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The main goal of this course is to get the necessary knowledge on atmospheric and fluid dynamics in order to quantify the wind resource of a local or regional area.
We’ll learn about basic meteorology, the specific dynamics of turbulent boundary layers and some standard techniques to estimate wind resources regardless of the type of turbine used or the level of efficiency achieved. Then, we will see what are the turbines characteristics to consider in order to estimate the electricity production from an isolated turbine or from a turbine farm. The differences and similarity between wind or marine resource assessment will also be discussed.
Finally, you will have the opportunity to get hands-on experience with real in-situ data sets and apply what you have learned on wind resource assessment.
Q1. Which one of these units is a unit of energy ?
Q2. What energy is of the same order of magnitude as 1 Toe ?
Q3. The amount of USEFUL ENERGY to heat a house during one year depends on
Q4. The amount of FINAL ENERGY to heat a house during one year depends on
Q5. Which of these power plants has a CAPACITY FACTOR mainly impacted by the variability of the resource ?
Q6. The CAPACITY FACTOR of a wind farm
Q7. The nameplate capacity of the off shore Horns Rev I wind farm is 160MW while its average annual energy generation is 600GWh. The mean capacity factor is therefore:
Q1. One nuclear reactor having a nominal power of 800MW generate an annual amount of 514k toe (1k =1000) of electricity. What is the correct capacity factor of this power unit ?
Q2. The above capacity factor is mainly due to
Q3. We consider an offshore wind farm of 150 turbines of 6MW of nominal power each. The annual capacity factor of this large wind farm is around 35%. The annual amount of electric energy produced will be around:
Q4. How many offshore wind turbines of 6MW (same capacity factor as Q3) will be needed to produce the same amount of annual energy as a nuclear reactor of 800MW having a capacity factor of 78%
Q5. We consider the above offshore wind farm of 150 turbines of 6MW of nominal power each. The annual capacity factor is around 35%. The typical seasonal variability of the energy production for this wind farm is given by the following graph:
This graph gives, in percentage, a relative value of the energy produced each month. The monthly mean energy (the annual energy /12) correspond to 100.
Find which statements are true.
Q1. The atmospheric layer absorb
Q2. The will be no winds if
Q3. The temperature of the troposphere decays with height mainly because
Q1. The vertical component of the Coriolis force
Q2. If we consider a small atmospheric structure having a typical horizontal scale L=H=10km and keeps all the other terms unchanged
Q3. In the tropics there is on average
Q1. Surface winds
Q2. The bottom drag
Q3. The boundary layer height
Q1. The Coriolis force
Q2. The geostrophic wind is a theoretical wind that
Q3. Close to the ground winds are also subjected to the bottom friction that result in a force opposite to wind direction. Find which sentence is true
Q4. On average, the strongest winds are located
Q5. The Rossby number is
Q6. Today we mainly extract wind power in
Q7. In the boundary layer, the winds tend to be
Q1. We consider an atmospheric boundary layer where the temperature (as the velocity field) can be decomposed in two terms, a steady temperature ⟨T⟩ and turbulent fluctuations. We can then write:
where ⟨. ⟩ corresponds to a statistical mean. The statistical average of the diffusion term
Q2. We keep here the same hypothesis and notations as in the previous question.The statistical average of the non-linear term
Q3. We keep here the same hypothesis and notations as in the previous question.The statistical average of the non-linear term
Q1. We consider the equation of advection-diffusion of heat within an 2D idealized atmospheric boundary layer :
where the temperature (as the velocity field) can be decomposed in two terms, a steady profile ⟨T⟩ and turbulent fluctuations. We consider that this idealized boundary layer is invariant along Oy, in other words ∂y = 0 for all the variables.
