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SwRI engineers design, build and test a prototype wind turbine array

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Going Green<br />

<strong>SwRI</strong> <strong>engineers</strong> <strong>design</strong>,<br />

<strong>build</strong> <strong>and</strong> <strong>test</strong> a <strong>prototype</strong><br />

<strong>wind</strong> <strong>turbine</strong> <strong>array</strong><br />

By David L. Ransom, P.E. <strong>and</strong> J. Jeffrey Moore, Ph.D.<br />

An early move toward renewable,<br />

<strong>wind</strong>-derived electric power<br />

in the United States was made<br />

in the 1930s when rural power<br />

distribution was too expensive for energy<br />

companies to pursue. Wind <strong>turbine</strong>s of<br />

yesteryear were low-power devices that<br />

provided just enough power for radios<br />

<strong>and</strong> lights. As part of the movement to<br />

develop more renewable energy sources,<br />

<strong>wind</strong>-derived energy is once again a topic<br />

of growing interest. Today’s <strong>wind</strong> <strong>turbine</strong>s<br />

are built at the utility scale. Instead of<br />

300 or 400 watts on the ranch, utility <strong>wind</strong><br />

<strong>turbine</strong>s typically generate up to 3 megawatts,<br />

enough to power entire communities.<br />

This significant increase in power<br />

brings significant technical challenges.<br />

Issues such as mechanical reliability,<br />

production costs, <strong>and</strong> energy storage<br />

<strong>and</strong> distribution are of particular interest<br />

in today’s push for renewable energy.<br />

Southwest Research Institute has been<br />

involved in this growing research field,<br />

providing third-party engineering <strong>design</strong><br />

reviews of machinery reliability, modeling<br />

torsional dynamics of drivetrain<br />

components <strong>and</strong> <strong>test</strong>ing sub-scale <strong>prototype</strong>s<br />

of alternative concepts.<br />

A team of <strong>SwRI</strong> <strong>engineers</strong> recently<br />

assisted a client in <strong>test</strong>ing an alternative<br />

<strong>wind</strong> <strong>turbine</strong> concept that uses an <strong>array</strong><br />

of several small <strong>wind</strong> <strong>turbine</strong>s. In this<br />

concept, a single <strong>turbine</strong> of 200-meter<br />

diameter can be replaced with an <strong>array</strong><br />

of 20 <strong>turbine</strong>s, each having a diameter of<br />

45 meters; thus each <strong>design</strong> has the same<br />

swept area, the area swept by the revolving<br />

<strong>wind</strong> <strong>turbine</strong> blades. The client’s needs<br />

included validating the <strong>design</strong> concept,<br />

demonstrating power performance equivalent<br />

to that of a single <strong>turbine</strong> of the same<br />

swept area <strong>and</strong> developing a validated<br />

computer model for future <strong>design</strong><br />

studies. In support of the client’s development<br />

program, <strong>SwRI</strong> was contracted to<br />

validate the initial concept through experiment<br />

<strong>and</strong> computer simulation, looking<br />

for any possible blade-wake interactions<br />

between adjacent rotors, which might<br />

serve to either prevent some of the <strong>turbine</strong>s<br />

from reaching full power or lead to<br />

adverse blade dynamic stresses caused by<br />

the flow interaction at the <strong>turbine</strong> blade<br />

tips. The intent of this study was to validate<br />

the <strong>wind</strong> <strong>turbine</strong> <strong>array</strong> concept <strong>and</strong> gain<br />

an initial underst<strong>and</strong>ing of the anticipated<br />

2<br />

Technology Today • Summer 2009


D016925-2097<br />

David L. Ransom, P.E., (left) is a principal<br />

engineer in <strong>SwRI</strong>’s Fluids Engineering<br />

Department in the Mechanical <strong>and</strong> Materials<br />

Engineering Division. Ransom specializes in<br />

rotordynamics <strong>and</strong> structural dynamics for both<br />

energy <strong>and</strong> space exploration applications.<br />

Dr. J. Jeffrey Moore is a program manager in<br />

the Fluids Engineering Department. Moore’s<br />

areas of expertise include turbomachinery<br />

rotordynamics <strong>and</strong> fluid dynamics research for<br />

the natural gas, power generation <strong>and</strong> <strong>wind</strong><br />

power industries.<br />

D017017<br />

<strong>design</strong> challenges for a full-scale <strong>array</strong>.<br />

