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**Research articles**
18 Jun 2018

**Research articles** | 18 Jun 2018

Towards practical dynamic induction control of wind farms

- Department of Mechanical Engineering, KU Leuven, Celestijnenlaan 300A, 3001 Leuven, Belgium

- Department of Mechanical Engineering, KU Leuven, Celestijnenlaan 300A, 3001 Leuven, Belgium

Abstract

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Wake interactions between wind turbines in wind farms lead to reduced energy extraction in downstream rows. In recent work, optimization and large-eddy simulation were combined with the optimal dynamic induction control of wind farms to study the mitigation of these effects, showing potential power gains of up to 20 % (Munters and Meyers, 2017, Phil. Trans. R. Soc. A, 375, 20160100, https://doi.org/10.1098/rsta.2016.010). However, the computational cost associated with these optimal control simulations impedes the practical implementation of this approach. Furthermore, the resulting control signals optimally react to the specific instantaneous turbulent flow realizations in the simulations so that they cannot be simply used in general. The current work focuses on the detailed analysis of the optimization results of Munters and Meyers, with the aim to identify simplified control strategies that mimic the optimal control results and can be used in practice. The analysis shows that wind-farm controls are optimized in a parabolic manner with little upstream propagation of information. Moreover, turbines can be classified into first-row, intermediate-row, and last-row turbines based on their optimal control dynamics. At the moment, the control mechanisms for intermediate-row turbines remain unclear, but for first-row turbines we find that the optimal controls increase wake mixing through the periodic shedding of vortex rings. This behavior can be mimicked with a simple sinusoidal thrust control strategy for first-row turbines, resulting in robust power gains for turbines in the entrance region of the farm.

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Munters, W. and Meyers, J.: Towards practical dynamic induction control of wind farms: analysis of optimally controlled wind-farm boundary layers and sinusoidal induction control of first-row turbines, Wind Energ. Sci., 3, 409-425, https://doi.org/10.5194/wes-3-409-2018, 2018.

1 Introduction

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Wake interactions between turbines within a wind farm cause reduced power extraction and increased turbine loading in downstream rows. The current control paradigm in such farms optimizes performance at the wind turbine level and does not account for these interactions, resulting in sub-optimal wind-farm efficiency. In contrast, control strategies at the farm level allow the wake interaction to be influenced and promise to improve overall wind-farm performance by improving wind conditions for downstream turbines. This can be achieved by redirecting propagating wakes (yaw control; see, e.g., Campagnolo et al., 2016; Fleming et al., 2014; Gebraad et al., 2016) or by affecting the induced wake velocity deficits (axial induction control; see, e.g., Annoni et al., 2016; Bartl and Sætran, 2016; Nilsson et al., 2015). A more exhaustive survey of wind-farm control in a broader context can be found in Knudsen et al. (2015) and Boersma et al. (2017).

In contrast to the studies cited above that all focus on the static set point optimization of wind farms, Goit and Meyers (2015) introduced a dynamic induction control approach based on large-eddy simulations (LES) and adjoint gradient optimization. In this study, individual turbines were used as dynamic flow actuators that influence the wind-farm boundary layer flow in such a way as to optimize aggregate wind-farm power extraction. The methodology was applied to the asymptotic case of a fully developed “infinite” aligned wind farm, and power gains of about 16 % were quantified. Later, this approach was also used in induction control studies of wind farms with entrance effects in Goit et al. (2016) and more recently in Munters and Meyers (2017), in which similar gains of the order of 15–20 % were achieved. It is important to note that the computational cost of this LES-based dynamic induction control methodology is orders of magnitude too high for direct implementation as a practical control strategy. However, the methodology allows us to assess the theoretical potential for wind-farm control, and increased understanding of the flow physics can lead to simplified control strategies that can be applied in practice.

Recently, the methodology of Goit and Meyers (2015) was generalized to include dynamic yaw control in Munters and Meyers (2018). In this study, induction control and yaw control were compared for a relatively small aligned wind farm, and yaw control was found to yield higher power gains for this setup. Furthermore, the high potential of combined induction and yaw control was quantified, and analysis of the yaw control signals allowed for the identification of practical simplified dynamic yaw control strategies. The search for similar practical control strategies for induction control has remained unsuccessful to date.

The current paper presents efforts on understanding optimal control dynamics observed in the optimal induction control simulations by Munters and Meyers (2017) (further denoted as MM17). The outline of the paper is as follows: first, Sect. 2 discusses the numerical setup and optimal control simulations of MM17 that will be further analyzed in the current paper. Section 3 presents an analysis of the control and thrust force dynamics and performs some numerical experiments to elucidate the characteristics of the optimal controls. It will be shown that the coherent behavior of turbines situated in the first row of the wind farm stands out from their downstream counterparts. Thereafter, Sect. 4 identifies the shedding of vortex rings from the first row based on a flow visualization. Further, a simple sinusoidal thrust control approach is presented that successfully mimics this process with a robust increase in power extraction in the second row. Next, Sect. 5 shortly discusses the behavior of the intermediate rows, i.e., turbines that have both upstream and downstream neighbors, for which similar simple control strategies remain elusive thus far. In conclusion, Sect. 6 summarizes the main findings of this paper.

2 Description of optimal control simulations in MM17

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The current section describes the optimal control simulations performed by MM17, the results of which are further analyzed in the current paper. First, the methodology is introduced. Then, the numerical setup is detailed. Afterwards, the optimization results on power extraction and time-averaged flow field features are discussed.

A schematic overview of the wind-farm control methodology is shown in
Fig. 1. Figure 1a
illustrates the control block diagram: an iterative optimization loop updates
the wind-farm control vector ** φ**(

Within each optimization window, the total wind-farm power is optimized by solving the following optimization problem constrained by partial differential equations.

