Nodal Discontinuous Galerkin Methods:
Nodal Discontinuous Galerkin Methods:
Nodal Discontinuous Galerkin Methods:
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5<br />
85, +17 : a(u x , v) Ω should be a(u x , φ) Ω<br />
87, +3 : ‖ε N ‖ 2 Ω,h should be ‖ε h‖ 2 Ω,h<br />
89, +16 : Should be<br />
[<br />
− iωh<br />
2 M + aS . . .<br />
has the meaning of the interpolation of the pro-<br />
109, last equation : Should be ν → 0 in lim.<br />
118, Sec 5.2 : Clarification: In this section, fh k<br />
jection of f, i.e.,<br />
N p<br />
∑<br />
fh k (x, t) = (P N f)(x i , t)l k i (x).<br />
This is equivalent to assuming that all integrals are exact.<br />
119, -8 : ”from” should be ”form”.<br />
122, +5 : Eq.(5.8) should be<br />
1 d<br />
2 dt ‖u h‖ 2 Ω,h ≤ 0.<br />
i=1<br />
123, -8 : Last expression should be<br />
N<br />
∑ p<br />
fh k (x, t) = fh k (x k i , t)l k i (x),<br />
i=1<br />
124, +3 : u k h (x i, t) should be u k h (xk i , t).<br />
130, +10 : Eq.(5.16), lower limit should be η c < η ≤ 1.<br />
134, -3 : The statement is only true for ˆn = 1. The general statement should be<br />
ˆn · (au) ∗ =<br />
2a+ a − (<br />
a + + a − {{u}} + 1 )<br />
2 [u]<br />
151, -9 : Should be<br />
ul = uh; ul(3:Np,:) =0; ul = V*ul;<br />
162,-1 to 163, +2 : Statements<br />
drho (mapI) = ...<br />
drhou(mapI) = ...<br />
dEner(mapI) = ...