The <strong>SwRI</strong> team proposed to arrange<br />

multiple commercially available <strong>wind</strong><br />

<strong>turbine</strong>s in an <strong>array</strong> pattern <strong>and</strong> perform<br />

<strong>test</strong>s to evaluate the <strong>design</strong> for<br />

performance as well as mechanical<br />

integrity. <strong>SwRI</strong> researchers also used<br />

computational fluid dynamics to study<br />

the possible blade-wake or tip-vortex<br />

interactions between adjacent rotors.<br />

Wind tunnel <strong>test</strong>ing<br />

As a result of the initial evaluation,<br />

the <strong>SwRI</strong> team <strong>design</strong>ed, built <strong>and</strong> <strong>test</strong>ed<br />

a <strong>turbine</strong> <strong>array</strong> <strong>prototype</strong> to verify key<br />

performance characteristics <strong>and</strong> to support<br />

future <strong>design</strong> work<br />

on larger <strong>turbine</strong> <strong>array</strong>s.<br />

The <strong>array</strong> consisted of<br />

seven 400-watt, commercially<br />

available <strong>wind</strong><br />

<strong>turbine</strong>s constructed on<br />

a 25-foot-tall platform.<br />

The center <strong>turbine</strong> of the<br />

<strong>array</strong> was erected at a<br />

height of 15 feet to meet<br />

the centerline of the<br />

<strong>wind</strong> tunnel at NASA’s<br />

Langley Research Center<br />

in Hampton, Va. The<br />

Langley Full Scale Tunnel<br />

(LFST) is a National Historical<br />

L<strong>and</strong>mark significant<br />

to the advancement<br />

of aeronautical research<br />

dating from 1931 <strong>and</strong><br />

continuing today through model <strong>test</strong>s<br />

of all current front-line U.S. jet fighter<br />

aircraft. The tunnel is 50 feet in length, 60<br />

feet wide <strong>and</strong> 30 feet high.<br />

Performance <strong>test</strong> results<br />

Researchers added instrumentation<br />

to each <strong>turbine</strong> in <strong>SwRI</strong>’s seven-rotor <strong>array</strong><br />

to provide data on center <strong>turbine</strong> power,<br />

blade strain <strong>and</strong> <strong>turbine</strong> speed. Several<br />

flow visualization features were included<br />

in the experimental rig to better underst<strong>and</strong><br />

potential <strong>turbine</strong> interactions.<br />

The seven-rotor <strong>array</strong> was <strong>test</strong>ed in<br />

a variety of conditions, including varying<br />

the number of active <strong>turbine</strong>s, spacing<br />

between active <strong>turbine</strong>s, <strong>wind</strong> speed <strong>and</strong><br />

The <strong>wind</strong> <strong>turbine</strong> <strong>array</strong> was evaluated in the Langley Full Scale Tunnel,<br />

at NASA Langley Research Center, Hampton, Va. The center <strong>turbine</strong> is<br />

15 feet from the tunnel floor. The <strong>wind</strong> tunnel is 30 feet high.<br />

D017014<br />

Technology Today • Summer 2009 3


D017028<br />

Spacing study results for 9 meters per second <strong>wind</strong><br />

speed indicate no measurable difference in power<br />

performance of the middle <strong>turbine</strong> over the full range of<br />

spacing conditions.<br />

<strong>array</strong> yaw relative to <strong>wind</strong> direction. The<br />