$$\begin{array}{ll}\text{(1)}& {\displaystyle}& {\scriptscriptstyle \begin{array}{c}\mathrm{minimize}\\ \mathit{\phi},\mathit{q}\end{array}}\phantom{\rule{1em}{0ex}}\mathcal{J}(\mathit{\phi},\mathit{q})=-\underset{\mathrm{0}}{\overset{T}{\int}}\sum _{i=\mathrm{1}}^{{N}_{t}}{P}_{i}\phantom{\rule{0.25em}{0ex}}\mathrm{d}t{\displaystyle}& {\displaystyle}\mathrm{s}.\mathrm{t}.\phantom{\rule{1em}{0ex}}{\displaystyle \frac{\partial \stackrel{\mathrm{\u0303}}{\mathit{u}}}{\partial t}}+\left(\stackrel{\mathrm{\u0303}}{\mathit{u}}\cdot \mathrm{\nabla}\right)\phantom{\rule{0.25em}{0ex}}\stackrel{\mathrm{\u0303}}{\mathit{u}}=-\mathrm{\nabla}\left(\stackrel{\mathrm{\u0303}}{p}+{\stackrel{\mathrm{\u0303}}{p}}_{\mathrm{\infty}}\right)/\mathit{\rho}-\mathrm{\nabla}\cdot {\mathit{\tau}}_{\mathrm{sgs}}\\ \text{(2)}& {\displaystyle}& {\displaystyle}\phantom{\rule{1em}{0ex}}\phantom{\rule{1em}{0ex}}+\sum _{i=\mathrm{1}}^{{N}_{t}}{\mathit{f}}_{i}\phantom{\rule{0.25em}{0ex}}\mathrm{in}\phantom{\rule{0.25em}{0ex}}\mathrm{\Omega}\times (\mathrm{0},T),\text{(3)}& {\displaystyle}& {\displaystyle}\phantom{\rule{1em}{0ex}}\phantom{\rule{1em}{0ex}}\mathrm{\nabla}\cdot \stackrel{\mathrm{\u0303}}{\mathit{u}}=\mathrm{0}\phantom{\rule{0.25em}{0ex}}\mathrm{in}\phantom{\rule{0.25em}{0ex}}\mathrm{\Omega}\times (\mathrm{0},T),\text{(4)}& {\displaystyle}& {\displaystyle}\phantom{\rule{1em}{0ex}}\phantom{\rule{1em}{0ex}}\mathit{\tau}{\displaystyle \frac{\mathrm{d}{\widehat{C}}_{T,i}^{\prime}}{\mathrm{d}t}}={C}_{T,i}^{\prime}-{\widehat{C}}_{T,i}^{\prime}i=\mathrm{1}\mathrm{\dots}{N}_{t}\phantom{\rule{0.25em}{0ex}}\mathrm{in}\phantom{\rule{0.25em}{0ex}}(\mathrm{0},T),\text{(5)}& {\displaystyle}& {\displaystyle}\phantom{\rule{1em}{0ex}}\phantom{\rule{1em}{0ex}}\mathrm{0}\le \phantom{\rule{0.25em}{0ex}}{C}_{T,i}^{\prime}\le {C}_{T,\mathrm{max}}^{\prime}i=\mathrm{1}\mathrm{\dots}{N}_{t}\phantom{\rule{0.25em}{0ex}}\mathrm{in}\phantom{\rule{0.25em}{0ex}}(\mathrm{0},T),\end{array}$$

The cost functional that is optimized in Eq. (1) is the total
wind-farm energy extraction over time horizon *T*. The control variables are
the time-dependent thrust coefficient set points ${C}_{T,i}^{\prime}$ of every turbine
*i* (=1…*N*_{t}), i.e., $\mathit{\phi}=\left[{C}_{T,\mathrm{1}}^{\prime}\right(t),\mathrm{\dots},{C}_{T,{N}_{t}}^{\prime}(t\left)\right]$, and the state variables are denoted as
$\mathit{q}=\left[\stackrel{\mathrm{\u0303}}{\mathit{u}}\right(\mathit{x},t);\phantom{\rule{0.25em}{0ex}}\stackrel{\mathrm{\u0303}}{p}(\mathit{x},t);\phantom{\rule{0.25em}{0ex}}{\widehat{C}}_{T,\mathrm{1}}^{\prime}(t),\mathrm{\dots},{\widehat{C}}_{T,{N}_{t}}^{\prime}(t\left)\right]$, with $\stackrel{\mathrm{\u0303}}{\mathit{u}}$ the filtered
velocity, $\stackrel{\mathrm{\u0303}}{p}$ the filtered pressure, and ${\widehat{C}}_{T,i}^{\prime}$ the
(time-filtered) thrust coefficient for turbine *i* (see below).

The filtered Navier–Stokes momentum and continuity state equations in
Eqs. (2)–(3) are
solved using an in-house LES solver (see, e.g., Calaf et al., 2010; Goit et al., 2016; Meyers and Meneveau, 2010 for a detailed discussion of the solver).
The time-filtering state equation in Eq. (4) applies
a one-sided exponential time filter to the thrust coefficient set points
${C}_{T,i}^{\prime}$ with a characteristic wind turbine response timescale *τ*
(Munters and Meyers, 2016). Finally, the box constraints in
Eq. (5) limit the variations in the turbine thrust
coefficients to technically feasible values.

The forces exerted by turbine *i* on the boundary layer flow are parameterized
using a standard nonrotating actuator disk model as ${\mathit{f}}_{i}(\mathit{x},t)=-(\mathrm{1}/\mathrm{2}){\widehat{C}}_{T,i}^{\prime}\left(t\right){V}_{i}\left(t{)}^{\mathrm{2}}{\mathcal{R}}_{i}\right(\mathit{x}){\mathit{e}}_{\u27c2,i}$, where
ℛ_{i} is a smoothed representation of the geometric footprint of
the turbine on the LES grid and ${\mathit{e}}_{\u27c2,i}$ is the
rotor-perpendicular vector. Further, the disk-averaged velocity is defined as
${V}_{i}=(\mathrm{1}/{A}_{i}){\int}_{\mathrm{\Omega}}{\mathcal{R}}_{i}\left(\mathit{x}\right)\stackrel{\mathrm{\u0303}}{\mathit{u}}\cdot {\mathit{e}}_{\u27c2,i}\phantom{\rule{0.25em}{0ex}}\mathrm{d}\mathit{x}$, with *A*_{i} the rotor disk area. Mechanical power
captured by the wind turbine is calculated as ${P}_{i}=(\mathrm{1}/\mathrm{2}){C}_{P,i}^{\prime}\left(t\right){V}_{i}(t{)}^{\mathrm{3}}{A}_{i}$, with ${C}_{P,i}^{\prime}=\mathrm{0.9}{C}_{T,i}^{\prime}$, resulting from a fit of LES
results to momentum theory, eliminating the overprediction of wind turbine
power on typical wind-farm LES grid resolutions (Munters and Meyers, 2017).

