数值分析作业插值法2

发布于:2025-03-26 ⋅ 阅读:(271) ⋅ 点赞:(0)

埃尔米特插值

不仅要求函数值重合,而且要求若干阶导数也重合,这种插值问题称为埃尔米特插值问题。

低次埃尔米特插值多项式

  1. 二点三次埃尔米特插值多项式

    **问题描述:**给定区间 [ x 0 , x 1 ] [x_0, x_1] [x0​,x1​] 两端点的函数值与导数值:

    x x x x 0 x_0 x0​ x 1 x_1 x1​
    f ( x ) f(x) f(x) y 0 y_0 y0​ y 1 y_1 y1​
    f ′ ( x ) f'(x) f′(x) m 0 m_0 m0​ m 1 m_1 m1​

    要求构造三次多项式 H 3 ( x ) H_3(x) H3​(x),满足:
    { H 3 ( x 0 ) = y 0 , H 3 ( x 1 ) = y 1 H 3 ′ ( x 0 ) = m 0 , H 3 ′ ( x 1 ) = m 1 \begin{cases} H_3(x_0) = y_0, & H_3(x_1) = y_1 \\ H_3'(x_0) = m_0, & H_3'(x_1) = m_1 \end{cases} {H3​(x0​)=y0​,H3′​(x0​)=m0​,​H3​(x1​)=y1​H3′​(x1​)=m1​​


    解法形式

    设 H 3 ( x ) H_3(x) H3​(x) 为:
    H 3 ( x ) = α 0 ( x ) y 0 + α 1 ( x ) y 1 + β 0 ( x ) m 0 + β 1 ( x ) m 1 H_3(x) = \alpha_0(x)y_0 + \alpha_1(x)y_1 + \beta_0(x)m_0 + \beta_1(x)m_1 H3​(x)=α0​(x)y0​+α1​(x)y1​+β0​(x)m0​+β1​(x)m1​
    其中 α i ( x ) \alpha_i(x) αi​(x) 和 β i ( x ) \beta_i(x) βi​(x) 为基函数(三次式),满足以下条件:

    1. 插值条件:

      • α i ( x j ) = δ i j \alpha_i(x_j) = \delta_{ij} αi​(xj​)=δij​( δ i j \delta_{ij} δij​ 为克罗内克函数)
      • α i ′ ( x j ) = 0 \alpha'_i(x_j) = 0 αi′​(xj​)=0
      • β i ( x j ) = 0 \beta_i(x_j) = 0 βi​(xj​)=0
      • β i ′ ( x j ) = δ i j \beta'_i(x_j) = \delta_{ij} βi′​(xj​)=δij​
    2. 基函数构造:
      [
      \alpha_i(x) = (a_i x + b_i) l_i^2(x), \quad \beta_i(x) = c_i(x - x_i) l_i^2(x)
      ]
      其中 l i ( x ) = x − x j x i − x j l_i(x) = \frac{x - x_j}{x_i - x_j} li​(x)=xi​−xj​x−xj​​( j ≠ i j \neq i j=i)为拉格朗日基函数。


