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(1)

Renewable Energy Technologies I – WS05/06

1

Solution to Exercise Nr. 8 Design of a CPC for a Solar Furnace 1.

( ) 1000 0.85 0.553085 sin 45º 4.65 3.43mrad

C sin

2 error

2 error

rim 2 or concentrat heliostat

max = =

+

=

θ ρ φ

ρ

2. Losses in power and concentration are due to geometrical imperfections (such as heliostat flatness, facets misalignment, structural bending and deformations, and a segmented approximation to the exact parabolic profile), optical imperfections (such as the reflectivity and specularity of the mirrors and glass absorption), shading effects (such as shading caused by the venetian shutter, receiver, and the non-reflective space or frame around each mirror facet), and tracking imperfections.

3. Fig. 2, for aperture diameter 5 cm: C~

= 4200.

K 2934 )

K W/(m² 10

5.67

4200 m

/ W 1000 C~

T I

25 . 0 4 8

- 25 2

. 0

stagnation ⎟⎟ =

⎜⎜

=

⎟⎟

⎜⎜

=⎛ ⋅ σ 4.

( ) 0 T 1457K

4 C~ I T T

T 75 . 0

Toptimal5 L optimal4 L ⎟⎟= optimal

⎜⎜

σ

5.

Φ 45º 30º

rout 2.5 cm 2.5 cm

CCPC = sin-2Φ 2 4

rin = rout·(CCPC)0.5 3.54 cm 5.0 cm L = (rin+rout)·cotΦrim 6.04 cm 13.0 cm

(2)

Renewable Energy Technologies I – WS05/06

2 6.

Φ 45º 30º

CCPC 2 4

rin 3.54 cm 5.0 cm

Qsolar (Fig 2) ≈14 kW ≈20 kW

C~

(Fig 2) ≈3500 ≈2600

ηAcceptance (For Φrim = 45º) 100% 41.8%

CPC reflectivity ρ 0.9 0.9

Total Power = Qsolar⋅ρ⋅ηAcceptance ≈12.6 kW ≈7.6 kW Total Mean Concentration =

C~CCPC⋅ρ⋅ηAcceptance

≈6300 ≈3900

7.

Φ 45º 30º

Total Mean Concentration = C~CCPC⋅ρ⋅ηAcceptance

≈6300 ≈3900

Tstagnation 3247 K 2880 K

Toptimal 1576 K 1434 K

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