The wind farm considered in MM17 has an aligned pattern of 12 rows by
6 columns. The wind turbines have a hub height *z*_{h}=100 m with a rotor
diameter *D*=100 m and are spaced apart by 6*D* in both the axial and
transversal directions. The flow is simulated on a domain of $\mathrm{10}\times \mathrm{3.6}\times \mathrm{1}$ km^{3} discretized on a simulation grid of $\mathrm{384}\times \mathrm{192}\times \mathrm{144}$ grid points. A snapshot of the streamwise velocity field is shown in
Fig. 2. The wind farm was controlled over a total of
*N*_{A}=15 time windows with a prediction horizon *T*=240 s
(i.e.,
the time it takes for the flow to pass four rows of turbines) and a flow
advancement time of ${T}_{\mathrm{A}}=T/\mathrm{2}=\mathrm{120}$ s, resulting in a total
control time ${T}_{\mathrm{tot}}={N}_{\mathrm{A}}{T}_{\mathrm{A}}=\mathrm{30}$ min.

A conventionally (greedily) controlled wind farm with steady ${C}_{T}^{\prime}=\mathrm{2}$ was
defined as a reference case. Note that this would correspond to a farm with
ideal turbines for which generator torque is being controlled dynamically to
track the maximum power point at the Betz limit perfectly. In a real turbine
controller this may, e.g., be achieved with the extremum-seeking control
proposed by Ciri et al. (2017). Several different optimal control cases
were defined based on the wind turbine response time *τ*=0, 5, or 30 s
(instantaneous, fast, or slow response; see Eq. 4)
and the maximal thrust coefficient ${C}_{T,\mathrm{max}}^{\prime}=\mathrm{2}$ or 3, with
thrust forces that can respectively only be reduced (underinductive) or
increased (overinductive) compared to the Betz optimum at ${C}_{T}^{\prime}=\mathrm{2}$ (see
Eq. 5). Cases are denoted as $C<X>t<Y>$, where *X*
and *Y* represent ${C}_{T,\mathrm{max}}^{\prime}$ and *τ*, respectively, e.g., C3t30
for the case with ${C}_{T,\mathrm{max}}^{\prime}=\mathrm{3}$ and *τ*=30 s. The choice of
(and sensitivity to) setup parameters is further elaborated in MM17.

Figure 3 illustrates the energy extraction of the optimally controlled wind-farm cases normalized by the greedy reference control case. Figure 3a shows that the adjoint LES-based control approaches achieve energy gains ranging from a minor 2 % in the most restrictive C2t30 case to over 20 % in the C3t0 case. From Fig. 3b it can be seen that, for all cases except C3t30, power is curtailed in the first row to a limited degree, whereas the downstream rows compensate for this loss by extracting significantly more energy. Furthermore, not taking into account the first row, the last row achieves the highest energy extraction in every case, as it can act greedily without compromising power extraction in downstream neighbors.

In the remainder of this section, time-averaged wind-farm flow properties will be investigated. Here and throughout the remainder of this paper, we focus on case C3t5, as it produces similar energy gains as the highest-yield case C3t0 (see Fig. 3a), but achieves this with smoother thrust coefficient signals. In the following discussion, the time-averaging operation is denoted by an overline, and flow field variables are decomposed into mean and fluctuating components as $\stackrel{\mathrm{\u0303}}{u}=\stackrel{\mathrm{\u203e}}{\stackrel{\mathrm{\u0303}}{u}}+{\stackrel{\mathrm{\u0303}}{u}}^{\prime}\equiv \stackrel{\mathrm{\u0303}}{U}+{\stackrel{\mathrm{\u0303}}{u}}^{\prime}$. Figure 4 illustrates the time-averaged flow field quantities of the reference case (left panels, a1–g1) and the differences between the optimized C3t5 case and the reference case (right panels, a2–g2). Simulation results are averaged over the different columns and are shown as either top views at hub height (Fig. 4b, f, g) or side views through a turbine column (Fig. 4a, c, d, e).

Figure 4a and b illustrate side views and top views of the axial velocity throughout the wind farm. It can be seen that downstream turbines in the controlled case experience consistently higher incoming velocities, which explains the increased energy extraction discussed above. Furthermore, a larger drop in streamwise velocity over the turbine disk can be observed, most notably in the first-row turbines, indicating deeper wakes with enhanced recovery before hitting the next row of turbines. Furthermore, it can be observed that the axial velocity in the flow above and beside the wind turbine column is reduced, indicating that the mean flow kinetic energy is depleted in these regions to the benefit of the flow passing through the wind turbines.

Figure 4c shows side views of turbulence kinetic
energy *k*. The figure shows an increase in turbulence throughout the entire
wind farm, spreading to the internal boundary layer above the turbines. Note
specifically the sharp increase in turbulence in the core wake region behind
the first-row turbine, for which an enhanced recovery was found as discussed
above. The turbulence intensity $TI\equiv (\mathrm{2}k/\mathrm{3}{)}^{\mathrm{1}/\mathrm{2}}/{U}_{\mathrm{\infty}}$ at hub
height (not shown in the figure) is 10 % at the inlet for both the
reference case and the controlled case. The combination of reduced near-wake
mean velocities and increased velocity fluctuations in the controlled case
increase local *T**I* in the turbine wakes (ranging from ≈2 % points in the wakes of the middle rows to ≈12 % points in
the first and last rows). This increase in turbulence intensity dissipates to
below a 1 % point difference at 10*D* downstream of the last row.

Figure 4d and e show side views through the rotor centerline of top-down turbulence and mean flow transport of axial momentum, i.e., $-\stackrel{\mathrm{\u203e}}{{\stackrel{\mathrm{\u0303}}{u}}_{x}^{\prime}{\stackrel{\mathrm{\u0303}}{u}}_{z}^{\prime}}$ and $-{\stackrel{\mathrm{\u0303}}{U}}_{x}{\stackrel{\mathrm{\u0303}}{U}}_{z}$, respectively. It can be seen that, although mean flow vertical transport is virtually unaffected, the turbulence top-down transport of axial momentum is increased significantly in the upper part of the wakes, indicating increased turbulent mixing with the internal boundary layer above the wind-farm canopy. The effect is somewhat more pronounced in the wake behind the first row of turbines, for which a slight increase in the upwards transport of momentum can also be observed in the lower part of the wake.

Figure 4f and g show plan views at hub height of
the transversal turbulence and mean flow transport of axial momentum, i.e.,
$\stackrel{\mathrm{\u203e}}{{\stackrel{\mathrm{\u0303}}{u}}_{x}^{\prime}{\stackrel{\mathrm{\u0303}}{u}}_{y}^{\prime}}$ and ${\stackrel{\mathrm{\u0303}}{U}}_{x}{\stackrel{\mathrm{\u0303}}{U}}_{y}$,
respectively. The sign convention is such that positive values correspond to
transport in the positive *y* direction in the figure. A slight increase in
turbulent transversal transport towards the wake centerline can be observed
behind every row. The mean flow transversal momentum transport into the wake
region is increased significantly behind the first two turbine rows.
Downstream of these rows, the difference between these cases and the
reference case is far less coherent. The latter can be explained by the fact
that ${\stackrel{\mathrm{\u0303}}{U}}_{x}$ in the inter-column channels starts to deviate
significantly from the reference case as shown in
Fig. 4b.

