43

Narrow tank productivity in the 46 spectra. Henry Young 1982

Embed Size (px)

Citation preview

Page 1: Narrow tank productivity in the 46 spectra. Henry Young 1982
Page 2: Narrow tank productivity in the 46 spectra. Henry Young 1982
Page 3: Narrow tank productivity in the 46 spectra. Henry Young 1982
Page 4: Narrow tank productivity in the 46 spectra. Henry Young 1982
Page 5: Narrow tank productivity in the 46 spectra. Henry Young 1982

Narrow tank productivity in the 46 spectra. Henry Young 1982

Page 6: Narrow tank productivity in the 46 spectra. Henry Young 1982

Narrow tank productivity in the 46 spectra. Henry Young 1982

Page 7: Narrow tank productivity in the 46 spectra. Henry Young 1982

35 kW / m x 400 km = 14 GW

Installed capacity (2009) = 12.2 GW

Planned 19 GW

Peak demand ~ 6 GW

14 GW x 8760 hours = 122 TWH

Annual Scottish demand = 29 TWH

Ratio 4.2

Page 8: Narrow tank productivity in the 46 spectra. Henry Young 1982

Narrow tank freak wave tests 1978

Page 9: Narrow tank productivity in the 46 spectra. Henry Young 1982
Page 10: Narrow tank productivity in the 46 spectra. Henry Young 1982
Page 11: Narrow tank productivity in the 46 spectra. Henry Young 1982
Page 12: Narrow tank productivity in the 46 spectra. Henry Young 1982
Page 13: Narrow tank productivity in the 46 spectra. Henry Young 1982

Inflation from1998 to 2013 is 1.43

Page 14: Narrow tank productivity in the 46 spectra. Henry Young 1982

2013 – 1982 = 31 years

Cable length 43 km = 1333 km years.

At 10 km years per fault this is 133 faults.

From Lords Select Committee on European Communities HL paper 88 May 1988

Page 15: Narrow tank productivity in the 46 spectra. Henry Young 1982

What’s wrong with wave energy?

Control by nuclear people >False information

Impatient investors >Unreliable components > Ignorance of stresses

Waste of sea front by solo devices

Inadequate installation equipment

Preference for vertical motion.

Page 16: Narrow tank productivity in the 46 spectra. Henry Young 1982

No names, no pack drill.

Page 17: Narrow tank productivity in the 46 spectra. Henry Young 1982

Unswept flow passage ≡ leaky pipe

Page 18: Narrow tank productivity in the 46 spectra. Henry Young 1982

Open flow field Power1

2 Area Velocity

316

27

Duct Power g Area Velocity Head

Page 19: Narrow tank productivity in the 46 spectra. Henry Young 1982
Page 20: Narrow tank productivity in the 46 spectra. Henry Young 1982

R.A. McAdam , G.T. Houlsby , M.L.G. OldfieldStructural and Hydrodynamic Model Testing of the Transverse

Horizontal Axis Water Turbine EWTEC 2011

Page 21: Narrow tank productivity in the 46 spectra. Henry Young 1982
Page 22: Narrow tank productivity in the 46 spectra. Henry Young 1982
Page 23: Narrow tank productivity in the 46 spectra. Henry Young 1982

Edinburgh vertical-axis, variable-pitch with rim power take off.

EWTEC Patras 1998

Page 24: Narrow tank productivity in the 46 spectra. Henry Young 1982
Page 25: Narrow tank productivity in the 46 spectra. Henry Young 1982
Page 26: Narrow tank productivity in the 46 spectra. Henry Young 1982
Page 27: Narrow tank productivity in the 46 spectra. Henry Young 1982

Edinburgh vertical-axis, variable-pitch with rim power take off.

EWTEC Patras 1998

Page 28: Narrow tank productivity in the 46 spectra. Henry Young 1982
Page 29: Narrow tank productivity in the 46 spectra. Henry Young 1982
Page 30: Narrow tank productivity in the 46 spectra. Henry Young 1982

Cells are 1 minute of arc lat. 1.5 minutes long = 2.617 km2.

Power = 6.165 TW x CfCourtesy Proudman Labs

Page 31: Narrow tank productivity in the 46 spectra. Henry Young 1982

From Black and Veatch 2011.

Using values for the Pentland Firth U = 3m/s, ρ = 1025 kg/m3, channel length = 23 km,

channel width = 10 km

in combination with a more appropriate bed friction coefficient CD = 0.0015 energy dissipated due to bed friction averaged over a tidal cycle calculated is 4.05 GW.

Page 32: Narrow tank productivity in the 46 spectra. Henry Young 1982

Laminaria Hyperborea (kelp) are found along the

edges of the Pentland Firth at depths up to 30 m.

Length can reach 3.5 metres.

Cf = ?

Page 33: Narrow tank productivity in the 46 spectra. Henry Young 1982

Pentland bed stills. P Hayes. Fisheries Research Aberdeen 2006-8

68 mm bob

Page 34: Narrow tank productivity in the 46 spectra. Henry Young 1982
Page 35: Narrow tank productivity in the 46 spectra. Henry Young 1982
Page 36: Narrow tank productivity in the 46 spectra. Henry Young 1982

70 60 50 40 30 20 10 0 10 20 30 40 50 60 700

0.2

0.4

0.6

0.8

1

1.2Downstream force on a 140 diameter rotor as a fraction of ideal

1.2

0

fdsi 4

FDSi 4

DR

2

DR2

Xi

Page 37: Narrow tank productivity in the 46 spectra. Henry Young 1982
Page 38: Narrow tank productivity in the 46 spectra. Henry Young 1982
Page 39: Narrow tank productivity in the 46 spectra. Henry Young 1982
Page 40: Narrow tank productivity in the 46 spectra. Henry Young 1982

What’s wrong with tidal stream designs?

Ignorance of flow impedance.

> Wrong energy input

Open flow field equation in a ‘duct’ > Swept area too small

Wrong blade support > Bearing load levered up

Cramped power compartment

Tip vortex losses

Page 41: Narrow tank productivity in the 46 spectra. Henry Young 1982

Google images

Page 42: Narrow tank productivity in the 46 spectra. Henry Young 1982

Speed up x 30Range up x 6000

Payload up x 20,000Cost per ton-mile down ÷ 100

Google images

Page 43: Narrow tank productivity in the 46 spectra. Henry Young 1982

Something for the simpletons