I wonder if the truncation error that I derived in the following approximation really has order 2? If so I also wonder what happens to the $u_{xxxx}$ term since it does not cancel out? $$u^n_{j+2}-4u^n_{j+1}+6u^n_j-4u^n_{j-1}+u^n_{j-2}$$ $$=\frac{1}{\Delta x^4}(u+2\Delta x u_x+\frac{4}{2}\Delta x^2 u_{xx}+\frac{8}{3!}\Delta x^3u_{xxx}+\frac{16}{4!}\Delta x^4 u_{xxxx}+\frac{32}{5!}\Delta x^5 u_{xxxxx}+\frac{64}{6!}\Delta x^6 u_{xxxxxx}$$ $$ -4(u+\Delta x u_x+\frac{1}{2}\Delta x^2 u_{xx}+\frac{1}{3!}\Delta x^3 u_{xxx}+\frac{1}{4!} \Delta x^4 u_{xxxx}+\frac{1}{5!}\Delta x^5 u_{xxxxx}+\frac{1}{6!}\Delta x^6 u_{xxxxxx})$$ $$ +6u-4(u-\Delta x u_x + \frac{1}{2} \Delta x^2 u_{xx} - \frac{1}{3!} \Delta x^3 u_{xxx}+ \frac{1}{4!}\Delta x^4 u_{xxxx}-\frac{1}{5!}\Delta x^5 u_{xxxxx}+\frac{1}{6!}\Delta x^6 u_{xxxxxx})$$ $$+u-2\Delta x u_x + \frac{4}{2}\Delta x^2 u_{xx}-\frac{8}{3!} \Delta x^3 u_{xxx}+ \frac{16}{4!} \Delta x^4 u_{xxxx}-\frac{32}{5!}\Delta x^5 u_{xxxxx}+\frac{64}{6!}\Delta x^6 u_{xxxxxx}+O(\Delta x^7))$$ $$=O(\Delta x^2)$$
2026-02-23 02:52:20.1771815140
Truncation error
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By taylor series expansions (setting $\Delta x=h$)
\begin{align}u^n_{j+2}&=u+2h u_x+4h^2u_{xx}+8h^3u_{xxx}+16h^4 u_{xxxx}+32h^5u_{xxxxx}+64h^6u_{xxxxxx}\\&+O(h^7),\\ -4u^n_{j+1}&=-4u-4h u_x-4h^2u_{xx}-4h^3u_{xxx}-4h^4 u_{xxxx}-4h^5u_{xxxxx}-4h^6u_{xxxxxx}\\&+O(h^7),\\ 6u^n_{j}&=6u,\\ -4u^n_{j-1}&=-4u+4h u_x-4h^2u_{xx}+4h^3u_{xxx}-4h^4 u_{xxxx}+4h^5u_{xxxxx}-4h^6u_{xxxxxx}\\&+O(h^7),\\ u^n_{j-2}&=u-2h u_x+4h^2u_{xx}-8h^3u_{xxx}+16h^4 u_{xxxx}-32h^5u_{xxxxx}+64h^6u_{xxxxxx}\\&+O(h^7), \end{align}
we see that everything cancels up to the $u_{xxxx}$ terms as
$$16h^4-4h^4-4h^4+16h^4 \ne 0.$$
The $u_{xxxxxx}$ terms also don't cancel because
$$64h^6-4h^6-4h^6+64h^6 \neq 0,$$
so if we make the above cancellations then
\begin{align}\frac {1}{h^4}\left(u^n_{j+2}-4u^n_{j+1}+6u^n_j-4u^n_{j-1}+u^n_{j-2}\right)&=24u_{xxxx}+120h^2u_{xxxxxx}\\&= 24u_{xxxx}+O(h^2). \end{align}