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To show this solution is global, we need to prove that (tau_{e}=infty) a.s.s
To show this solution is global, we need to show that τ e = ∞ a.s.s
To show this solution is global, we only need to show that (tau_{e}=infty ).
To show this solution is global, we need to show that (tau_{e}=infty) a.s.s
To show this solution is global, we need to show that a.s.s
It follows from the theory of SDE [6] that (2.7) has a unique local solution (x t)) on ([0,t_{e})), where (t_{e}) is the explosion time. To show this solution is global, we only need to prove that (t_{e}=+infty) a.s. Let (n_{0}) be sufficiently large such that (x 0)) remains in the interval ([ frac{1}{n_{0}}, n_{0}]).
Similar(51)
By using Theorem 3.5, we only can obtain the existence and uniqueness of solution of problem (4.2), however, it is not difficult to show this, and the exact solution is (u(t)=frac{t^{2}}{[2]_{q}}-t {[2]_{q}}-t
I do not sketch the outlines of this dizzying structure to show the solution to the problem of TV, merely to show what the problem really is — or what I think it really is.
To further demonstrate in practical applications and to show the solutions of this type of problems to civil engineers, a comprehensive parametric analysis and systematic calculations are performed with various controlling parameters to evaluate the dynamic response of the vibrating soil foundation system.
To show that this solution is global, we need to show that (tau_{infty}=infty) almost surely.
Now, we are going to show that this solution is global, that is, that (tau_{e}=infty) a.s.s
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Justyna Jupowicz-Kozak
CEO of Professional Science Editing for Scientists @ prosciediting.com