The analysis of flow features given above indicates that the optimal controls in case C3t5 influence the wind-farm flow field in such a way as to provide better flow conditions for downstream turbines. Increased axial velocities are observed for all downstream turbines, and enhanced momentum transport towards the turbine region is achieved. Furthermore, many of the observed flow features are most salient for the first-row turbines. In the following section, the optimized thrust coefficients themselves will be investigated. It will be shown that, also from a controls perspective, first-row turbines stand out from their downstream counterparts.

3 Thrust coefficient analysis and numerical experiments

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The current section focuses on the optimal thrust coefficients generated by the optimal control simulations in MM17 and performs numerical experiments to uncover some of the characteristics of these control signals. Note that the conclusions drawn within this section should be interpreted as observations of the current C3t5 optimal control cases given specific wind-farm layout and flow conditions, and hence cannot just be generalized for any wind-farm control in general.

First, the thrust coefficient signals themselves are analyzed in Sect. 3.1. Second, the optimized thrust coefficients are applied only to subsets of turbine rows in Sect. 3.2. In this way, the interdependency of optimized thrust coefficients in different rows can be evaluated. Third, additional optimal control simulations, in which only one single active row is optimized, are discussed in Sect. 3.3. These optimizations provide an indication of how increased power potential is distributed among the rows and allows us to compare the resulting single-row optimized thrust coefficients with the fully cooperative coefficients from case MM17. Fourth, Sect. 3.4 evaluates the dependency of optimized thrust coefficients on the actual turbulent flow realization. Finally, Sect. 3.5 discusses the main conclusions from the abovementioned sections and summarizes the lessons learned.

Figure 5 illustrates the time evolution of some of the thrust coefficients ${\widehat{C}}_{T}^{\prime}$ in the C3t5 case. The figure shows that, for all rows but the last one (i.e., R12), ${\widehat{C}}_{T}^{\prime}$ varies significantly in time and that the amplitudes and frequencies of these variations are somewhat higher in the upstream rows of the farm. In contrast, row 12 features only minor unsteadiness at lower frequencies and has an increased mean value of ${\widehat{C}}_{T}^{\prime}$. This relatively steady behavior of the last row can be explained by the fact that there are no further downstream turbines that can benefit from row 12 actively influencing local flow conditions; hence, the row optimizes its own power only. The increase in mean ${\widehat{C}}_{T}^{\prime}$ in row 12 can be explained based on Fig. 6, which shows the power extraction as a function of steady ${\widehat{C}}_{T}^{\prime}$ for unwaked turbines, subject to identical turbulent inlet as in case C3t5. Although momentum theory predicts maximal power extraction for steady uniform inflow at ${\widehat{C}}_{T}^{\prime}=\mathrm{2}$, the actual optimal steady value for the ADM at the current spatial resolution lies somewhat higher at ${\widehat{C}}_{T}^{\prime}\approx \mathrm{2.4}$, for which power extraction is about 1.4 % higher than at ${\widehat{C}}_{T}^{\prime}=\mathrm{2}$. This behavior is related to the overprediction in ADM power due to the diffuse turbine representation on typical simulation grids: the mass flow through the rotor disk at ${\widehat{C}}_{T}^{\prime}>\mathrm{2}$ is slightly too high compared to momentum theory, resulting in a shift of optimal ${\widehat{C}}_{T}^{\prime}$ towards somewhat higher values. Although the linear fit ${C}_{P}^{\prime}=a{\widehat{C}}_{T}^{\prime}$ introduced in Munters and Meyers (2017), Appendix A, eliminates the error in maximal power extraction, it does not correct the value of the optimal ${\widehat{C}}_{T}^{\prime}$ (note that this could be achieved through a more complex relation between ${C}_{P}^{\prime}$ and ${\widehat{C}}_{T}^{\prime}$). Returning to the more complex thrust coefficients in the other rows, it is worth noting that based on the current dataset no statistically significant correlations between the thrust coefficients of different turbines could be found. Furthermore, attempts towards linking thrust coefficient dynamics to upstream flow measurements (e.g., velocities, shear or kinetic energy) through linear regression models and random forest regressors have been unsuccessful to date.

Figure 7a and b show row-averaged power spectral
densities of the thrust forces and thrust coefficients, respectively. The
figure shows that the variances of both the thrust coefficients and their
resulting forces are highest in row 1. Further downstream, rows 2 to 11 have
very similar spectral behavior, and row 12 shows significantly lower
variability. The high-frequency slopes of around −5 observed both for *f*_{T}
and ${\widehat{C}}_{T}^{\prime}$ indicate that force variability on short timescales is
caused mainly by thrust coefficient variations, whereas the slower thrust
force dynamics tend more to a $-\mathrm{5}/\mathrm{3}$ slope, suggesting that these are
governed by the unsteadiness in the turbulence instead. Note that, even
though the spectra for all rows except row 12 collapse at frequencies below
0.05 Hz, the first-row spectrum shows a small peak at *f*≈0.02 … 0.03 Hz ($fD/{U}_{\mathrm{\infty}}\approx \mathrm{0.2}\phantom{\rule{0.125em}{0ex}}\mathrm{\dots}\phantom{\rule{0.125em}{0ex}}\mathrm{0.3}$) as indicated by
the purple arrow. It will be shown later in this paper that variations in the
thrust coefficient around this frequency are directly related to increased
power extraction.

In order to further study how the optimal controls increase overall wind-farm power, Fig. 8 shows power extraction resulting from applying a subset of the optimal controls to specific turbine rows only. Figure 8a depicts simulation results for which the optimized controls are applied only to one specific row, with the thrust coefficient in all other rows kept at the reference value of ${\widehat{C}}_{T}^{\prime}=\mathrm{2}$. From the figure it can be seen that only for the controls of the first row (R1) does this result in a significant power increase in rows 2 and 3. This indicates that the optimal controls, as generated by the optimization at the wind-farm level, react to the precise flow conditions caused by upstream control actions and can hence only be applied independently for the first row, which has no upstream dependence on other controls.

