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Turning The Tide Towards a Low Carbon Future:
A Novel New Design for The Severn Barrage
Rod Rainey
Director, Rod Rainey & Associates Ltd., www.RRandA.co.uk
Rod Rainey & Associates Ltd
What is the most important principle in Engineering?• Newton’s laws of motion
• First law of thermodynamics
• Navier-Stokes equation
• Second law of thermodynamics
• Maxwell’s equations
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None of the above!
The most important principle in Engineering is:
“If it ain’t broke, don’t fix it”
Engineering, like medicine, proceeds mainly by trial-and-error – the role of engineers in society is mainly to remember what worked last time, and keep doing it.
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Features of La Rance design
• Size of entry/exit ports maximised to minimise kinetic energy loss in exit jet
• Taper of ducts limited to preserve duct flow
• Hence large barrage size, to minimise turbine size
• Concrete construction has advantage of maximising weight, which is helpful to foundations
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But for the Severn, the La Rance design is “broke”, for 2 reasons
• Uneconomic. 2010 DECC Report found cost to be 30p/kWh, compared with 10p/kWh for offshore wind
• Tidal range upstream reduced by factor of 2, reducing inter-tidal habitat by a much larger factor, because of concave estuary cross-section. Very bad for migrating birds. Also some shipping relies on high tides.
So, under the First Principle of Engineering, we can try to “fix it”
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Theory of tidal power barragesGarrett and Cummins (2004) consider a small bay of area A:
and vary the flow resistance of turbines to maximise the average power, which they show to be:
¼ρgAωa2
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This result is best appreciated with the standard electrical analogy (pressure = voltage, volume flow rate = current)
As the resistance varies the point A describes a semicircle, and the power is proportional to the area of the triangle (shaded)
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But why not make the turbine resistance a reactance?
That way, the pre-barrage tidal range in the bay can be kept unchanged, and the power also increased – a win-win situation
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Required pressure-flow characteristic of turbine
Characteristic of resistive component (yellow), inductive component (blue) and combined characteristic (red/green). Red = pumping.
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Power output (before conversion losses) over tidal cycle
The pumping power is surprisingly small – less than 4% of the generated power. The pumping energy is even less – only 0.65%
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The breast-shot water wheel
The blades act like the vanes in a vane pump, not the paddles in a paddle-steamer. Unlike a turbine, when the wheel stops, so does the flow, as required at points “B” in the characteristic.
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A 200-year-old concept, e.g. Claverton Pumping Station
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Photos courtesy www..claverton.org
Recent application is small-scale hydropower in developing countries. Tests show high efficiency.
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From G. Muller et.al., ICE J. Engineering Sustainability, Vol 157, paper 13806
Hydraulic power take-off for Severn Barrage
• A hydraulic power take-off, used on construction machinery and some wind turbines, functions like a gearbox with infinitely-adjustable gear ratio.
• Coupled to a synchronous generator/motor which runs at constant speed, it allows us to set any flow rate and hence follow the required elliptical characteristic
• No hydraulic motors exist for our size, so twin hydraulic rams with brake calipers can be used, alternately gripping a brake disc, like a strand jack.
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For the Severn we need extra elements in the circuit
The reservoir has a resistance added to model seabed friction, giving it an overall impedance Z1, and the imperfect access to the open ocean gives it a source impedance Z2
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Outgoing tidal wave generated by barrage (gives Z2)
Wave amplitude (blue) and phase (green). Note “kink” at abrupt channel width increase at Section A. See JFM vol 636 pp 497-507
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Annual-average power, before conversion losses
For a site between C and D, power = 6GW, or 4GW after conversion losses
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Environmental impact, with head across barrage 0.6 ×pre-barrage tidal amplitude (range/2), see last slide
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Jurassic Limestone (Lias) cliffs at Nash Point Rod Rainey & Associates Ltd
This formation extends under the sea almost to Hurlstone Point, as level bare rock ideal for piled foundations
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hydraulic rams
calipers
support frame
roller bearing
bearing cradle
water wheel
brake disc
Barrage construction, installation, maintenance
• Plated steel construction, like a ship. Extensive use of corrugated plate, like the bulkheads in a modern tanker, to minimise fabrication cost. Wheel can also be rotated for fabrication, to avoid working at height.
