Power Curve and Design Optimization of Drag Power Kites
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1 Institute for Electrical Drive Systems and Power Electronics, Department of Electrical Engineering and Information Technology, Technische Universität München Power Curve and Design Optimization of Drag Power Kites Florian Bauer, R. Kennel, C. Hackl, F. Campagnolo, M. Patt, R. Schmehl October 5th, 2017, Airborne Wind Energy Conference 2017, Freiburg, Germany
2 2
3 How does an optimal drag power kite look like? 2
4 How does an optimal drag power kite look like?... and what are the sensitivities of design parameters? 2
5 Outline 1. Model Derivation 2. Power Curve Optimization 3. Design Parameter Optimization 4. Parameter Studies 5. Conclusions 3
6 Kinematics 4
7 Assumption 1: Loyd s model (extended) 5
8 Assumption 1: Loyd s model (extended) v a = cos(ϕ) cos(ϑ)v w C 2 L +(C D,eq + C D,rot ) 2 C D,Σ 5
9 Assumption 1: Loyd s model (extended) v a = cos(ϕ) cos(ϑ)v w C 2 L +(C D,eq + C D,rot ) 2 C D,Σ Assumption 2: azimuth and elevation are constant effective values 5
10 Kinematics Kite Aerodynamics 6
11 cf.: D. Vander Lind. Airfoil for a flying wind turbine. US Patent 9,709,026. July
12 8
13 CFD result 8
14 CFD result Assumption 3: quadratic approximation c D = c D,0 + c D,2 c 2 L 8
15 Assumption 4: thin airfoil C L = c L 1+ 2 A with A = b2 A/n mw C D,k = c D + C2 L πea C D,k,i + C D,k,a + C D,k,o cf.: J. Katz and A. Plotkin. Low-Speed Aerodynamics. Cambridge Aerospace Series. Cambridge University Press, ISBN:
16 Assumption 4: thin airfoil C L = c L 1+ 2 A with A = b2 A/n mw C D,k = c D + C2 L πea C D,k,i + C D,k,a + C D,k,o cf.: J. Katz and A. Plotkin. Low-Speed Aerodynamics. Cambridge Aerospace Series. Cambridge University Press, ISBN:
17 Assumption 4: thin airfoil C L = c L 1+ 2 A with A = b2 A/n mw C D,k = c D + C2 L πea C D,k,i + C D,k,a + C D,k,o Assumption 5: no interaction between wings and rotors cf.: J. Katz and A. Plotkin. Low-Speed Aerodynamics. Cambridge Aerospace Series. Cambridge University Press, ISBN:
18 Kinematics Kite Aerodynamics Tether 10
19 Assumption 6: wind contribution on airspeed negligible along tether length After conversions: C D,te = 1 4 d te L te A c D,te cf. e.g.: B. Houska, M. Diehl, Optimal control for power generating kites, in: Proceedings of the 9th European Control Conference, Kos, Greece, 2007, pp
20 12
21 Mechanical strength: F te,max A te,core Electrical resistance: R te,wire L te A te,wire R te = R te,wire n te,c,+ + R te,wire n te,c, Dielectric strength: Total diameter, mass: Feasibility condition: E te,ins = f(u te,n,r wire,w ins ) [straight-forward summation] [no overlapping electrical cables] 13
22 Kinematics Rotors Kite Aerodynamics Tether 14
23 Aerodynamic power: P a = 1 2 ρav3 ac D,rot 15
24 Aerodynamic power: P a = 1 2 ρav3 ac D,rot Assumption 7: actuator disk Single rotor: F rot,s =2ρA rot,s v 2 aa(1 a) P rot,s =2ρA rot,s v 3 aa(1 a) 2 15
25 Aerodynamic power: P a = 1 2 ρav3 ac D,rot Assumption 7: actuator disk Single rotor: F rot,s =2ρA rot,s v 2 aa(1 a) P rot,s =2ρA rot,s v 3 aa(1 a) 2 After conversions: C D,rot =4 n rota rot,s A a(1 a) and η a,+ =1 a r rot 15
26 Kinematics Rotors Kite Aerodynamics Power Conversions Tether 16
27 17
28 η a,+ =1 a 17
29 η a,+ =1 a via P te-loss = R te I 2 te 17
30 η a,+ =1 a via P te-loss = R te I 2 te Assumption 8: constant efficiency factors for others 17
31 Kinematics Rotors Atmosphere Kite Aerodynamics Power Conversions Tether 18
32 Assumption 9: logarithmic wind shear v w = v w,href ln h z 0 ln href z 0 with h = h to + L te sin(ϑ) Assumption 10: Rayleigh distribution p(v w,href )= v w,h ref ṽ 2 w,h ref exp v2 w,h ref 2ṽ 2 w,h ref 19
33 Kinematics Rotors Atmosphere Kite Aerodynamics Power Conversions Economics Tether 20
34 Assumption 11: launch & landing energy consumption negligible 21
35 Assumption 11: launch & landing energy consumption negligible Year energy yield: E el,yr [Wh/yr] = 8, 760 h 1yr 0 p(v w,href )P el,+ (v w,href )dv w,href 21
36 Assumption 11: launch & landing energy consumption negligible Year energy yield: E el,yr [Wh/yr] = 8, 760 h 1yr 0 p(v w,href )P el,+ (v w,href )dv w,href LCOE: k LCOE = k E el,yr 21
