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model is too idealistic or the target is almost impossible to be stationary, the usual target tracking problem does not take into account the static model described above. However, in a soccer robot game, the target is still in a very high probability, such as the gatekeeper robot in most cases is static, and other play defensive or offensive role of the robot to reach its defensive position or the passing point will also stop to wait for further development of the situation. In these cases, on

Introduction Since Csdn's Markdown editor can easily support the formula representation of LATEX \latex.So, today, let's count the symbolic representation of the LATEX \latex mathematical formula so that we can look it up later. 1. Emphasis mode A^aˇ\hat{a}\check{a}a´a ' \acute{a}\grave{a}a¯a⃗\bar{a}\vec{a}a˙a¨\dot{a}\ddot{a}a˘a~\breve{a}\tilde{a} \begin{ Equation} \begin{array}{l} \hat{a} \text{\hat{a}} \acute{a} \text{\acute{a}} \bar{a} \text{

+\overbrace{b+\dots+b}^{m\mbox{\tiny 个}}}_{20\mbox{\scriptsize 个}}$ display as: \ (\underbrace{a+\overbrace{b+\dots+b}^{m\mbox{\tiny a}}}_{20\mbox{\scriptsize}}\) Mathematical Stress SymbolsTake a for example, if the letter I or J is accented, the letter i,y should be replaced with \imath, \jmath$$\hat{a}\check{a}\breve{a}\tilde{a}\bar{a}\vec{a}\acute{a}\grave{a}\mathring{a}\dot{a}\ddot{a}$$The results shown are:\[\hat{a}\check{a}\brev

Symmetric packed He Hermitian HB Hermitian band HP Hermitian packed Tr Triangular TB Triangular band TP Triangular packed Each operation is defined for four precisions, S Single real D Double real C Single Complex Z Double Complex Thus, for example, the name sgemm stands for "Single-precision general matrix-matrix multiply" and zgemm stands fo

} (\ Omega )? \) Space \ (\ Omega _ {open} \ subset \ mathbb {r} ^ {d }? \), \ (D \ Ge 1? \), And \ (\ Omega? \) YesLebesgueMeasurable.\ [\ Begin {Align *} \ mit L ^ {p} : = \ left \ {v \, \, \ big | \ int _ {\ Omega }\, \ left | V (x) \ right | \, ^ p \, DX \ Leq \ infty \ right \}, \, 1 \ Leq p \, Its norm is\ [\ Begin {Align *} | v | _ {\ mit L ^ {P }}:=\ left (\ int _ {\ Omega }\, \ left | V (x) \ right | \, ^ p \, DX \ right) ^ {1/p}, \, 1 \ Leq p \, \ (\ Mit L ^ {2} (\ Omega) \) space is

. \ [\ Begin {Align *} \ mit L ^ {p} : = \ left \ {v \, \, \ big | \ int _ {\ Omega }\, \ left | V (x) \ right | \, ^ p \, DX \ Leq \ infin \ right \}, \, 1 \ Leq p \, ? Its norm is\ [\ Begin {Align *} | v | _ {\ mit L ^ {P }}:=\ left (\ int _ {\ Omega }\, \ left | V (x) \ right | \, ^ p \, DX \ right) ^ {1/p}, \, 1 \ Leq p \, \ (\ Mit L ^ {2} (\ Omega) \) space is actually a Hilbert space assigned to the right inner product, $ (W, V){\ Mit L ^ {2} (\ Omega)} = \ int{\ Omega}, w (x

displacement and does not require time. the "Time-variant"δ function is 0 on T and the other times the same as D. "Virtual" \ (δw=\textbf{f}\cdotδ\textbf{r}\) the "ideal constraint" internal and external binding of the virtual force is zero. \ (\sum\limits_i\textbf{f}_{ni}\cdotδ\textbf{r}_i=0\) where the binding is recorded as FN Common Ideal constraints: 1. Particles moving along smooth surfaces 2. Two particles are connected by a rigid light rod 3. Two rigid bodies with smooth table contact M