    基函数推导

    α 0 ( x ) \alpha_0(x) α0​(x) 的构造
    通过条件 α 0 ( x 0 ) = 1 \alpha_0(x_0) = 1 α0​(x0​)=1 和 α 0 ′ ( x 0 ) = 0 \alpha'_0(x_0) = 0 α0′​(x0​)=0,解得:
    { a 0 = − 2 x 0 − x 1 , b 0 = 1 + 2 x 0 x 0 − x 1 \begin{cases} a_0 = -\dfrac{2}{x_0 - x_1}, \\ b_0 = 1 + \dfrac{2x_0}{x_0 - x_1} \end{cases} ⎩ ⎨ ⎧​a0​=−x0​−x1​2​,b0​=1+x0​−x1​2x0​​​
    最终形式为:
    α 0 ( x ) = ( 1 − 2 x − x 0 x 0 − x 1 ) ( x − x 1 x 0 − x 1 ) 2 \alpha_0(x) = \left(1 - 2\dfrac{x - x_0}{x_0 - x_1}\right)\left(\dfrac{x - x_1}{x_0 - x_1}\right)^2 α0​(x)=(1−2x0​−x1​x−x0​​)(x0​−x1​x−x1​​)2
    α 1 ( x ) = ( 1 − 2 x − x 1 x 1 − x 0 ) ( x − x 0 x 1 − x 0 ) 2 \alpha_1(x) = \left(1 - 2\dfrac{x - x_1}{x_1 - x_0}\right)\left(\dfrac{x - x_0}{x_1 - x_0}\right)^2 α1​(x)=(1−2x1​−x0​x−x1​​)(x1​−x0​x−x0​​)2
    β i ( x ) \beta_i(x) βi​(x) 的构造
    β 0 ( x ) = ( x − x 0 ) ( x − x 1 x 0 − x 1 ) 2 , β 1 ( x ) = ( x − x 1 ) ( x − x 0 x 1 − x 0 ) 2 \beta_0(x) = (x - x_0)\left(\dfrac{x - x_1}{x_0 - x_1}\right)^2, \quad \beta_1(x) = (x - x_1)\left(\dfrac{x - x_0}{x_1 - x_0}\right)^2 β0​(x)=(x−x0​)(x0​−x1​x−x1​​)2,β1​(x)=(x−x1​)(x1​−x0​x−x0​​)2


    最终表达式
    H 3 ( x ) = y 0 ( 1 − 2 x − x 0 x 0 − x 1 ) ( x − x 1 x 0 − x 1 ) 2 H_3(x) = y_0\left(1 - 2\dfrac{x - x_0}{x_0 - x_1}\right)\left(\dfrac{x - x_1}{x_0 - x_1}\right)^2 H3​(x)=y0​(1−2x0​−x1​x−x0​​)(x0​−x1​x−x1​​)2

    • y 1 ( 1 − 2 x − x 1 x 1 − x 0 ) ( x − x 0 x 1 − x 0 ) 2 y_1\left(1 - 2\dfrac{x - x_1}{x_1 - x_0}\right)\left(\dfrac{x - x_0}{x_1 - x_0}\right)^2 y1​(1−2x1​−x0​x−x1​​)(x1​−x0​x−x0​​)2
    • m 0 ( x − x 0 ) ( x − x 1 x 0 − x 1 ) 2 m_0(x - x_0)\left(\dfrac{x - x_1}{x_0 - x_1}\right)^2 m0​(x−x0​)(x0​−x1​x−x1​​)2
    • m 1 ( x − x 1 ) ( x − x 0 x 1 − x 0 ) 2 m_1(x - x_1)\left(\dfrac{x - x_0}{x_1 - x_0}\right)^2 m1​(x−x1​)(x1​−x0​x−x0​​)2

    ∑ i = 0 1 α i ( x ) = 1 (当  f ( x ) = 1  时) \sum_{i=0}^1 \alpha_i(x) = 1 \quad \text{(当 $f(x) = 1$ 时)} i=0∑1​αi​(x)=1(当 f(x)=1 时)

    余项为:
    R ( x ) = 1 4 ! f ( 4 ) ( ξ ) ( x − x 0 ) 2 ( x − x 1 ) 2 , ξ ∈ ( x 0 , x 1 ) R(x) = \frac{1}{4!}f^{(4)}(\xi)(x - x_0)^2(x - x_1)^2, \quad \xi \in (x_0, x_1) R(x)=4!1​f(4)(ξ)(x−x0​)2(x−x1​)2,ξ∈(x0​,x1​)

  2. 三点三次带一个导数值的插值多项式

    问题描述
    给定函数表如下:

    x x x x 0 x_0 x0​ x 1 x_1 x1​ x 2 x_2 x2​
    f ( x ) f(x) f(x) y 0 y_0 y0​ y 1 y_1 y1​ y 2 y_2 y2​
    f ′ ( x ) f'(x) f′(x) m 1 m_1 m1​