If we take into account the volume conservation in the xOz plane, the flow is non-divergent and satisfies
We can then re-write the equation (1)
Q2. If we apply the statistical mean to the modified equation (1) chosen above and if we assume that
Q1. The vertical profile of the horizontal wind speed is usually modeled by either a logarithmic law or a power law. Specify which of the following statement is true
Q2. The wind profile within a stable a strongly stratified boundary layer is better described by:
Q3. The 1/7 power law is more relevant for
Q4. The turbulence intensity of an atmospheric boundary layer:
Q5. The sea breeze winds
Q1. Which instrument will be the most accurate to quantify the turbulence intensity
Q2. The sodar measurements
Q3. The wind lidar measurements
Q4. Remote sensing instruments (lidar or sonar)
Q5. Specific hydrometeors or aerosols moving in the atmosphere
Q1. According to the Betz law the optimal turbine efficiency is reached when:
Q2. The underlying assumptions to derive the Betz law are
Q3. For a real turbine with fixed wind intensity and a fixed diameter
Q1. To optimize the efficiency of real turbines the tip speed of the blades should
Q2. There is generally no cut-out speed for marine turbines because
Q3. The turbulence of the upstream flow could modify the turbine efficiency by
Q1. The efficiency of a wind farm depends on
Q2. The efficiency of a single (isolated) wind turbine depends on
Q3. The relative downstream velocity deficit of an single (isolated) turbine wake depends
Q1. Wind probability distribution function (PDF) will be accurate for an annual resource assessment
Q2. At a given location, the wind distribution function is generally approximated by a Weibull law:
with k and C the two parameters of the law. Find which sentence is true ?
Q3. From your knowledge on meteorology and Weibull wind probability distribution law find which of the following sentences are true
Q4. The Weibull law will fit accurately the PDF of the observed winds when
Q5. We consider two distinct sites for which the following Weibull parameters have been determined:
Site 1: k=1.5, C=4.0 m/s
Site 2: k=2.2, C=4.1 m/s
To answer the following questions take the time to do some quantitative calculations using the following curve for the gamma function.
Q1. In a first step you are going to study the distribution of the shear exponent \alphaα throughout the year.
You need the wind data that you have already downloaded in the “in-video quizz” and the short code that you have written to compute a power law fit to the wind vertical profile of 2014/08/01. Write a code (based on a loop over the 4750 wind vertical profiles of the data file Lidar_wind_vertical_profiles.txt) that compute for each vertical profile the value of \alphaα.
You should obtain 4750 values of \alphaα with a minimum value of 0.003 and a maximum value of 0.839. Plot the histogram of \alphaα using intervals of width 0.02 for dividing the range of alpha from 0 to 0.84 (i.e. first interval: [0-0.02] and last interval [0.82-0.84]).
What kind of distribution of \alphaα is revealed by the histogram?
Q2. What is the median of the distribution of α ?
Answer:
Q3. The distribution of α that cover all measurements is bimodal. It should be possible to extract two distributions when restricting the data considered. Physically, we expect a variation of the shear exponent α between day and night. To investigate that point, extract from the set α the subset that corresponds to the daytime (defined between 8 a.m. and 7 p.m. included) and the subset that corresponds to the night (defined between 8 p.m. and 7 a.m. included). Afterwards, plot the histograms that represent the distributions of α for day and night separately.
What is the median of α during the daytime ?
Answer:
Q4. Recall that during the day, the heating of the sun tend to homogenize the boundary layer while during the night the boundary layer become stable which causes stratification. Using the two distributions of the shear exponents that you obtain for daytime and for the night and your knowledge of the boundary layer physics, select the good propositions.
Q5. We want now to investigate the typical variations of α throughout the year. For that purpose compute the median of α for each month for daytime and night separately. Plot for daytime on the one hand and for night on the other hand the evolution of the median of alpha as a function of the month.
Q6. What is the median value of alpha in July for the daytime period ?
Answer:
Q1. Download the file attached below that contains wind velocities at 40m and 140m.
Plot the histogram of the wind distributions at these two different altitudes. Using the method of power density method (described in the session “Weibull Rayleigh distribution”) fit the wind distribution to a Weibull distribution. You obtain for the two altitudes of 40m and 140m the shape parameters kk and the scale parameters cc.
