2016
DOI: 10.14311/nnw.2016.26.018
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Paradoxes in Numerical Calculations

Abstract: Precise wind energy potential assessment is vital for wind energy generation and planning and development of new wind power plants. This work proposes and evaluates a novel two-stage method for location-specific wind energy potential assessment. It combines accurate statistical modelling of annual wind direction distribution in a given location with supervised machine learning of efficient estimators that can approximate energy efficiency coefficients from the parameters of optimized statistical wind direction… Show more

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Cited by 8 publications
(5 citation statements)
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“…Finally, from Equations (7) and (6), and Kepler's third law a3false/T2=GMfalse/()4π2$$ {a}^3/{T}^2={GM}_{\odot }/\left(4{\pi}^2\right) $$, it follows that after one period (more precisely, between two successive perihelion passages) the perihelion shifts about the angle left{right left}trueε=2false(ϕπfalse)=3παa1e2=3π2italicGMitalicac21e2=24π3a2T2c21e2,$$ {\displaystyle \begin{array}{cc}\varepsilon & =2\left(\phi -\pi \right)=3\pi \frac{\alpha }{a\left(1-{e}^2\right)}=3\pi \frac{2{GM}_{\odot }}{ac^2\left(1-{e}^2\right)}\\ {}& =24{\pi}^3\frac{a^2}{T^2{c}^2\left(1-{e}^2\right)},\end{array}} $$ that is, the relationship (1), which according to (2) yields the idealized value of the relativistic perihelion shift of Mercury 43″ per century. Here, one subtracts two numbers of almost the same size, namely ϕ – π , which is a delicate numerical operation, see Brandts et al (2016).…”
Section: A Methods Of Albert Einsteinmentioning
confidence: 99%
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“…Finally, from Equations (7) and (6), and Kepler's third law a3false/T2=GMfalse/()4π2$$ {a}^3/{T}^2={GM}_{\odot }/\left(4{\pi}^2\right) $$, it follows that after one period (more precisely, between two successive perihelion passages) the perihelion shifts about the angle left{right left}trueε=2false(ϕπfalse)=3παa1e2=3π2italicGMitalicac21e2=24π3a2T2c21e2,$$ {\displaystyle \begin{array}{cc}\varepsilon & =2\left(\phi -\pi \right)=3\pi \frac{\alpha }{a\left(1-{e}^2\right)}=3\pi \frac{2{GM}_{\odot }}{ac^2\left(1-{e}^2\right)}\\ {}& =24{\pi}^3\frac{a^2}{T^2{c}^2\left(1-{e}^2\right)},\end{array}} $$ that is, the relationship (1), which according to (2) yields the idealized value of the relativistic perihelion shift of Mercury 43″ per century. Here, one subtracts two numbers of almost the same size, namely ϕ – π , which is a delicate numerical operation, see Brandts et al (2016).…”
Section: A Methods Of Albert Einsteinmentioning
confidence: 99%
“…that is, the relationship (1), which according to (2) yields the idealized value of the relativistic perihelion shift of Mercury 43 ′′ per century. Here, one subtracts two numbers of almost the same size, namely 𝜙 -𝜋, which is a delicate numerical operation, see Brandts et al (2016).…”
Section: A Methods Of Albert Einsteinmentioning
confidence: 99%
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“…However, this is an ill-conditioned problem due to the subtraction of two quite inexact numbers of almost equal magnitude [7]. Moreover, the quantities O and C are not uniquely defined.…”
Section: Mercury's Perihelion Shift Revisitedmentioning
confidence: 99%
“…Further problems arise from the nonlinearity and instability of Einstein's equations, division by zero, subtraction of two inexact numbers of almost the same size. This usually leads to a catastrophic loss of accuracy [7]. Finally note that many conclusions in cosmology are not in the form of mathematical implications, since various simplifications and approximations are done.…”
mentioning
confidence: 99%