    要求构造三次多项式 H 3 ( x ) H_3(x) H3​(x),满足:
    { H 3 ( x i ) = y i , i = 0 , 1 , 2 H 3 ′ ( x 1 ) = m 1 \begin{cases} H_3(x_i) = y_i, & i = 0, 1, 2 \\ H_3'(x_1) = m_1 \end{cases} {H3​(xi​)=yi​,H3′​(x1​)=m1​​i=0,1,2

    解法形式
    利用满足插值条件的 Newton 插值多项式,设:
    H 3 ( x ) = y 0 + f [ x 0 , x 1 ] ( x − x 0 ) + f [ x 0 , x 1 , x 2 ] ( x − x 0 ) ( x − x 1 ) + k ( x − x 0 ) ( x − x 1 ) ( x − x 2 ) H_3(x) = y_0 + f[x_0, x_1](x - x_0) + f[x_0, x_1, x_2](x - x_0)(x - x_1) + k(x - x_0)(x - x_1)(x - x_2) H3​(x)=y0​+f[x0​,x1​](x−x0​)+f[x0​,x1​,x2​](x−x0​)(x−x1​)+k(x−x0​)(x−x1​)(x−x2​)
    其中 k k k 为待定系数。

    待定系数求解
    通过导数条件 H 3 ′ ( x 1 ) = m 1 H_3'(x_1) = m_1 H3′​(x1​)=m1​ 确定 k k k:
    H 3 ′ ( x 1 ) = f [ x 0 , x 1 ] + f [ x 0 , x 1 , x 2 ] ( x 1 − x 0 ) + k ( x 1 − x 0 ) ( x 1 − x 2 ) = m 1 H_3'(x_1) = f[x_0, x_1] + f[x_0, x_1, x_2](x_1 - x_0) + k(x_1 - x_0)(x_1 - x_2) = m_1 H3′​(x1​)=f[x0​,x1​]+f[x0​,x1​,x2​](x1​−x0​)+k(x1​−x0​)(x1​−x2​)=m1​
    解得:
    k = m 1 − f [ x 0 , x 1 ] − f [ x 0 , x 1 , x 2 ] ( x 1 − x 0 ) ( x 1 − x 0 ) ( x 1 − x 2 ) k = \frac{m_1 - f[x_0, x_1] - f[x_0, x_1, x_2](x_1 - x_0)}{(x_1 - x_0)(x_1 - x_2)} k=(x1​−x0​)(x1​−x2​)m1​−f[x0​,x1​]−f[x0​,x1​,x2​](x1​−x0​)​

    最终表达式
    将 k k k 代入后, H 3 ( x ) H_3(x) H3​(x) 的完整形式为:
    H 3 ( x ) = y 0 + f [ x 0 , x 1 ] ( x − x 0 ) + f [ x 0 , x 1 , x 2 ] ( x − x 0 ) ( x − x 1 ) H_3(x) = y_0 + f[x_0, x_1](x - x_0) + f[x_0, x_1, x_2](x - x_0)(x - x_1) H3​(x)=y0​+f[x0​,x1​](x−x0​)+f[x0​,x1​,x2​](x−x0​)(x−x1​)

    • m 1 − f [ x 0 , x 1 ] − f [ x 0 , x 1 , x 2 ] ( x 1 − x 0 ) ( x 1 − x 0 ) ( x 1 − x 2 ) ( x − x 0 ) ( x − x 1 ) ( x − x 2 ) \frac{m_1 - f[x_0, x_1] - f[x_0, x_1, x_2](x_1 - x_0)}{(x_1 - x_0)(x_1 - x_2)} (x - x_0)(x - x_1)(x - x_2) (x1​−x0​)(x1​−x2​)m1​−f[x0​,x1​]−f[x0​,x1​,x2​](x1​−x0​)​(x−x0​)(x−x1​)(x−x2​)

    余项为:
    R ( x ) = 1 4 ! f ( 4 ) ( ξ ) ( x − x 0 ) ( x − x 1 ) 2 ( x − x 2 ) , ξ ∈ ( x 0 , x 2 ) R(x) = \frac{1}{4!}f^{(4)}(\xi)(x - x_0)(x - x_1)^2(x - x_2), \quad \xi \in (x_0, x_2) R(x)=4!1​f(4)(ξ)(x−x0​)(x−x1​)2(x−x2​),ξ∈(x0​,x2​)

