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2131 - 2140 of 13135 for Second Fundamental Theoremof CalculusSearch Results
The partial differential equation u_t=u_(xxx)u^3.
Let X be a metric space, A be a subset of X, and d a number >=0. The d-dimensional Hausdorff measure of A, H^d(A), is the infimum of positive numbers y such that for every ...
For n>=3, there exist no additive finite and invariant measures for the group of displacements in R^n.
The havercosine, also called the haversed cosine, is a little-used trigonometric function defined by havercosz = vercosz (1) = 1/2(1+cosz), (2) where vercosz is the vercosine ...
A metric on a bunch of segments with a common endpoint O, which defines the distance between two points P_1 and P_2 as the length of the shortest path connecting them inside ...
The system of partial differential equations S_t=SxS_(xx).
In bipolar coordinates, the Helmholtz differential equation is not separable, but Laplace's equation is.
The Helmholtz differential equation is not separable in bispherical coordinates.
The Helmholtz differential equation is not separable in toroidal coordinates
An absolutely continuous measure on partialD whose density has the form exp(x+y^_), where x and y are real-valued functions in L^infty, ||y||_infty<pi/2, exp is the ...
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