What is the value in m/s of the scale parameter cc for the altitude of 40m ?
Note : at 140 you should obtain the following parameters : k=2.49k=2.49, C=7.67C=7.67m/s.
Answer:
Q2. For each altitude, superpose the histogram of the wind distributions and the probability density function of the Weibull distribution fit that you have computed. Which one of the following propositions is true ?
Q3. It is interesting to compare the Weibull fit that are obtained with different method. You can use the Maximum likelihood estimator (MLE as described in the session “Weibull Rayleigh distribution”) to compute another fit to the wind distributions. Which one of the following proposition is true ?
Note : The numerical software that you are using may have a built-in algorithm to compute a Weibull fit, see what method it uses to compute the shape and scale parameters.
Q4. We now imagine the situation, described in the previous video, where we only have the wind speed measures at the altitude of 40m and we want to extrapolate a Weibull distribution at the altitude of 140m.
With the shape and scale parameters that you have obtained at the altitude of 40m with the power density method, use the formula of Justus and Mikhail presented in the video to extrapolate from these values the parameters k_{140m}k140m and c_{140m}c140m. (Consider α=0.31 which corresponds to the median value of the distribution of α studied in the previous quizz)
Compare this set of parameters obtained by extrapolation to those directly computed from the wind speed measures at 140m. Keep the two sets of scale and shape parameters at the altitude of 140m, as they will be useful for the next quizz.
What is the value of k_{140m}k140m obtained by extrapolation ?
Answer:
Q1. The goal of that question is to compute the mean power of the wind turbine if it was installed on the site of SIRTA using the full set of measures that we have at 140m.
Discretize the wind speed range 0 to 20 m/s in intervals of width 0.1 m/s and count for each interval, the number of times the wind speed at 140 m/s belongs to that interval. Denote by V_1=0.05\, {m/s}V1=0.05m/s, V_2=0.15\, {m/s}V2=0.15m/s, … , V_{200}=19.95\, {m/s}V200=19.95m/s the 200 mean wind speed values of the intervals. The number of times, the measured wind speed V \in (V_i-0.05,V_i+0.05)V∈(Vi−0.05,Vi+0.05) is denoted by N_iNi.
Based on the power curve V P(V)V↦P(V) of the 2 MW wind turbine given in the previous video and the histogram of wind velocities at 140 m compute the mean power of the wind turbine with the formula:
P_{mean}={\sum_i N_i P(V_i)}{_i N_i} Pmean=∑iNi∑iNiP(Vi) .
Give P_{mean}Pmean in kW.
Answer:
Q2. Give, in percent (%), the capacity factor of that wind turbine if it was installed on the site of SIRTA.
Answer:
Q3. We now want to quantify the error that we would make in estimating the annual mean power of the wind turbine by using the Weibull distribution with the parameters directly computed with the power density method at 140m.
Compute the annual mean power of the wind turbine using the probability density function of the Weibull distribution f(V)f(V) with the parameters k_{140m}=2.49k140m=2.49 and c_{140m}=7.67 \, {m/s}c140m=7.67m/s:
P_{mean}=_{V=0}^{\infty} P(V) f(V){d}VPmean=∫V=0∞P(V)f(V)dV
Give P_{mean}Pmean in kW.
Answer:
Q4. By computing the annual mean power of the wind turbine using the Weibull distribution obtained by extrapolation from the measures at the altitude of 40 m (i.e., k_{140m}^{extra}=2.62k140mextra=2.62 and c_{140m}^{extra}=7.63 \, \mathrm{m/s}c140mextra=7.63m/s) we obtain: P_{mean}=646 \mathrm{kW}Pmean=646kW.
In that context, it means that an industrial that would install a mast at the height of 40 m and extrapolate the Weibull distribution at 140 m in order to asses the annual power production of a wind turbine at this location will:
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