一般埃尔米特插值多项式

问题描述
已知节点 x 0 , x 1 , … , x n x_0, x_1, \ldots, x_n x0​,x1​,…,xn​ 处的函数值 y 0 , y 1 , … , y n y_0, y_1, \ldots, y_n y0​,y1​,…,yn​ 和导数值 y 0 ′ , y 1 ′ , … , y n ′ y'_0, y'_1, \ldots, y'_n y0′​,y1′​,…,yn′​,要求构造次数为 2 n + 1 2n+1 2n+1 的多项式 H 2 n + 1 ( x ) H_{2n+1}(x) H2n+1​(x)(这样的Hermite 插值唯一),满足:
{ H 2 n + 1 ( x i ) = y i , H 2 n + 1 ′ ( x i ) = y i ′ ( i = 0 , 1 , … , n ) \begin{cases} H_{2n+1}(x_i) = y_i, \\ H'_{2n+1}(x_i) = y'_i \end{cases} \quad (i = 0, 1, \ldots, n) {H2n+1​(xi​)=yi​,H2n+1′​(xi​)=yi′​​(i=0,1,…,n)

解法形式
设多项式为:
H 2 n + 1 ( x ) = ∑ i = 0 n y i α i ( x ) + ∑ i = 0 n y i ′ β i ( x ) H_{2n+1}(x) = \sum_{i=0}^n y_i \alpha_i(x) + \sum_{i=0}^n y'_i \beta_i(x) H2n+1​(x)=i=0∑n​yi​αi​(x)+i=0∑n​yi′​βi​(x)
其中基函数 α i ( x ) \alpha_i(x) αi​(x) 和 β i ( x ) \beta_i(x) βi​(x) 满足:
{ α i ( x j ) = δ i j , α i ′ ( x j ) = 0 β i ( x j ) = 0 , β i ′ ( x j ) = δ i j \begin{cases} \alpha_i(x_j) = \delta_{ij}, & \alpha'_i(x_j) = 0 \\ \beta_i(x_j) = 0, & \beta'_i(x_j) = \delta_{ij} \end{cases} {αi​(xj​)=δij​,βi​(xj​)=0,​αi′​(xj​)=0βi′​(xj​)=δij​​

α i ( x ) \alpha_i(x) αi​(x) 和 β i ( x ) \beta_i(x) βi​(x) 均为 2 n + 1 2n+1 2n+1 次多项式。
基函数构造

α i ( x ) \alpha_i(x) αi​(x) 的构造

  1. 零点性质: α i ( x ) \alpha_i(x) αi​(x) 在 x 0 , x 1 , … , x n x_0, x_1, \ldots, x_n x0​,x1​,…,xn​ 处有二重零点(除 x i x_i xi​ 外)。

  2. 形式假设:
    α i ( x ) = [ A i x + B i ] l i 2 ( x ) \alpha_i(x) = [A_i x + B_i] l_i^2(x) αi​(x)=[Ai​x+Bi​]li2​(x)
    其中 l i ( x ) = ∏ j ≠ i x − x j x i − x j l_i(x) = \prod_{\substack{j \neq i}} \dfrac{x - x_j}{x_i - x_j} li​(x)=∏j=i​​xi​−xj​x−xj​​ 为拉格朗日基函数。

  3. 条件求解:

    • α i ( x i ) = 1 ⇒ B i = 1 \alpha_i(x_i) = 1 \Rightarrow B_i = 1 αi​(xi​)=1⇒Bi​=1
    • α i ′ ( x i ) = 0 ⇒ A i = − 2 l i ′ ( x i ) \alpha'_i(x_i) = 0 \Rightarrow A_i = -2 l_i'(x_i) αi′​(xi​)=0⇒Ai​=−2li′​(xi​)

    最终形式为:
    α i ( x ) = [ 1 − 2 l i ′ ( x i ) ( x − x i ) ] l i 2 ( x ) \alpha_i(x) = \left[ 1 - 2 l_i'(x_i)(x - x_i) \right] l_i^2(x) αi​(x)=[1−2li′​(xi​)(x−xi​)]li2​(x)