results of all conditions were compared<br />

to the baseline performance results of a<br />

single <strong>turbine</strong>. The repeatability of the<br />

results was found to be around 4 percent.<br />

This demonstrates that even across a<br />

wide range of <strong>test</strong> article configurations,<br />

the maximum possible impact to <strong>turbine</strong><br />

performance is less than 4 percent, suggesting<br />

that performance from operation<br />

in an <strong>array</strong> configuration does not significantly<br />

affect performance.<br />

The <strong>SwRI</strong> team conducted a study in<br />

which the outer six <strong>turbine</strong>s were initially<br />

spaced at 2 percent of the diameter relative<br />

to the center <strong>turbine</strong>. Spacing was<br />

then incrementally increased to a maximum<br />

of 16 percent. Spacing study results<br />

indicated that the influence of the neighboring<br />

rotors in the full seven-rotor <strong>array</strong><br />

was not detectable within the repeatability<br />

of the <strong>test</strong> results. This indicated that<br />

any possible effects of rotor interaction<br />

on <strong>array</strong> performance were limited to less<br />

than 4 percent when compared to singlerotor<br />

performance. Tests run in the yaw<br />

condition did show a distinct drop in performance<br />

as expected, but the spacing<br />

influence in yaw was still negligible.<br />

Flow visualization<br />

Using a<br />

smoke rake integrated<br />

with the<br />

LFST traversing<br />

mechanism, <strong>SwRI</strong><br />

<strong>engineers</strong> injected<br />

smoke streams<br />

into the flow for<br />

overall streamline<br />

visualization. Initial<br />

results showed<br />

periodic fluctuations in the smoke streams<br />

corresponding to the vortex shedding frequency<br />

of the primary rake structure. This<br />

is an unsteady flow phenomenon in<br />

which vortices form behind an obstruction<br />

in the flow (the rake structure)<br />

<strong>and</strong> periodically detach, creating disturbances<br />

in the smoke flow. Because<br />

of this, additional smoke <strong>test</strong>ing was<br />

performed by rotating the rake so that<br />

the outflow ports of the tines were not<br />

directly downstream of this wake.<br />

The team attempted several variations<br />

in the smoke rake arrangements,<br />

such as spacing <strong>and</strong> restricting the number<br />

of tubes to obtain clearer images,<br />

but inherent turbulence in the flow<br />

made it difficult to generate a clear<br />

image of the flow field surrounding the<br />

A smoke generator <strong>and</strong> smoke rake were<br />

installed in the Langley Full Scale Tunnel.<br />

The traversing mechanism permitted remote<br />

control of rake location to help visualize flow<br />

at different locations on the <strong>array</strong>.<br />

D016580<br />

4<br />

Technology Today • Summer 2009


D017011<br />

Smoke streams illustrate periodic vortex shedding<br />

from the smoke rake wake on the smoke<br />

streams. The influence of vortex shedding is<br />

minimized by rotating the rake.<br />

<strong>turbine</strong>s. In still images <strong>and</strong> video, no<br />

clear structure of the flow field was evident<br />

because of the <strong>turbine</strong>s. St<strong>and</strong>ard<br />

<strong>and</strong> slow-motion video with stroboscopic<br />

illumination synchronized to the<br />

rotation of the center <strong>turbine</strong> showed<br />

the flow field passing through the <strong>turbine</strong><br />

planes with no apparent effect.<br />

This was evidenced by the fact that the<br />

strobe light could not “freeze” images of<br />

smoke patterns. Instead, the smoke continually<br />

moved in all recorded images.<br />

<strong>SwRI</strong> researchers used a mixture of<br />

titanium dioxide (TiO 2<br />

), kerosene <strong>and</strong><br />

oleic acid to record flow patterns on<br />

the rotating blades. The mixture was<br />

painted onto the front <strong>and</strong> back sides<br />

of one of the center <strong>turbine</strong> blades, <strong>and</strong><br />

the tunnel was subsequently brought<br />

up to operating condition. This allowed<br />

the TiO 2<br />

mixture to travel on the surface<br />

under the aerodynamic forces while the<br />

kerosene evaporated, leaving a trace of<br />

the surface flow patterns.<br />

