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Workshop/6 min exploration

Inside a Pelton turbine

Why does turning a water jet backward turn a turbine forward?

A Pelton turbine operates in air. Water accelerates through a nozzle and strikes the ridge between two curved cups. The cups split the jet and turn it back toward either side of the wheel. That change in momentum pushes the buckets forward. The bucket meeting the jet centerline turns orange; watch the next bucket take its place.

3D model

Explore the model and follow its moving parts.

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The nozzle sets the jet speed. The buckets extract power by redirecting the jet while moving slower than it.

At fixed nozzle head, what happens to ideal flow when effective jet diameter doubles?

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How the parts work together

  1. Meet the splitter

    Pause and follow the jet to the orange bucket on the upper-left side of the runner. Orbit to inspect its central ridge. Two cups turn the water toward opposite sides, avoiding a sustained one-sided axial push in this symmetric model. Play again to watch the next bucket receive the jet.

  2. Give the jet more head

    Raise head from 200 to 400 m with the jet diameter fixed. The ideal jet speed rises by √2. Since the same opening now passes faster water, flow also rises by √2; incoming hydraulic power rises by 2√2.

  3. Widen the jet

    Return to 200 m and increase jet diameter. Its cross-sectional area grows with diameter squared, so doubling diameter would quadruple flow and ideal power at fixed head and speed ratio.

  4. Match the runner to the jet

    At low runner speed, buckets exert strong turning force but move slowly. Near jet speed, they capture little momentum. With a fixed 165° relative-flow turn and no bucket friction, this model peaks at a rim speed equal to half the jet speed. Actual turbine efficiency includes further losses.

The main parts

Nozzle & spear
The taper accelerates water into a free jet. A central spear regulates the opening in a real injector. Here the control specifies an effective circular jet diameter; the visible spear shift is illustrative, not a calibrated valve-flow model.
Paired cups & splitter
Each of the eighteen buckets has two concave cups meeting at a central ridge. The jet divides toward opposite sides of the shaft. Orange identifies the bucket meeting the center of the jet, so the highlight passes from bucket to bucket as the runner turns.
Runner disc
The bucket stems meet a common disc. All buckets turn rigidly with the disc and shaft. The geometry is an original teaching assembly with a half-metre pitch radius, not the CAD of a commercial runner.
Shaft & coupling
The shaft leaves the wheel perpendicular to its plane, passes through two bearings, and ends at a bolted coupling. Mechanical power is torque multiplied by angular speed. A generator is outside this cutaway.
Two bearing supports
Two bored housings support the shaft on opposite sides of the runner. Pedestals and feet connect them to the base. Bearing lubrication, friction and loads are not solved.
Splash casing
The casing catches discharged water. Its backplate has a real shaft opening; the cutaway removes the front face to expose the working parts. Unlike a reaction turbine, this runner is not submerged in a pressurized casing.
Jet & split discharge
Blue lines sample the width of the free jet and stop at their individual first bucket contacts. They represent paths, not solid cylinders of water. The two discharge ribbons indicate the split toward opposite sides; they are schematic direction cues, not computed water trajectories.
Drain tray
Spent water falls below the runner and leaves the open collection tray. The nozzle head is specified independently of this illustrative drain height.

One discovery leads to another.

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