β i ( x ) \beta_i(x) βi​(x) 的构造

  1. 零点性质: β i ( x ) \beta_i(x) βi​(x) 在 x 0 , x 1 , … , x n x_0, x_1, \ldots, x_n x0​,x1​,…,xn​ 处有二重零点(除 x i x_i xi​ 外)。

  2. 形式假设:
    [
    \beta_i(x) = C_i (x - x_i) l_i^2(x)
    ]

  3. 条件求解:

    • β i ′ ( x i ) = 1 ⇒ C i = 1 \beta'_i(x_i) = 1 \Rightarrow C_i = 1 βi′​(xi​)=1⇒Ci​=1

    最终形式为:
    β i ( x ) = ( x − x i ) l i 2 ( x ) \beta_i(x) = (x - x_i) l_i^2(x) βi​(x)=(x−xi​)li2​(x)

余项分析
设区间 [ a , b ] [a, b] [a,b] 满足 a = x 0 < x 1 < ⋯ < x n = b a = x_0 < x_1 < \cdots < x_n = b a=x0​<x1​<⋯<xn​=b,且 f ∈ C 2 n + 2 [ a , b ] f \in C^{2n+2}[a, b] f∈C2n+2[a,b],则插值余项为:
R n ( x ) = f ( 2 n + 2 ) ( ξ ) ( 2 n + 2 ) ! [ ∏ i = 0 n ( x − x i ) ] 2 R_n(x) = \frac{f^{(2n+2)}(\xi)}{(2n+2)!} \left[ \prod_{i=0}^n (x - x_i) \right]^2 Rn​(x)=(2n+2)!f(2n+2)(ξ)​[i=0∏n​(x−xi​)]2
其中 ξ ∈ ( a , b ) \xi \in (a, b) ξ∈(a,b)。

分段低次插值

分段线性插值

定义
设已知节点 a < x 0 < x 1 < ⋯ < x n = b a < x_0 < x_1 < \cdots < x_n = b a<x0​<x1​<⋯<xn​=b 处的函数值为 f 0 , f 1 , … , f n f_0, f_1, \ldots, f_n f0​,f1​,…,fn​,记区间宽度:
h k = x k + 1 − x k , h = max ⁡ k h k h_k = x_{k+1} - x_k, \quad h = \max_k h_k hk​=xk+1​−xk​,h=kmax​hk​
分段线性插值通过折线段连接插值点逼近 f ( x ) f(x) f(x),构造折线函数 I h ( x ) I_h(x) Ih​(x) 满足:

  1. 连续性: I h ( x ) ∈ C [ a , b ] I_h(x) \in C[a, b] Ih​(x)∈C[a,b]
  2. 插值条件: I h ( x k ) = f k ( k = 0 , 1 , … , n ) I_h(x_k) = f_k \quad (k = 0, 1, \ldots, n) Ih​(xk​)=fk​(k=0,1,…,n)
  3. 分段线性:在每段区间 [ x k , x k + 1 ] [x_k, x_{k+1}] [xk​,xk+1​] 上, I h ( x ) I_h(x) Ih​(x) 为线性函数。

分段线性插值函数可表示为:
I h ( x ) = ∑ k = 0 n f k l k ( x ) I_h(x) = \sum_{k=0}^n f_k l_k(x) Ih​(x)=k=0∑n​fk​lk​(x)
其中 l k ( x ) l_k(x) lk​(x) 为分段线性基函数。

基函数定义
基函数 l k ( x ) l_k(x) lk​(x) 在区间内的表达式为:
l k ( x ) = { x − x k − 1 x k − x k − 1 , x ∈ [ x k − 1 , x k ] ( k ≠ 0 ) x − x k + 1 x k − x k + 1 , x ∈ [ x k , x k + 1 ] ( k ≠ n ) 0 , x ∉ [ x k − 1 , x k + 1 ] l_k(x) = \begin{cases} \dfrac{x - x_{k-1}}{x_k - x_{k-1}}, & x \in [x_{k-1}, x_k] \quad (k \neq 0) \\ \dfrac{x - x_{k+1}}{x_k - x_{k+1}}, & x \in [x_k, x_{k+1}] \quad (k \neq n) \\ 0, & x \notin [x_{k-1}, x_{k+1}] \end{cases} lk​(x)=⎩ ⎨ ⎧​xk​−xk−1​x−xk−1​​,xk​−xk+1​x−xk+1​​,0,​x∈[xk−1​,xk​](k=0)x∈[xk​,xk+1​](k=n)x∈/[xk−1​,xk+1​]​