37 Assumption 11: launch & landing energy consumption negligible Year energy yield: E el,yr [Wh/yr] = 8, 760 h 1yr 0 p(v w,href )P el,+ (v w,href )dv w,href LCOE: k LCOE = k E el,yr Yearly costs: k = k inv + k op k inv = K inv I(1 + I) T/yr (1 + I) T/yr 1 k op = I op K inv 21
38 Assumption 11: launch & landing energy consumption negligible Year energy yield: E el,yr [Wh/yr] = 8, 760 h 1yr 0 p(v w,href )P el,+ (v w,href )dv w,href LCOE: k LCOE = k E el,yr Yearly costs: k = k inv + k op k inv = K inv I(1 + I) T/yr (1 + I) T/yr 1 k op = I op K inv Total capital costs: K inv = k dt P el,n-ins + K inv,o&p 21
39 Kinematics Rotors Atmosphere Kite Aerodynamics Power Conversions Economics Tether 22
40 Outline 1. Model Derivation 2. Power Curve Optimization 3. Design Parameter Optimization 4. Parameter Studies 5. Conclusions 23
41 Assumption 12: v w,href [0,v w,href,cut-out] : arg{max u P a} arg{max u P el} 24
42 Assumption 12: v w,href [0,v w,href,cut-out] : arg{max u P a} arg{max u P el} Assumption 13: C 2 L + C2 D,Σ C L 24
43 power wind speed 25
44 power 0= dp a dc D,rot wind speed 25
45 power 0= dp a dc D,rot C D,rot = C D,eq 2 wind speed 25
46 power 0= dp a dc D,rot C D,rot = C D,eq 2 P a v 3 w wind speed 25
47 power 0= dp a dc D,rot C D,rot = C D,eq 2 P a v 3 w wind speed 25
48 power II 0= dp a dc D,rot C D,rot = C D,eq 2 P a v 3 w wind speed 25
49 power F a = F a,min II 0= dp a dc D,rot C D,rot = C D,eq 2 P a v 3 w wind speed 25
50 power F a = F a,min C D,rot v w const. II 0= dp a dc D,rot C D,rot = C D,eq 2 P a v 3 w wind speed 25
51 power F a = F a,min C D,rot v w const. P a v w const. II 0= dp a dc D,rot C D,rot = C D,eq 2 P a v 3 w wind speed 25
52 power F a = F a,min C D,rot v w const. P a v w const. II 0= dp a dc D,rot C D,rot = C D,eq 2 P a v 3 w wind speed 25
53 power I(a) I(b) II F a = F a,min 0= dp a dc D,rot C D,rot v w const. P a v w const. C D,rot = C D,eq 2 P a v 3 w wind speed 25
54 power I(a) I(b) II F a = F a,min 0= dp a dc D,rot C D,rot v w const. P a v w const. C D,rot = C D,eq 2 P a v 3 w Fa = Fa,max wind speed 25
55 power I(a) I(b) II F a = F a,min 0= dp a dc D,rot C D,rot v w const. P a v w const. C D,rot = C D,eq 2 P a v 3 w Fa = Fa,max wind speed 25
56 power I(a) I(b) II III(a) F a = F a,min 0= dp a dc D,rot C D,rot v w const. P a v w const. C D,rot = C D,eq 2 P a v 3 w Fa = Fa,max wind speed 25
57 power I(a) I(b) II III(a) F a = F a,min 0= dp a dc D,rot P a = const. C D,rot v w const. P a v w const. C D,rot = C D,eq 2 P a v 3 w Fa = Fa,max wind speed 25
58 power I(a) I(b) II III(a) F a = F a,min 0= dp a dc D,rot P a = const. C D,rot v w const. P a v w const. C D,rot = C D,eq 2 P a v 3 w Fa = Fa,max wind speed 25
59 power I(a) I(b) II III(a) III(b) F a = F a,min 0= dp a dc D,rot P a = const. C D,rot v w const. P a v w const. C D,rot = C D,eq 2 P a v 3 w Fa = Fa,max wind speed 25
60 power I(a) I(b) II III(a) III(b) F a = F a,min 0= dp a dc D,rot P a = const. IV C D,rot v w const. P a v w const. C D,rot = C D,eq 2 P a v 3 w Fa = Fa,max wind speed 25
61 Outline 1. Model Derivation 2. Power Curve Optimization 3. Design Parameter Optimization 4. Parameter Studies 5. Conclusions 26
62 27
63 Key ideas 27
64 Key ideas serious estimates/better models for investment costs of other parts/profit margin as well as for mass: not possible/too hard 27
65 Key ideas serious estimates/better models for investment costs of other parts/profit margin as well as for mass: not possible/too hard! INSTEAD: compute maximum allowed investment costs and maximum allowed mass as result, which are requirements for detailed design 27
66 Key ideas serious estimates/better models for investment costs of other parts/profit margin as well as for mass: not possible/too hard! INSTEAD: compute maximum allowed investment costs and maximum allowed mass as result, which are requirements for detailed design rearrange equations into sequence of explicit analytical equations 27
67 Key ideas serious estimates/better models for investment costs of other parts/profit margin as well as for mass: not possible/too hard! INSTEAD: compute maximum allowed investment costs and maximum allowed mass as result, which are requirements for detailed design rearrange equations into sequence of explicit analytical equations optimize free design parameters w.r.t. cost function w/ constraints w/ CMA-ES 27
