Conditions Definition and 1000 Threads

In mathematical optimization, the Karush–Kuhn–Tucker (KKT) conditions, also known as the Kuhn–Tucker conditions, are first derivative tests (sometimes called first-order necessary conditions) for a solution in nonlinear programming to be optimal, provided that some regularity conditions are satisfied.
Allowing inequality constraints, the KKT approach to nonlinear programming generalizes the method of Lagrange multipliers, which allows only equality constraints. Similar to the Lagrange approach, the constrained maximization (minimization) problem is rewritten as a Lagrange function whose optimal point is a saddle point, i.e. a global maximum (minimum) over the domain of the choice variables and a global minimum (maximum) over the multipliers, which is why the Karush–Kuhn–Tucker theorem is sometimes referred to as the saddle-point theorem.The KKT conditions were originally named after Harold W. Kuhn and Albert W. Tucker, who first published the conditions in 1951. Later scholars discovered that the necessary conditions for this problem had been stated by William Karush in his master's thesis in 1939.

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  1. J

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    Homework Statement Solve the diffusion equation: u_{xx}-\alpha^2 u_{t}=0 With the boundary and initial conditions: u(0,t)=u_{0} u(L,t)=u_{L} u(x,0=\phi(x) The Attempt at a Solution I want to solve using separation of variables... I start by assuming a solution of the form...
  2. M

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  3. D

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  4. B

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  6. C

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  7. F

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  8. V

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  9. D

    MHB Boundary conditions spherical coordinates

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  10. S

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  11. A

    Under what conditions does quantum mechanics reduce to classical mechanics?

    Homework Statement "At 310K thermal energy kT=4.28x(10^-21). Use the equation you derived above (which I worked out to be E=(n²h²)/(8mL²) )to determine under which conditions quantum mechanics reduces to classical mechanics." The hint was that "you need to find the value of mL² for which change...
  12. S

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  13. C

    Mapping Conditions in Transformational Space

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  14. M

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  15. D

    MHB Solving the Heat Equation with Initial Conditions

    I have already solved the main portions. I have $$ T(x,t) = \sum_{n = 1}^{\infty}A_n\cos\lambda_n x\exp(-\lambda_n^2t) $$ The eigenvalues are determined by $$ \tan\lambda_n = \frac{1}{\lambda_n} $$ The initial condition is $T(x,0) =1$. For the particular case of $f(x) = 1$, numerically...
  16. D

    MHB Orthogonality of Eigenfunctions of Mixed Boundary Conditions

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  17. B

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  18. T

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  19. T

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  20. A

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  21. G

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  22. R

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  23. mnb96

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  24. E

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  25. V

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  26. R

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  27. Runei

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  28. K

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  29. G

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  30. C

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  31. S

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  34. U

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  35. U

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  36. H

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  37. O

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  38. H

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  39. T

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  40. A

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  41. N

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  42. M

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  43. T

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  44. P

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  46. D

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  47. D

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  48. Evo

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  50. G

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