区间分段表达式
左半区间 [ x k − 1 , x k ] [x_{k-1}, x_k] [xk−1​,xk​]:
I h ( x ) = x − x k − 1 x k − x k − 1 f k + x − x k x k − 1 − x k f k − 1 I_h(x) = \dfrac{x - x_{k-1}}{x_k - x_{k-1}} f_k + \dfrac{x - x_k}{x_{k-1} - x_k} f_{k-1} Ih​(x)=xk​−xk−1​x−xk−1​​fk​+xk−1​−xk​x−xk​​fk−1​

右半区间 [ x k , x k + 1 ] [x_k, x_{k+1}] [xk​,xk+1​]:
I h ( x ) = x − x k + 1 x k − x k + 1 f k + x − x k x k + 1 − x k f k + 1 I_h(x) = \dfrac{x - x_{k+1}}{x_k - x_{k+1}} f_k + \dfrac{x - x_k}{x_{k+1} - x_k} f_{k+1} Ih​(x)=xk​−xk+1​x−xk+1​​fk​+xk+1​−xk​x−xk​​fk+1​

收敛性与性质

  1. 一致收敛性:当 h → 0 h \to 0 h→0 时, I h ( x ) I_h(x) Ih​(x) 在 [ a , b ] [a, b] [a,b] 上一致收敛到 f ( x ) f(x) f(x)。

  2. 光滑性缺失:分段线性插值函数仅连续( C 0 C^0 C0),但不可导(失去原函数的光滑性)。

插值误差
max ⁡ x k ≤ x ≤ x k + 1 ∣ f ( x ) − I h ( x ) ∣ ≤ M 2 2 max ⁡ x k ≤ x ≤ x k + 1 ∣ ( x − x k ) ( x − x k + 1 ) ∣ \max_{x_k \leq x \leq x_{k+1}} |f(x) - I_h(x)| \leq \frac{M_2}{2} \max_{x_k \leq x \leq x_{k+1}} |(x - x_k)(x - x_{k+1})| xk​≤x≤xk+1​max​∣f(x)−Ih​(x)∣≤2M2​​xk​≤x≤xk+1​max​∣(x−xk​)(x−xk+1​)∣
或
max ⁡ a ≤ x ≤ b ∣ f ( x ) − I h ( x ) ∣ ≤ M 2 8 h 2 \max_{a \leq x \leq b} |f(x) - I_h(x)| \leq \frac{M_2}{8} h^2 a≤x≤bmax​∣f(x)−Ih​(x)∣≤8M2​​h2
其中
M 2 = max ⁡ a ≤ x ≤ b ∣ f ′ ′ ( x ) ∣ M_2 = \max_{a \leq x \leq b} |f''(x)| M2​=a≤x≤bmax​∣f′′(x)∣

分段三次 Hermite 插值

问题描述
在节点 x 0 < x 1 < ⋯ < x n x_0 < x_1 < \cdots < x_n x0​<x1​<⋯<xn​ 上已知函数值 f k f_k fk​ 和导数值 f k ′ = m k f'_k = m_k fk′​=mk​,构造分段插值多项式函数 I h ( x ) I_h(x) Ih​(x) 满足:

  1. 光滑性: I h ∈ C 1 [ a , b ] I_h \in C^1[a, b] Ih​∈C1[a,b]
  2. 插值条件:
    I h ( x k ) = f k , I h ′ ( x k ) = f k ′ ( k = 0 , 1 , … , n ) I_h(x_k) = f_k, \quad I'_h(x_k) = f'_k \quad (k = 0, 1, \ldots, n) Ih​(xk​)=fk​,Ih′​(xk​)=fk′​(k=0,1,…,n)
  3. 分段三次多项式:在每段区间 [ x k , x k + 1 ] [x_k, x_{k+1}] [xk​,xk+1​] 上, I h ( x ) I_h(x) Ih​(x) 为三次多项式。