• Wheel and cradle will float, to ease installation. Cradle piles fit into holes in rock seabed, pre-drilled through a template. Similar limestone is drilled in quarries for explosives, at rates of 10m/hr.
• All machinery in air and accessible by road, for ease of maintenance. Wheel, with bearings, can be floated out for maintenance
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Rotating workpiece for automatic weldingRod Rainey & Associates Ltd
Photo courtesy Quoceant Ltd. www.quoceant.com
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HIGH TIDE
Water wheel can be floated out and removed by an anchor-handling tug
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HIGH TIDE
15mm plate. Drum used for buoyancy during float-out
50 m
30 m
20 mm plate
Stresses in water wheel bladesAssume corrugated wheel blades 10m wide with 1.111m wide corrugations in 15mm thick steel plate, and 2.5m head (0.025 MPa) pressure loading:
• Local bending stress in face = (0.025×1.1112/12)×0.0075/(0.0153/12) = 69 MPa
• Bending of 10m long corrugation = {(0.025×3×1.111×102/12)×1.111×√3/4}/
{2×1.111×0.015×(1.111×√3/4)2×(4/3)} = 32 MPa
• This compares with a Code fatigue stress range (at 108 cycles ≈ 200 years) of 70 MPa for plain steel, 30 MPa for Class E welded joint
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Stresses around calipers
• Torque on water wheel at 2.5m head (0.025 MPa) = 0.025×10×50×10 = 125 MN-m
• Force on each caliper = (125/2)/15 = 4.2 MN
• Assuming 5m long caliper and 20mm thick disc, stress = 4.2/(5×0.02) = 42 MPa
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Weight of steel in water wheel• Blades: 8×50×10×(4/3)×0.015×7.85 = 628 tonnes
• Drum: 50×10π×0.015×7.85 = 185 tonnes
• Internal bulkheads: 4×302×(π/4)×0.015×7.85 = 332 tonnes
• End bulkheads: 2×302×(π/4)×2×0.02×7.85 = 444 tonnes
• Total = 628+185+332+444 = 1600 tonnes
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Plating continued underneath, for torsional strength, and also to allow cradle to be floated out as a barge, and then ballasted down into holes pre-drilled on the seabed through a template
10mm plate
Stresses in cradle platingAssume corrugated panels 10.5m wide with 0.8m wide corrugations in 10mm thick steel plate, and 2.5m head (0.025 MPa) pressure loading:
• Local bending stress in face = (0.025×0.82/12)×0.005/(0.013/12) = 80 MPa
• Bending of 10m long corrugation = {(0.025×3×0.8×10.52/12)×0.8×√3/4}/
{2×0.8×0.01×(0.8×√3/4)2×(4/3)} = 75 MPa
• This compares with a yield strength of 355 MPa – the large margin is typical of prudent conceptual design practice.
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Weight of steel in cradle and support structure• Plating: {55×(13+5)+11×20}×2×(4/3)×0.01×7.85 = 253 tonnes
• Piles: {2×70+4×30}×2π×0.03×7.85 = 385 tonnes
• Cross-beam: 60×(2×2+2×√2)×0.02×7.85 = 64 tonnes
• Breast and filler plates: (55×13×0.02+10×30π×0.01)×7.85 = 186 tonnes
• Total = 253+385+64+186 = 900 tonnes
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Comparison with Beatrice offshore wind farm
• Beatrice wind turbines are 7MW max, so about 3MW annual-average. By comparison, annual-average power of single waterwheel is 4,000/250 = 16 MW.
• Beatrice wind turbines weigh about 300 tonnes, and have 865 tonne substructures, anchored by 500 tonnes of piles. So 1650 tonnes in all. By comparison, water wheels weigh 1600+900 = 2500 tonnes.
• So Severn Barrage is less than one third the steel weight, per unit energy. Installation and maintenance also easier – no cranes needed.
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