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Exact(5)
Let û be the numerical solution of an obstacle problem.
Let (v^{k}_{i}) be the numerical solution computed by (4).
Let û and φ be the numerical solution and the lower obstacle, respectively.
Let u be the exact solution of the problem (1.4), and (u_{h}) be the numerical solution of scheme (3.1).
It follows that (Vert EVert =O(h^4).) We summarize the above result in the following theorem: Let y(x) be the exact solution of two-parameter singularly perturbed boundary value problem (1.1) and let (y_i) be the numerical solution obtained from the difference scheme (4.1).
Similar(55)
In order to improve accuracy, let (U^{n+1}=(V^{n+1}+W^{n+1})/2) be the numerical solutions at ((n+1))st time level. .
Then the average of two above values is chosen to be the numerical solutions at ((n+1))st time level.
and it is the numerical solution of an ordinary differential equation calculated in Timer1 ISR using 8 8 fixed point calculation.
The dashed line is the numerical solution of the perturbed oscillator's heat capacity.
The lines are the numerical solution to the respective switching differential equations described in the text.
This implies that the numerical solution to initial problem is the numerical solution to the random periodic solution.
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Since I tried Ludwig back in 2017, I have been constantly using it in both editing and translation. Ever since, I suggest it to my translators at ProSciEditing.

Justyna Jupowicz-Kozak
CEO of Professional Science Editing for Scientists @ prosciediting.com