The <strong>SwRI</strong> team installed a grid<br />

of retro-reflective tufts on the <strong>array</strong><br />

structure downstream of the <strong>turbine</strong><br />

blade plane to<br />

examine flow<br />

structure in the<br />

wake of the <strong>turbine</strong>s.<br />

During<br />

operation, the<br />

tufts reacted to<br />

the local flow<br />

field. Photographs<br />

of the<br />

tuft <strong>array</strong> showed the flow structure at<br />

the tuft grid for the two-rotor case when<br />

the center <strong>and</strong> upper rotors are separated<br />

by 2 percent. Capturing images in<br />

this configuration was difficult because<br />

of the added wake of the photographer<br />

<strong>and</strong> camera when filming from upstream<br />

of the <strong>turbine</strong> <strong>array</strong>. Nonetheless, the<br />

tufts showed some angularity in the wake<br />

of the two active <strong>turbine</strong>s <strong>and</strong> were very<br />

well aligned with the mean flow direction<br />

everywhere else. A more straight-on<br />

view might have shown the dividing line<br />

between the swirled flow at the bottom<br />

of the top <strong>turbine</strong> (swirled flow to the<br />

left) <strong>and</strong> the top of the middle <strong>turbine</strong><br />

(swirled flow to the right).<br />

D017013<br />

Strain gage measurements<br />

Researchers installed strain gages<br />

on a single blade of the <strong>array</strong>’s center<br />

<strong>turbine</strong>. The gages were placed at three<br />

locations: outboard, midboard <strong>and</strong> inboard<br />

from the tip <strong>and</strong> data was transmitted<br />

through a telemetry system. Measured<br />

root mean square (RMS) strain distribution<br />

at the 12 m/sec <strong>wind</strong> speed shows<br />

typical cantilever beam shape with peak<br />

strain at the inboard (IB) location <strong>and</strong><br />

minimum strain at the outboard (OB)<br />

location. This is an indication of the blade<br />

load distribution, which would demonstrate<br />

more variation between various<br />

Technology Today • Summer 2009 5


This photo shows grid tuft visualization for a<br />

two-rotor configuration at 2 percent <strong>turbine</strong><br />

<strong>array</strong> spacing.<br />

D017012<br />

spacing configurations if there was a<br />

real influence on <strong>turbine</strong> performance.<br />

These results show no clear difference<br />

in the RMS strain distribution, even with<br />

closely spaced <strong>turbine</strong>s.<br />

Researchers compared data from<br />

the frequency spectrum of the measured<br />

dynamic strain between the two-rotor<br />

data at 2 percent spacing <strong>and</strong> the full<br />

<strong>array</strong> data at 2 percent spacing, all at 9<br />

meters per second (m/sec) <strong>wind</strong> speed.<br />

The synchronous response was elevated<br />

for the two closely spaced rotor <strong>test</strong>s<br />

compared to the single rotor results. This<br />

indicates some amount of blade wake<br />

interaction, despite the inability to detect<br />

interaction with either performance measurement<br />

or flow visualization.<br />

Computational fluid dynamics (CFD)<br />

simulation<br />

To support future <strong>design</strong> studies,<br />

the research team developed <strong>and</strong> analyzed<br />

a CFD model of the <strong>test</strong> rotor for<br />

D017015<br />

various<br />

<strong>wind</strong> speed<br />

<strong>and</strong> <strong>turbine</strong><br />

spacing conditions.<br />

With a<br />

CFD simulation<br />

that was validated<br />

by experimental data,<br />

<strong>SwRI</strong> <strong>engineers</strong> gained<br />

more insight into the<br />

structure of the flow<br />

through the <strong>turbine</strong> <strong>array</strong>.<br />

Similar to the <strong>wind</strong> tunnel <strong>test</strong>s,<br />

a parametric spacing study was<br />

performed in CFD simulation with<br />

similar results. The CFD-predicted<br />

power performance of the <strong>turbine</strong>s<br />

was not strongly influenced by the<br />

<strong>array</strong> configuration. However, it was<br />

clear that there was some interaction<br />

between neighboring <strong>turbine</strong>s, such as a<br />

reduction in tangential velocity between<br />

two co-rotating <strong>turbine</strong>s.<br />

The center <strong>turbine</strong> blade was instrumented with six strain gages using<br />