Figure 8b shows results from simulations in which the
controls are applied for all rows up to a certain row; i.e., R1–R3
indicates the application of optimized controls generated by case C3t5 to
rows 1, 2, and 3. An interesting observation from this figure is that for
any row *i* except the last one, the power potential as observed in case C3t5
is almost fully recovered by only applying the optimal controls up to row
*i*−1. This suggests that self-optimization is very limited: the optimal
controls for a given turbine are designed to create favorable flow conditions
in the downstream rows instead of increasing local power. Furthermore,
although the discussion in the previous paragraph has shown that downstream
controls are optimized with the upstream actions in mind, the converse is not
true: upstream control actions do not require a specific downstream response
in order to increase power in that downstream row.

The previous section has shown that, based on the full-farm optimization case, the first-row controls can be applied independently from other turbine controls, whereas this does not work for the downstream rows. To further quantify the potential for increasing wind-farm power in each row of turbines, the current section considers a set of additional optimal control cases in which only a single active row is optimized, with all other rows remaining passive. Furthermore, by comparing the optimized controls of these cases with the full-farm optimization case C3t5, the degree of cooperation between turbines can be assessed. Note that the current single-row optimal control is not equivalent to greedy control: the optimizer still aims to increase aggregate farm power by taking into account wake interactions with downstream turbines. Furthermore, in contrast to the single-row control simulations from the previous section (i.e., in Fig. 8a), the current optimizations will yield controls that are explicitly designed to increase power given that all other rows are passive. To limit computational costs, the additional optimizations are only performed for a single time window.

Figure 9 shows the relative increase in wind-farm
power extraction for each of the 12 individually optimized control cases.
The optimization is run until the continuous adjoint gradient accuracy
prevents further progress in the optimization. Upon interpreting the actual
values from the figure, it is important to note that the reported power gain
covers the full optimization horizon *T* and is hence affected by
finite-horizon effects. Furthermore, the first window of an optimal control
simulation as considered here contains an initial dead zone corresponding
to the wake advection lag before upstream turbines start influencing their
downstream neighbors. This tends to reduce gains compared to later time
windows. Nevertheless, the relative order of the different cases still
provides information that can be generalized to full optimal control studies
with multiple windows and longer time horizons.

The figure shows that the first row (R1) holds by far the most promise for optimizing wind-farm power. This is not surprising as R1 produces the most power of all rows and typically leaves the deepest wakes, causing second-row turbines to perform poorly in aligned wind-farm layouts (see, e.g., Nilsson et al., 2015; Porté-Agel et al., 2013; and Stevens et al., 2016). At the other end of the spectrum, the last row (R12) is the least useful. The intermediate rows (R2–R11) lie closer together, with the general trend being that the potential is somewhat decreased with downstream distance into the wind farm, although this decrease is not monotonous.

Figure 10 illustrates the row-wise relative power
increase matrix for each of the single-row optimization cases. The figure
indicates that, for each of the optimization cases, the largest power
increase is observed in the first row downstream of the active turbine (i.e.,
*R*_{i+1}) and that the influence on row *R*_{i+3} is limited. This is
explained by the fact that the finite optimization horizon used in MM17
(i.e.,
*T*=240 s) allows for more interactions with directly neighboring turbines
than with those located further downstream. Furthermore, except for the
optimal control case of the last row (R12), self-optimization is virtually
nonexistent: power gains are achieved by modifying the flow to yield more
favorable conditions for downstream rows.

The observations from previous sections illustrate that, at least to some degree, the optimized thrust coefficients are tuned to local flow conditions. In the current section, the possibility of whether the coefficients contain traits that are independent of flow conditions is investigated. To this end, the optimized thrust coefficients are modified in such a way that correlations between them and specific flow events are eliminated. This is done in two independent test cases.

In the first case, the controls, which were specifically generated for
selected turbines, are reassigned to other turbines by randomly swapping the
control sets of different turbine columns. In doing so, each turbine will
receive controls that were specifically designed for another turbine in the
same row. To avoid erroneous conclusions based on coincidence, the column
swap is performed in two random independent ways. The variability of flow
conditions for different columns can be qualitatively observed in Fig. 2. To
further strengthen the hypothesis of the current experiment, we verified that
the correlation between flow conditions in different columns is small, i.e.,
with an average Pearson correlation coefficient of 0.12 between columns for
the incoming velocity fluctuations 6*D* upstream of the first row.
The row-averaged power for these cases is shown in Fig. 11a.

In the second case, controls remain assigned to their original turbines, but
are shuffled in time by randomly swapping optimal controls generated for
different control windows. In this way, the spectral thrust characteristics
for timescales smaller than the control horizon *T*_{A}=120 s
remain unchanged, whereas the time synchronization of control actions to
specific flow events is eliminated. Similar to the first case, this is done
in two random ways, and the limited correlation between velocity fluctuations
in different time windows was quantified at 0.07.
Figure 11b illustrates the row-averaged power for these
cases.

The figure shows similar behavior for each of the modified control cases: only in the second row (R2) can a consistent (though small) increase in power extraction be observed. This suggests the presence of flow-invariant features in the control signals of the first row. Note, however, that the full power gain in the second row is only partially attained, indicating that the first turbine row also reacts to the specific flow conditions.

The observations and experiments from previous sections have revealed information that increases the understanding of the optimized thrust coefficients and can be used as a starting point towards designing practical wind-farm controllers that do not require computationally expensive LES-based optimal control simulations.

A first conclusion is that wind turbines can be classified into three distinct categories based on their position within the farm: first-row turbines, last-row turbines, and intermediate turbines. The most salient behavior can be found in the first-row turbines (R1). It was shown that these turbines exhibit the largest variability in thrust forces and hold the greatest potential for power optimization. Furthermore, they are not influenced by upstream turbine control action and are the only turbines that retain part of the power gains after eliminating possible correlation between controls and specific flow events. The characteristics of the last-row turbines (R12) also stand out from the rest due to the fact that by definition the last row has no downstream turbines and hence holds no further potential for coordinated control. The remaining intermediate rows (R2–R11) have similar spectral thrust characteristics and potential for power increase, as they are situated between but clearly separated from the first- and last-row turbines. Further, it is worth noting that the behavior and analysis of control actions in these turbines is most complex: not only do they influence downstream turbines, but they in turn are also dependent on the controls of upstream turbines.

