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The method depended upon finding the normal, the line perpendicular to the tangent, using the algebraic condition that it be the unique radius to intersect the curve in only one point.
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In the meantime, the total flux for the unique radius is convergent and can be calculated with considerably greater value Π H S ( k, n, 1 ) ≈ 19427.858848843922, while, e.g., for r = 2 the flux value is substantially greater and its value is obtained as Π HS ≈ 1375905492.377.
The variety Λ is shown to have the determinantal representationΛ="{ s,p ∈Γ:det(F+pF⁎−sI)="0}, where F is the unique matrix of numerical radius not greater than 1 that satisfiesS−S⁎P="(I−P⁎P 12F(I−P⁎P 12F
If T is completely continuous, then r ( L ), the spectral radius of T, is the unique positive eigenvalue of T with its eigenfunction in K.
The radius of the arc centerline was considered to be the femoral radius.
R is the hydraulic radius.
R * is the equivalent radius.
These are the core radius (rc), the half-light radius (rh), and the tidal radius (rt).
:*\scriptstyle R is the gas constant r_k is the Kelvin radius, the radius of the droplets.
This is the horizontal radius.
This is the vertical radius.
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