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A method is developed for calculating the intensification of heat transfer in the neighborhood of a stagnation point (line) of a body in a turbulent (uniform or jet) flow.
      
No binary matroid has a minor isomorphic toU42, the "four-point line", and Tutte showed that, conversely, every non-binary matroid has aU42 minor.
      
In this paper we present the best known theoretical algorithm and a practical subquadratic algorithm for computing a 50% breakdown point line estimator, the Siegel or repeated median line estimator.
      
If H is a hyperplane of a projective space P, and the point line geometry Γ has an embedding in P , then the pullback from H is a geometric hyperplane of Γ.
      
If q is odd, then moreover NQ+(3, q) satisfies the property that for each non-incident point line pair (x,L), there are either (q-1)/2 or (q+1)/2 points incident with L that are collinear with x.
      
The four independent diffusion coefficients were found to decrease rapidly along the constant plait-point line as the temperature approached the consolute or plait temperature.
      
We also show that this transformation is expressed as the symmetric component of the tensor product of the transformation based on point/line correspondences and itself.
      
In this paper, considering this problem from the point of view of Laguerre geometry, we reduce it to the classification of point/line and line/line pairs in the pseudo-Euclidean space with Lorenz metrics.
      
It follows from [5, 12] that any projective embedding of this point line geometry is a homomorphic image of the one afforded by the 56-dimensional module for the groupE7(K).
      
A raster display represents point line and area features by utilising a grid of values.
      
Any CC matroid can be obtained by a series of these operations starting from the 3-point line.
      
This states the the only obstruction to binary representability is the four point line U2,4.
      
This matching can be point/line/region based with a need for development of suitable similarity measures.
      
The position of SC4 and the ion open-closed field line boundary is marked with a white triangle on SC4's red magnetic foot point line.
      
The only CC matroid of dimension 1 is the 3 point line.
      
The solid line is for the lognormal SV model; the point line is for the N-SV model.
      
The time constants were calculated by fitting the currents with an exponential function and the data was fitted by a point-to-point line.
      
 

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