A second conclusion is that, whether or not the wind farm is controlled with
the possibility of active response and cooperation between turbines, the
resulting power and thrust characteristics are very similar. It was shown
that self-optimization is very limited and that for any row *i* the full
potential in power increase is virtually attained by applying controls only
for the upstream turbines up to row *i*−1. These observations strongly
suggest that the optimized thrust coefficients are designed in a parabolic
manner, i.e., with a unidirectional propagation of control information from
the first row to the last and very little upstream influence of downstream
turbine actions. With this in mind, the following section of this paper will
focus on the first and most promising link in the control chain: the turbines
situated in the first row of the wind farm.

4 First-row turbine behavior

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The current section further focuses on the analysis of the first-row turbines. First, a qualitative analysis of the instantaneous flow field is performed in Sect. 4.1, resulting in the observation of vortex rings being shed from first-row turbines. Thereafter, this mechanism is mimicked by imposing sinusoidally varying thrust coefficients in these turbines in Sect. 4.2, with the aim of increasing power through similar mechanisms as in the computationally expensive optimal control cases.

Figure 12 shows snapshots of the vorticity and
velocity fields at *t*=300 s for the reference case (left) and the optimal
control case C3t5 (right). Figure 12a and b show
isosurfaces of vorticity magnitude colored by streamwise velocity
${\stackrel{\mathrm{\u0303}}{u}}_{x}$. Figure 12a shows that in the
reference case the first-row turbines shed relatively stable vortex sheets
that demarcate the wake from the free-stream flow. The sheets destabilize and
break up as they are advected downstream, resulting in complex
three-dimensional vortical structures. Furthermore, as also shown in
Fig. 12c, wake mixing is limited, and downstream
turbines experience reduced velocities. In contrast, the optimized case shows
coherent vortex rings being shed from the first-row turbine. As indicated by
the black arrows in Fig. 12b, the locations of the
rings in the controlled case coincide with naturally occurring bulges in the
vortex sheet of the reference case: the controlled turbines further
destabilize the sheet through well-timed temporal variations in its thrust
coefficient. Figure 12c shows that this results in
smaller velocity deficits in the wake region. Note that downstream of the
second turbine the vorticity field becomes much more complex and differences
in the flow fields are less coherent.

The observed shedding of ring vortices seems to occur at specific flow-synchronized times to exploit the natural instabilities in the original vortex sheets. Therefore, the remainder of this paper will attempt to accomplish the same effect through simple sinusoidal thrust variations.

The aim of the current section is to mimic the quasi-periodic shedding of
vortex rings by upstream turbines as observed above through the use of simple
periodic variations in the thrust coefficient. Instead of optimizing a
high-dimensional control signal that can evolve freely in time as in MM17, we
impose a sinusoidal perturbation on the Betz-optimal coefficient
${\widehat{C}}_{T}^{\prime}=\mathrm{2}$, parameterized by its amplitude *A*, and its frequency in
the form of a nondimensional Strouhal number $\mathit{\text{St}}=fD/{U}_{\mathrm{\infty}}$,
with *f* the dimensional frequency, *D* the turbine diameter, and *U*_{∞}
the unperturbed time-averaged upstream velocity:

$$\begin{array}{}\text{(6)}& {\widehat{C}}_{T}^{\prime}\left(t\right)=\mathrm{2}+A\mathrm{sin}\left(\mathrm{2}\mathit{\pi}\mathit{\text{St}}{\displaystyle \frac{t{U}_{\mathrm{\infty}}}{D}}\right).\end{array}$$

Instead of optimizing *A* and *St* using a similar gradient-based
optimization setup as in MM17, we perform a parameter sweep to find optimal
parameter combinations. The reason for this is that we would need a rather
long optimization horizon *T* to find a robust parameter combination that is
independent of specific flow realizations. Unfortunately, the chaotic nature
of turbulent flow fields makes long-time optimization using adjoint LES
practically infeasible to date (see, e.g., Wang et al., 2014). However,
the fact that we have only two parameters renders a parameter sweep
computationally feasible. The sweep is performed for a reduced-size wind-farm
LES, as illustrated in Fig. 13. The farm consists of 4×4 turbines in an aligned layout with *S*=6*D* in both the streamwise and
span-wise directions, geometrically equivalent to the optimally controlled
wind farm in MM17. The simulation is performed on a domain of $\mathrm{4}\times \mathrm{2.4}\times \mathrm{1}$ km^{3} with a simulation grid of $\mathrm{192}\times \mathrm{256}\times \mathrm{144}$
grid points. A wall roughness length ${z}_{\mathrm{0}}={\mathrm{10}}^{-\mathrm{1}}$ m is used. A set of
wind-farm flow simulations is advanced in time by 30 min, during which
the front row is controlled using a sinusoidally varying thrust coefficient
${\widehat{C}}_{T}^{\prime}$, as defined in Eq. (6). Within this set,
the amplitude *A* is varied between 0.5 and 2, with increments of 0.5.
Furthermore, the Strouhal number *St* is varied between 0.05 and
0.6, with increments of 0.05. In total, this leads to 48 LES cases within the
set.

Figure 14 illustrates the power extraction for all
cases considered. Figure 14a illustrates the relative
power gains over the reference case. From the figure it can be seen that
there is a well-defined range of values for *A* and *St* for which
wind-farm power can be increased substantially through upstream sinusoidal
thrust variations, with a maximal power increase of ≈5 % at
$({\mathit{\text{St}}}^{\ast},{A}^{\ast})=(\mathrm{0.25},\mathrm{1.5})$. For instance, a Strouhal
number *St* =0.25 corresponds here to a sine wave period of
≈50 s for a turbine with diameter *D*=100 m and a free-stream
velocity *U*_{∞}=8.5 m s^{−1}. For instance, considering the NREL
5MW blade profiles, the maximum thrust coefficient of 3.5 can be attained by
slightly changing the rotor design, e.g., using a 50 % increase in blade
chord length and an operational tip speed ratio 25 % higher than the
original design value (see Appendix A in Goit and Meyers, 2015).
Furthermore, given such redesign, dynamic reductions from this value could be
realized through blade pitch control, for which actuation rates of the order
of 10^{∘} s^{−1} are possible (see, e.g.,
Jonkman et al., 2009). Figure 14b
illustrates normalized power extraction by row for the reference case, the
best sinusoidal case, and the first four rows of the optimal control case
C3t5 from MM17. The figure shows that the power gain in the sinusoidal cases
originates mostly from the second row and that power in the first row is
decreased by approximately 5 %. In contrast, optimal control case C3t5,
in which all rows are active, also increases power in rows 3 and 4 and
reduces first-row power by only 1 %.