68 Key ideas serious estimates/better models for investment costs of other parts/profit margin as well as for mass: not possible/too hard! INSTEAD: compute maximum allowed investment costs and maximum allowed mass as result, which are requirements for detailed design rearrange equations into sequence of explicit analytical equations optimize free design parameters w.r.t. cost function w/ constraints w/ CMA-ES optimization problem: max y s.t. ˆK inv,o&p A y y y 27
69 Outline 1. Model Derivation 2. Power Curve Optimization 3. Design Parameter Optimization 4. Parameter Studies 5. Conclusions 28
70 29
71 90 kw/m2 29
72 Parameter Value nominal airfoil lift coefficient 4.16 tether length m elevation angle tether voltage maximum allowed investment costs (o&p)/wing area 9.8 kv 56 k$/m2 total maximum allowed investment costs 5.5 Mio. $ energy yield per year tether mass maximum allowed kite mass maximum allowed kite mass/wing area 18.5 Mio. kwh 1.1 t 11.7 t 140 kg/m2 wing loading 1.6 t/m2 30
73 Parameter Value nominal airfoil lift coefficient 4.16 tether length m elevation angle tether voltage maximum allowed investment costs (o&p)/wing area 9.8 kv 56 k$/m2 total maximum allowed investment costs 5.5 Mio. $ energy yield per year tether mass maximum allowed kite mass maximum allowed kite mass/wing area 18.5 Mio. kwh 1.1 t 11.7 t 140 kg/m2 wing loading 1.6 t/m2 30
74 Parameter Value nominal airfoil lift coefficient 4.16 tether length m elevation angle tether voltage maximum allowed investment costs (o&p)/wing area 9.8 kv 56 k$/m2 total maximum allowed investment costs 5.5 Mio. $ energy yield per year tether mass maximum allowed kite mass maximum allowed kite mass/wing area 18.5 Mio. kwh 1.1 t 11.7 t 140 kg/m2 wing loading 1.6 t/m2 30
75 Parameter Value nominal airfoil lift coefficient 4.16 tether length m elevation angle tether voltage maximum allowed investment costs (o&p)/wing area 9.8 kv 56 k$/m2 total maximum allowed investment costs 5.5 Mio. $ energy yield per year tether mass maximum allowed kite mass maximum allowed kite mass/wing area 18.5 Mio. kwh 1.1 t 11.7 t 140 kg/m2 wing loading 1.6 t/m2 30
76 31
77 Summary of key results of further parameter studies: 31
78 Summary of key results of further parameter studies: tether material selection and nominal voltage have almost no effect 31
79 Summary of key results of further parameter studies: tether material selection and nominal voltage have almost no effect high airfoil lift and high wing loading are required for high maximum allowed cost and a high power density 31
80 optimum 32
81 Summary of key results of further parameter studies: tether material selection and nominal voltage have almost no effect high airfoil lift and high wing loading are required for high maximum allowed cost and a high power density 31
82 Summary of key results of further parameter studies: tether material selection and nominal voltage have almost no effect high airfoil lift and high wing loading are required for high maximum allowed cost and a high power density wide Region III(a) enables much lower wing loading and higher maximum allowed cost 31
83 Summary of key results of further parameter studies: tether material selection and nominal voltage have almost no effect high airfoil lift and high wing loading are required for high maximum allowed cost and a high power density wide Region III(a) enables much lower wing loading and higher maximum allowed cost a (low) tower might cover more than its own cost 31
84 Summary of key results of further parameter studies: tether material selection and nominal voltage have almost no effect high airfoil lift and high wing loading are required for high maximum allowed cost and a high power density wide Region III(a) enables much lower wing loading and higher maximum allowed cost a (low) tower might cover more than its own cost for offshore, the maximum allowed cost is more than the double 31
85 Summary of key results of further parameter studies: tether material selection and nominal voltage have almost no effect high airfoil lift and high wing loading are required for high maximum allowed cost and a high power density wide Region III(a) enables much lower wing loading and higher maximum allowed cost a (low) tower might cover more than its own cost for offshore, the maximum allowed cost is more than the double the technology is scalable: the larger the system, the higher the power density and maximum allowed cost 31
