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Super chlorination; overflow rate 5000 L/m2/h

Short answer

Super‑chlorination is used during epidemics, for new mains, or poor‑quality water; break‑point chlorination gives stable free residual, oxidizes ammonia, and removes tastes. For overflow rate 5000 L/m²/h (0.1389 cm/s) at 20°C: 0.06 mm vs=0.3215 cm/s, removed 100%; 0.03 mm vs=0.0804 cm/s, removed 57.9%.

When is super chlorination recommended in a water supply scheme? Write about the advantages of break point chlorination. A settling tank is designed for an overflow rate of 5000 liters per m2^2 per hour. What percentage of particles of diameter 0.06 mm and 0.03 mm will be removed in this tank? Temperature of water is 20°C and specific gravity of particles is 2.65.

When super-chlorination is recommended

Super-chlorination (a dose far above the demand, followed by de-chlorination) is used:

  • during epidemics of cholera, typhoid, hepatitis, etc.;
  • when a new main, pipe or tank is commissioned or repaired;
  • when the raw water is of highly variable or very poor quality, or the plant is overloaded;
  • when the contact time is short (so a high dose compensates);
  • for emergency or camp supplies and when pre-treatment is poor. The dose is 3 to 15 mg/l and the excess is removed by sulphur dioxide, sodium thiosulphate or activated carbon.

Advantages of break-point chlorination

  • Oxidises ammonia, organic matter and iron/manganese completely, which removes most tastes and odours.
  • Kills pathogens and algae far more effectively than combined chlorine, including organisms that resist chloramines.
  • Gives a stable free residual which protects the distribution system against recontamination.
  • The chlorine demand is fully satisfied and known, so the dose can be controlled accurately.

Numerical: removal in the settling tank

Overflow rate v0=5000v_0 = 5000 l/m²/h =5= 5 m³/m²/h:

v0=53600=1.389×10−3 m/s=0.1389 cm/sv_0 = \frac{5}{3600} = 1.389\times10^{-3}\ \text{m/s} = 0.1389\ \text{cm/s}

At 20 °C, ν=0.01007\nu = 0.01007 cm²/s, Ss=2.65S_s=2.65, g=981g=981 cm/s². By Stokes' law, vs=g(Ss−1)d218νv_s = \dfrac{g(S_s-1)d^2}{18\nu}.

Particle 0.06 mm (0.006 cm):

vs=981×1.65×0.006218×0.01007=0.3215 cm/sv_s = \frac{981\times1.65\times0.006^2}{18\times0.01007} = 0.3215\ \text{cm/s}

Re=0.19<1Re = 0.19 < 1 (Stokes' law holds). Since vs=0.3215v_s = 0.3215 > v0=0.1389v_0=0.1389 cm/s, the particles are removed 100 %.

Particle 0.03 mm (0.003 cm):

vs=981×1.65×0.003218×0.01007=0.0804 cm/sv_s = \frac{981\times1.65\times0.003^2}{18\times0.01007} = 0.0804\ \text{cm/s}

Re=0.02<1Re = 0.02<1. As vs<v0v_s<v_0, the removal is

vsv0=0.08040.1389=0.579⇒57.9 %\frac{v_s}{v_0} = \frac{0.0804}{0.1389} = 0.579 \Rightarrow 57.9\ \%

Answer: 0.06 mm particles: 100 % removed; 0.03 mm particles: 57.9 % removed.

✓ Answer checked by Claude Opus 5.5 (high effort)

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