Figure 15 illustrates instantaneous vorticity and axial velocities for a set of wind turbines of the aforementioned reference case (a), the best sinusoidal case with $(\mathit{\text{St}},A)=({\mathit{\text{St}}}^{\ast},{A}^{\ast})=(\mathrm{0.25},\mathrm{1.5})$ (b), and a sinusoidal case that does not lead to increased power extraction with $(\mathit{\text{St}},A)=(\mathrm{0.6},\mathrm{2})$ (c). The figure illustrates the fact that sinusoidal variations in the first-row thrust coefficient indeed cause the periodic shedding of vortex rings. Figure 15b shows that at the optimal frequency this leads to increased wake mixing, providing the second-row turbine with a higher incoming velocity. In contrast, Fig. 15c shows that even though higher-frequency thrust oscillations also result in the periodic shedding of vortex rings, this does not automatically lead to more favorable flow conditions for downstream turbines. Therefore, it can be concluded that the correct timing and spacing of vortex rings is essential for increased wake mixing.

In order to assess whether the same strategy can be used in the downstream turbines as well, Fig. 16 illustrates the results from an identical parameter sweep as discussed above, except that here the second turbine row is controlled using a sinusoidal thrust coefficient. Figure 16a indicates that the sinusoidal actuation of the second row invariably leads to losses in wind-farm power. Figure 16b shows that, for the optimal combination of parameters of $(\mathit{\text{St}},A)=(\mathrm{0.25},\mathrm{1.5})$ as reported for first-row actuation above, the minor power increase in the third row does not compensate for additional losses in the second and fourth row. This shows that the proposed simple control strategy does not work when applied to waked turbines and that more elaborate control strategies are required to harness the gains achieved by the optimal control simulation in the downstream regions of the farm.

It is interesting to note that, even though the current parameter sweep is performed using different initial and inlet conditions than those applied in MM17, the optimal frequency of sinusoidal variations in ${\widehat{C}}_{T}^{\prime}$ at ${\mathit{\text{St}}}^{\ast}=fD/{U}_{\mathrm{\infty}}=\mathrm{0.25}$ corresponds to the location of the peak in the first-row thrust coefficient spectrum of C3t5 in Fig. 7. In the following paragraphs, the robustness of the best parameter pair for first-row thrust variations, i.e., $(\mathit{\text{St}},A)=(\mathrm{0.25},\mathrm{1.5})$, is investigated with the aim of assessing the general applicability of this control strategy. To this end, similar parameter sweeps are performed for cases with varying turbine spacings and turbulence intensities.

Figure 17 shows the power extraction resulting from two
parameter sweeps with streamwise turbine spacings of 5*D* and 7*D*. The results are promising: for the given cases,
*St*^{∗} and *A*^{∗} do not depend on streamwise turbine
spacing. Furthermore, even in the 7*D* spacing case
(Fig. 17c–d), which naturally features lower overall
power losses in downstream rows, power extraction in the second row can be
significantly increased through sinusoidal variations in the first-row thrust
coefficient.

Figure 18 depicts the power extraction results from a
parameter sweep with the same wind-farm layout as in the baseline case, but
with a 10-fold increase in roughness length, i.e., *z*_{0}=1 m. This results
in a turbulence intensity of approximately 16 % compared to 10 % in
the baseline case. Again, the best parameter combination of
$({\mathit{\text{St}}}^{\ast},{A}^{\ast})=(\mathrm{0.25},\mathrm{1.5})$ remains unchanged. Further,
even for this higher turbulence case, in which downstream losses are lower
due to naturally better wake mixing, power is increased in the second row,
leading to a relative gain in wind-farm power of around 2 %.

As evidenced above, periodic sinusoidal variations in first-row thrust coefficients substantially increase power extraction in the second row, resulting in a net gain in total power for the considered 4×4 wind farm. Moreover, different simulation sets indicate that, at least for the range considered here, the best values for the Strouhal number and the amplitude of these variations, i.e., $({\mathit{\text{St}}}^{\ast},{A}^{\ast})=(\mathrm{0.25},\mathrm{1.5})$, are robust with respect to turbine spacing and turbulence intensity.

In the remainder of this section, the sinusoidal variation strategy will be tested in a full-scale wind-farm LES corresponding to the full 12×6 aligned wind farm of MM17. Simulations are performed for a reduced range of amplitudes and Strouhal numbers corresponding to the most favorable region identified in the parameter sweeps above. In order to increase statistical convergence, the time horizon for each simulation is extended to a physical time of 10 h.

Figure 19 shows the power extraction of the full-scale LES. Figure 19a shows the relative power gains over the reference case for the full wind farm. It can be seen that the total power gain or loss is below 0.5 % for each of the sinusoidal control cases. Figure 19b shows the row-wise power extraction for the reference case, the sinusoidal thrust case with $(\mathit{\text{St}},A)=(\mathrm{0.25},\mathrm{1.5})$, and the optimal control case C3t5. It is shown that, although the second row of the sinusoidal thrust case achieves similar power gains as those observed above, from the fifth row onwards power is slightly reduced in the sinusoidal case.

The top panel of Fig. 20 shows cross sections of time-averaged axial velocities ${\stackrel{\mathrm{\u0303}}{U}}_{x}$ at the rotor disk locations for the reference case. Further, the middle and bottom panels illustrate deviations from the reference velocity for the $({\mathit{\text{St}}}^{\ast},{A}^{\ast})$ sinusoidal case and the optimal control case C3t5, respectively. The figure shows that both controlled cases show similar characteristics at the second turbine row, with an increased axial velocity at the rotor disk accompanied by decreased velocities above and below. Downstream, it can be seen that the passive turbines of the sinusoidal case fail to retain increased velocities at the rotor disks, instead resulting in slightly lower disk velocities starting from the fifth row. In contrast, case C3t5, in which all turbines are actively controlled, succeeds in attaining similar cross section characteristics with higher rotor velocities in the downstream as well. Note also that for the fifth row the disk velocity is slightly lower for the sinusoidal control case than for the reference case, consistent with the decreased power extraction observed in Fig. 19. This can be explained by the fact that first-row control actions cause enhanced entrainment of momentum from the internal boundary layer above the turbine canopy that would otherwise be entrained by natural turbulent mixing in passive downstream rows. In consequence, lesser entrainment occurs for downstream rows, resulting in a slight decrease in disk velocities from the fifth row onwards.