86 Summary of key results of further parameter studies: tether material selection and nominal voltage have almost no effect high airfoil lift and high wing loading are required for high maximum allowed cost and a high power density wide Region III(a) enables much lower wing loading and higher maximum allowed cost a (low) tower might cover more than its own cost for offshore, the maximum allowed cost is more than the double the technology is scalable: the larger the system, the higher the power density and maximum allowed cost the model can reproduce measured data by Makani (model verfication, at least in part) 31
87 Source of left (bottom) figure: Damon Vander Lind. Analysis and Flight Test Validation of High Performance Airborne Wind Turbines. In: Airborne Wind Energy. Ed. by Uwe Ahrens, Moritz Diehl, and Roland Schmehl. Berlin, Heidelberg: Springer Berlin Heidelberg, Fig
88 Source of left (bottom) figure: Damon Vander Lind. Analysis and Flight Test Validation of High Performance Airborne Wind Turbines. In: Airborne Wind Energy. Ed. by Uwe Ahrens, Moritz Diehl, and Roland Schmehl. Berlin, Heidelberg: Springer Berlin Heidelberg, Fig
89 Outline 1. Model Derivation 2. Power Curve Optimization 3. Design Parameter Optimization 4. Parameter Studies 5. Conclusions 34
90 35
91 Achievements: 35
92 Achievements: multidisciplinary steady drag power kite model 35
93 Achievements: multidisciplinary steady drag power kite model covers dominant effects of all involved disciplines 35
94 Achievements: multidisciplinary steady drag power kite model covers dominant effects of all involved disciplines explicit, mostly analytical (white-box), based on first principles 35
95 Achievements: multidisciplinary steady drag power kite model covers dominant effects of all involved disciplines explicit, mostly analytical (white-box), based on first principles can reproduce measurements by Makani 35
96 Achievements: multidisciplinary steady drag power kite model covers dominant effects of all involved disciplines explicit, mostly analytical (white-box), based on first principles can reproduce measurements by Makani numerous parameter studies 35
97 Achievements: multidisciplinary steady drag power kite model covers dominant effects of all involved disciplines explicit, mostly analytical (white-box), based on first principles can reproduce measurements by Makani numerous parameter studies Outlook: 35
98 Achievements: multidisciplinary steady drag power kite model covers dominant effects of all involved disciplines explicit, mostly analytical (white-box), based on first principles can reproduce measurements by Makani numerous parameter studies Outlook: my dissertation/our papers: all details and additional enhancements 35
99 Achievements: multidisciplinary steady drag power kite model covers dominant effects of all involved disciplines explicit, mostly analytical (white-box), based on first principles can reproduce measurements by Makani numerous parameter studies Outlook: my dissertation/our papers: all details and additional enhancements airfoil optimizations 35
100 Achievements: multidisciplinary steady drag power kite model covers dominant effects of all involved disciplines explicit, mostly analytical (white-box), based on first principles can reproduce measurements by Makani numerous parameter studies Outlook: my dissertation/our papers: all details and additional enhancements airfoil optimizations verifications: wind tunnel, higher fidelity models, tiny-scale (1 kw) kite on the way, small-scale (20 kw) kite planned 35
101 36
102 37
103 38
104 Institute for Electrical Drive Systems and Power Electronics, Department of Electrical Engineering and Information Technology, Technische Universität München Power Curve and Design Optimization of Drag Power Kites Florian Bauer, R. Kennel, C. Hackl, F. Campagnolo, M. Patt, R. Schmehl October 5th, 2017, Airborne Wind Energy Conference 2017, Freiburg, Germany 39
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