a telemetry system to transmit data to the data acquisition system.<br />

The freestream <strong>wind</strong> flowing into<br />

the rotor blade usually generates a wake<br />

that develops downstream of the blade<br />

because of rotation. The wake can be<br />

divided into the central vortex<br />

generated by the hub <strong>and</strong> the<br />

tip vortex developed from<br />

the blade tip. The flow<br />

field results in an<br />

unusually complex<br />

three-dimensional<br />

vortex structure<br />

that was captured accurately<br />

with the<br />

CFD simulation<br />

for an <strong>array</strong> of<br />

two co-rotating<br />

<strong>turbine</strong>s. The interaction<br />

between the vortex structure<br />

produced by two co-rotating <strong>turbine</strong>s is<br />

quantified <strong>and</strong> power performance for the<br />

<strong>turbine</strong> <strong>array</strong> is predicted.<br />

6<br />

Technology Today • Summer 2009


The graph shows measured root mean square (RMS) strain<br />

distribution along the <strong>turbine</strong> blade. Measured<br />

results show no clear difference in RMS strain for varying<br />

<strong>turbine</strong> <strong>array</strong> spacing.<br />

Acknowledgments<br />

The authors would like to acknowledge the contributions<br />

of the other team members who made<br />

this project a success: Program Manager Leigh<br />

Griffith, Staff Scientist Dr. Jerome Helffrich, Research<br />

Engineer Dr. Vishy Iyengar, Research Engineer<br />

Jonathan Moody, Principal Technician Terry<br />

Schiebel, Engineer Melissa Wilcox <strong>and</strong><br />

former <strong>SwRI</strong> staff member Dr. Daniel Scharpf.<br />

D017029<br />

Future studies<br />

Based on the results of<br />

this combined experimental<br />

<strong>and</strong> analytical development<br />

program, <strong>SwRI</strong> researchers<br />

drew several conclusions<br />

regarding the operation of<br />

<strong>wind</strong> <strong>turbine</strong>s in a closely<br />

spaced <strong>array</strong>.<br />

Any possible effects of rotor interaction<br />

on <strong>array</strong> performance were limited<br />

to less than 4 percent when compared to<br />

single-rotor performance. Based on the<br />

single session repeatability, it was more<br />

likely that the influence of adjacent rotors<br />

was less than one percent for nearoptimum<br />

tip speed ratios. Operation in a<br />

yawed orientation did not impact the <strong>array</strong><br />

any more than it did a single rotor. Computational<br />

fluid dynamics tools can be<br />

used to model the multi-rotor concept,<br />

which can be very important in evaluating<br />

future <strong>wind</strong> <strong>turbine</strong> <strong>design</strong>s.<br />

The results of this activity were<br />

encouraging, <strong>and</strong> the experimental program<br />

provided a large amount of data<br />

to support future <strong>wind</strong> <strong>turbine</strong> <strong>array</strong><br />

development work. The performance<br />

data, flow visualization results <strong>and</strong> blade<br />

strain data can all be used to validate<br />

simulation tools as required in future<br />

<strong>design</strong> cycles. The progress made on the<br />

CFD modeling provided the knowledge<br />

necessary to more accurately model<br />

future <strong>design</strong>s with the ability to validate<br />

new ideas <strong>and</strong> techniques against existing<br />

experimental results. The effort<br />

expended in the current phase will continue<br />

to pay dividends as the <strong>wind</strong> <strong>turbine</strong><br />

<strong>array</strong> concept matures <strong>and</strong> reaches<br />

field operation. v<br />

Questions about this article<br />

Contact Ransom at (210) 522-5281 or<br />

david.ransom@swri.org or Moore at<br />

(210) 522-5812 or jeff.moore@swri.org.<br />

Computational fluid dynamic vector plot results demonstrate reduced tangential<br />

velocity at the interface between two <strong>turbine</strong>s. CFD simulation predicts only slight<br />

influence of adjacent <strong>turbine</strong>s on <strong>array</strong> performance.<br />

D017018<br />

Technology Today • Summer 2009 7

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