As shown throughout the current section, a qualitative analysis of instantaneous flow features in the optimal induction control wind farm from MM17 has led to the identification of a sinusoidal thrust control strategy for first-row turbines, resulting in increased power extraction in the second row. However, important comments should be made. First, sustained sinusoidal thrust variations with a large amplitude could contribute significantly to turbine fatigue loading of the first-row turbines. Furthermore, partial wake alleviation and unsteady passing of the abovementioned vortex rings could also increase fatigue loading in downstream rows. Hence, structural aspects should be taken into account upon evaluating the practical viability of the approach. Second, even though experiments have shown that, for practically relevant tip speed ratios, wind turbines shed vortices in a similar way as disk-like bluff bodies (Medici and Alfredsson, 2006), the current behavior could still be an artifact of the relatively simple ADM used throughout this study. Further verification using higher-fidelity wind turbine models, such as actuator line models, and wind tunnel testing is hence necessary.

5 Intermediate-row turbine behavior

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The current section discusses the intermediate rows. It was shown that, without active participation in these rows, upstream gains are lost in downstream rows, and only full optimal control succeeds in achieving significant gains in downstream rows as well (see Figs. 19, 20). It was already mentioned that the analysis and behavior of turbines within intermediate rows is more complex than in the first row: they aim to influence the flow to the benefit of downstream rows but are also dependent on the actions of upstream rows. The remainder of the current section aims to illustrate the additional difficulty of power increase in downstream rows and speculates on possible future paths for the identification of simplified control strategies as found for the first row.

First, as shown in the top panels of Fig. 20, even in the uncontrolled case the kinetic energy of the flow in the vicinity of the turbine rotor is depleted more and more in the downstream rows. This complicates control strategies for these rows as the opportunity for increased mixing with high-energy flow is decreased. Furthermore, intermediate turbines are subjected to increased turbulence levels and more complex vorticity dynamics, as illustrated in Fig. 12. This could explain why sinusoidal thrust control did not lead to increased power when applied to the second row: whereas the first row produces increased mixing by destabilizing relatively stable vortex sheets into vortex rings, the second row is already continuously immersed in complex vorticity patterns for which this simple approach does not work. However, note that R7 in Fig. 5, for instance, also seems to show quasi-periodic sinusoidal variations in ${\widehat{C}}_{T}^{\prime}$ at a time period of approximately 50 s. This is an indication that, also for intermediate rows, vortex ring shedding could amount to part of the power increase observed in the optimal control simulations, albeit at specific moments in time, synchronized with the local flow conditions.

Second, it is important to note that the vortex ring shedding mechanism constitutes only part of the power increase caused by the first row. Figure 8 illustrates that the first-row optimized thrust coefficient also results in a significant power increase in the third row, which is not observed using the sinusoidal thrust strategy. Furthermore, the analysis of the modified control cases in Fig. 11 proves that the first-row controls are also partially synchronized with the flow. This shows that other mechanisms, dependent on specific flow events for increasing wind-farm power, are at play as well. Even though the application of regression algorithms in an attempt to link turbine actions to low-dimensional flow measurements (e.g., local velocity, shear and kinetic energy) has been unsuccessful thus far, similar analysis based upon more complex flow features (e.g., vorticity structures, high-speed turbulent streaks, or downdrafts) might be more promising. This requires further optimal control simulations over an extended time, as the total control time horizon of 30 min in the current dataset is insufficient for robust statistics in this kind of analysis. This is an important remaining challenge to be addressed in future research.

6 Conclusions

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The current paper provided an analysis of the thrust coefficient control characteristics for the C3t5 optimal control case featured in Munters and Meyers (2017).

Analysis of the thrust coefficients and numerical experiments have shown a clear distinction between first-row turbines, last-row turbines, and intermediate turbines. Furthermore, observations strongly suggest that the optimization works in a unidirectional way: upstream turbines influence the flow field, resulting in favorable conditions for their downstream neighbors, yet information on the possibility of active response and cooperation in the latter has no influence on upstream control actions.

Qualitative analysis of instantaneous flow fields led to the observation of
the quasi-periodic shedding of vortex rings from first-row turbines in the
optimal control case. This flow feature was successfully mimicked using simple
sinusoidal thrust actuation of the first row. The best parameter set for
these sinusoidal variations proved robust to both wind turbine spacing and
turbulence intensity, with an amplitude ${A}^{\ast}=\mathrm{1.5}$ and a
nondimensional frequency at ${\mathit{\text{St}}}^{\ast}=\mathrm{0.25}$. Interestingly, this
frequency corresponds to the peak at *St*=0.2…0.3 observed
in the first-row thrust coefficient spectra of the optimal control case.
Although the first-row sinusoidal control led to a robust increase in total
power for a reduced-size 4×4 wind farm, a full-scale test indicated
that downstream turbine activity is required to obtain increased power at
larger farm scales. It was also shown that the simple sinusoidal strategy
does not lead to increased power extraction when applied to downstream
intermediate turbines. Identifying the mechanisms for power increase in these
turbines hence remains an important open research question. Finally, it is
important to remark that all current simulations were performed using a
standard nonrotating actuator disk model without the inclusion of mechanical
turbine loading. Therefore, wind tunnel testing and/or simulations with more
advanced turbine models (such as the actuator line model) including
the assessment of turbine loading are essential to evaluate the real-life
applicability of the sinusoidal thrust strategy.

Data availability

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Data availability.

Datasets supporting this article can be found in a figshare repository. These datasets include time-averaged flow fields, optimized controls and optimized wind-farm power extraction for the case reported in this paper (Munters and Meyers, 2016, Figshare data collection repository, https://doi.org/10.6084/m9.figshare.c.3520113).

Competing interests

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Competing interests.

The authors declare that they have no conflict of interest.

Acknowledgements

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Acknowledgements.

The authors received funding from the European Union's Horizon 2020
research and innovation program under grant agreement no. 727680
(TotalControl). The authors also acknowledge funding by the European Research
Council under grant agreement no. 306471 (ActiveWindFarms). The computational
resources and services used in this work were provided by the VSC (Flemish
Supercomputer Center), funded by the Research Foundation – Flanders (FWO) and
the Flemish Government, department EWI.

Edited by: Sandrine Aubrun

Reviewed by: two anonymous referees

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Short summary

Wake interactions in wind farms result in power losses for downstream turbines. We aim to mitigate these losses through coordinated control of the induced slowdown of the wind by each turbine. We further analyze results from earlier work towards the utilization of such control strategies in practice. Coherent vortex shedding is identified and mimicked by a sinusoidal control. The latter is shown to increase power in downstream turbines and is robust to turbine spacing and turbulence intensity.

Wake interactions in wind farms result in power losses for downstream turbines. We aim to...

Wind Energy Science

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