Efflux Jets from a Tank

tools.tank-jets.intro

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The fastest jet is not the one that goes furthest 🖖

Read the three speeds against the three ranges. The bottom hole is the fastest at 4.20 m/s and lands 1.039 m out. The top hole is the slowest at 2.43 m/s and lands at 1.039 m — the same spot. The middle hole, at 3.43 m/s, beats them both with 1.200 m. Depth buys speed and spends flight time, and the product of the two peaks in between rather than at either end.

The best range is the water depth, exactly 🖖

The range from a hole at depth y is 2√(y(H − y)), which is largest at y = H/2 and equals H there. Not close to H. The panel reads 1.200 m from a 1.2 m depth, and it will read your depth back to you whatever you set it to. It also explains the pairing: y and H − y give the same product, so holes at 0.30 m and 0.90 m water the same spot — which is what the Symmetric Twin Holes preset is showing.

Nothing in the speed is about the liquid 🖖

v = √(2gy) contains no density and no viscosity, so mercury leaves the hole at the same speed as water. The extra weight driving the heavier liquid is exactly the extra inertia resisting it, and the two cancel. The substance enters this page in one place only: the velocity coefficient. Switch it to 0.97 and the jet leaves at 97% of the ideal speed — that 3% is the whole of the real fluid.

Problem solved in full

  1. Two holes, one wet spot 6 steps

    A tank is kept full to 1.20 m. Three holes are drilled in the side of it, 0.30 m, 0.60 m and 0.90 m above the table it stands on. Work out where each jet lands, and find the height that throws the water furthest.

    1. Water leaving a hole has been pushed by the depth above it and by nothing else. That pressure buys it exactly the speed a dropped stone would have after falling the same distance, which is Torricelli's result. The lowest hole has 0.90 m of water over it.

    2. Out in the air the jet is a projectile fired horizontally, so how long it stays up is decided by how far it has to fall. The depth above the hole sets the speed. The height below the hole sets the time.

    3. Multiply the two and g cancels out of the answer. A jet on the Moon leaves slower and hangs in the air longer, and it lands on the same spot.

    4. The range only ever sees the product of the depth above and the height below, and those two always add up to H. Swapping y for H โˆ’ y leaves the product alone, so the hole at 0.90 m throws exactly as far as the hole at 0.30 m.

    5. Two numbers with a fixed sum multiply to the most when they are equal, which puts the best hole halfway up. Depth above and height below are then both H/2, and the range comes out at H on the nose.

    6. So no tank throws water further along the table than it is deep, whatever you do with the drill. And the twins land together without arriving together: the upper jet is airborne for 0.4284 s against the lower one's 0.2473 s, so the wet spot is hit twice, 0.18 s apart.

    Answer

    4.20 m/s out of the lowest hole, landing 1.039 m out. The hole at 0.90 m lands there too. The middle hole reaches 1.200 m, which is as far as a 1.20 m tank can throw. R = 2โˆš((H โˆ’ y)y) has no g in it and is symmetric about the midpoint, so every hole but the middle one has a partner in the wall that lands on the same spot.

Learning path

Water out of a tank: one speed, spent two ways

Leads to The tank emptying the efflux speed, and the fact that it follows the square root of the depth rather than the depth.

References (1)
  • Original formulation of Torricelli's law for liquid efflux speed from an orifice: E. Torricelli, De motu gravium naturaliter descendentium. Florence, 1644.

Example problems