| ∂ϕℓ∂t+∇(∅ℓ→V)−∇(Γℓ→V∅ℓ)=Rℓ(16) | |||
| l | ∅ℓ | Γℓ | |
| 1 | U | vt | −1ρ∂ρ∂x+∂∂x(vt∂u∂x)+∂∂y(vt∂v∂x)+∂∂z(vt∂w∂x)+gx |
| 2 | V | vt | −1ρ∂ρ∂y+∂∂x(vt∂u∂y)+∂∂y(vt∂v∂y)+∂∂z(vt∂w∂y)+gy |
| 3 | W | vt | −1ρ∂ρ∂z+∂∂x(vt∂u∂z)+∂∂y(vt∂v∂z)+∂∂z(vt∂w∂z)+gz |
| 4 | 1 | 0 | 0 |
| 5 | K | vt/ | G−ε |
| 6 | ε | vt/ | C1εkG−c2εkε |
Citation: Sri Kurniati, Sudirman Syam, Arifin Sanusi. Numerical investigation and improvement of the aerodynamic performance of a modified elliptical-bladed Savonius-style wind turbine[J]. AIMS Energy, 2024, 12(5): 1025-1026. doi: 10.3934/energy.2024048
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Numerical investigation and improvement of the aerodynamic performance of a modified elliptical-bladed Savonius-style wind turbine. By Sri Kurniati, Sudirman Syam and Arifin Sanusi. AIMS Energy, 2023, Volume 11, Issue 6: 1211–1230. Doi: 10.3934/energy.2023055
The authors would like to make the following corrections to the published paper [1].
On page 1213, we updated the contents of "one symbol statement: ρ" in section 2. The updated contents are as follows:
- ρ is the the density of air,
On page 1215, we updated the contents of "Eq 16" in section 2. The updated contents are as follows:
| ∂ϕϕℓ∂t+∇(∅ℓ→V)−∇(Γℓ→V∅ℓ)=Rℓ | (16) |
On page 1216, we updated the contents of "Table 2" in section 2. The updated contents are as follows:
| ∂ϕℓ∂t+∇(∅ℓ→V)−∇(Γℓ→V∅ℓ)=Rℓ(16) | |||
| l | ∅ℓ | Γℓ | |
| 1 | U | vt | −1ρ∂ρ∂x+∂∂x(vt∂u∂x)+∂∂y(vt∂v∂x)+∂∂z(vt∂w∂x)+gx |
| 2 | V | vt | −1ρ∂ρ∂y+∂∂x(vt∂u∂y)+∂∂y(vt∂v∂y)+∂∂z(vt∂w∂y)+gy |
| 3 | W | vt | −1ρ∂ρ∂z+∂∂x(vt∂u∂z)+∂∂y(vt∂v∂z)+∂∂z(vt∂w∂z)+gz |
| 4 | 1 | 0 | 0 |
| 5 | K | vt/ | G−ε |
| 6 | ε | vt/ | C1εkG−c2εkε |
DownLoad:
CSV
All authors declare no conflicts of interest in this paper.
| [1] |
Kurniati S, Syam S, Sanusi A (2023) Numerical investigation and improvement of the aerodynamic performance of a modified elliptical-bladed Savonius-style wind turbine. AIMS Energy 11: 1211–1230. https://doi.org/10.3934/energy.2023055 doi: 10.3934/energy.2023055
|
Sri Kurniati, Sudirman Syam, Arifin Sanusi. Numerical investigation and improvement of the aerodynamic performance of a modified elliptical-bladed Savonius-style wind turbine[J]. AIMS Energy, 2024, 12(5): 1025-1026. doi: 10.3934/energy.2024048
| ∂ϕℓ∂t+∇(∅ℓ→V)−∇(Γℓ→V∅ℓ)=Rℓ(16) | |||
| l | ∅ℓ | Γℓ | |
| 1 | U | vt | −1ρ∂ρ∂x+∂∂x(vt∂u∂x)+∂∂y(vt∂v∂x)+∂∂z(vt∂w∂x)+gx |
| 2 | V | vt | −1ρ∂ρ∂y+∂∂x(vt∂u∂y)+∂∂y(vt∂v∂y)+∂∂z(vt∂w∂y)+gy |
| 3 | W | vt | −1ρ∂ρ∂z+∂∂x(vt∂u∂z)+∂∂y(vt∂v∂z)+∂∂z(vt∂w∂z)+gz |
| 4 | 1 | 0 | 0 |
| 5 | K | vt/ | G−ε |
| 6 | ε | vt/ | C1εkG−c2εkε |
DownLoad:
CSV
