q_1 + Q_2 = 0.12 $$
  1. Let $Q_2 = x$, then $Q_1 = 5.66x$
  2. \[ 5.66x + x = 0.12 \]
  3. \[ x = 0.018 \]
  4. \[ Q_1 = 0.102,\quad Q_2 = 0.018 \]

7.4   Interpretation

  • Large pipe dominates flow

8   Worked example 2: iterative solution

  • $L_1 = L_2 = 100$ m
  • $D_1 = 0.20$ m, $D_2 = 0.15$ m
  • $Q = 0.10$ m3/s

8.1   Step 1: initial guess

  1. Try $Q_1 = 0.05$ and $Q_2 = 0.05$
  2. The smaller pipe has the larger head loss for the same flow
  3. So Pipe 2 is carrying too much flow

8.2   Step 2

  1. Adjust the guess to $Q_1 = 0.07$ and $Q_2 = 0.03$
  2. Compare the two head losses using $$ \frac{h_{L1}}{h_{L2}} = \frac{Q_1^2 / D_1^5}{Q_2^2 / D_2^5} $$
  3. The ratio is about $0.88$
  4. This means $h_{L1} < h_{L2}$, so increase $Q_1$ slightly

8.3   Step 3

  1. Try $Q_1 \approx 0.072$ and $Q_2 \approx 0.028$
  2. Now the two head losses are approximately equal

8.4   Final answer

$$ Q_1 \approx 0.072,\quad Q_2 \approx 0.028 $$

9   Physical interpretation

  • Flow redistributes to equalize energy loss
  • The lower-resistance branch carries more flow
  • The system naturally balances resistance and discharge

10   Common mistakes

  • Assuming equal flow
  • Ignoring nonlinear dependence
  • Mixing formulas incorrectly
  • Ignoring minor losses

11   Quick check

  • If Pipe 2 becomes rougher:
  1. $Q_2$ decreases
  2. Flow shifts to Pipe 1

12   Key points

  • Equal head loss controls flow split
  • Diameter strongly affects flow
  • Iteration is usually required
  • Always satisfy continuity and energy