全局表达式
插值函数可表示为:
I h ( x ) = ∑ k = 0 n [ f ( x k ) α k ( x ) + f ′ ( x k ) β k ( x ) ] I_h(x) = \sum_{k=0}^n \left[ f(x_k) \alpha_k(x) + f'(x_k) \beta_k(x) \right] Ih​(x)=k=0∑n​[f(xk​)αk​(x)+f′(xk​)βk​(x)]

区间局部表达式
在区间 [ x k , x k + 1 ] [x_k, x_{k+1}] [xk​,xk+1​] 上的具体形式为:
I h ( x ) = ( x − x k + 1 x k − x k + 1 ) 2 ( 1 + 2 x − x k x k + 1 − x k ) f k ( x − x k x k + 1 − x k ) 2 ( 1 + 2 x − x k + 1 x k − x k + 1 ) f k + 1 ( x − x k + 1 x k − x k + 1 ) 2 ( x − x k ) f k ′ ( x − x k x k + 1 − x k ) 2 ( x − x k + 1 ) f k + 1 ′ \begin{aligned} I_h(x) = &\left( \dfrac{x - x_{k+1}}{x_k - x_{k+1}} \right)^2 \left( 1 + 2 \dfrac{x - x_k}{x_{k+1} - x_k} \right) f_k \\ &\left( \dfrac{x - x_k}{x_{k+1} - x_k} \right)^2 \left( 1 + 2 \dfrac{x - x_{k+1}}{x_k - x_{k+1}} \right) f_{k+1} \\ &\left( \dfrac{x - x_{k+1}}{x_k - x_{k+1}} \right)^2 (x - x_k) f'_k \\ &\left( \dfrac{x - x_k}{x_{k+1} - x_k} \right)^2 (x - x_{k+1}) f'_{k+1} \end{aligned} Ih​(x)=​(xk​−xk+1​x−xk+1​​)2(1+2xk+1​−xk​x−xk​​)fk​(xk+1​−xk​x−xk​​)2(1+2xk​−xk+1​x−xk+1​​)fk+1​(xk​−xk+1​x−xk+1​​)2(x−xk​)fk′​(xk+1​−xk​x−xk​​)2(x−xk+1​)fk+1′​​

(基函数 α k ( x ) \alpha_k(x) αk​(x) 和 β k ( x ) \beta_k(x) βk​(x) 的定义已在前面详细给出,此处可省略重复内容以保持简洁)

α k ( x ) \alpha_k(x) αk​(x) 的分段表达式
α k ( x ) = { ( x − x k − 1 x k − x k − 1 ) 2 ( 1 + 2 x − x k x k − 1 − x k ) , x ∈ [ x k − 1 , x k ] ( k ≠ 0 ) ( x − x k + 1 x k − x k + 1 ) 2 ( 1 + 2 x − x k x k + 1 − x k ) , x ∈ [ x k , x k + 1 ] ( k ≠ n ) 0 , 其他区间 \alpha_k(x) = \begin{cases} \left( \dfrac{x - x_{k-1}}{x_k - x_{k-1}} \right)^2 \left( 1 + 2 \dfrac{x - x_k}{x_{k-1} - x_k} \right), & x \in [x_{k-1}, x_k] \quad (k \neq 0) \\ \left( \dfrac{x - x_{k+1}}{x_k - x_{k+1}} \right)^2 \left( 1 + 2 \dfrac{x - x_k}{x_{k+1} - x_k} \right), & x \in [x_k, x_{k+1}] \quad (k \neq n) \\ 0, & \text{其他区间} \end{cases} αk​(x)=⎩ ⎨ ⎧​(xk​−xk−1​x−xk−1​​)2(1+2xk−1​−xk​x−xk​​),(xk​−xk+1​x−xk+1​​)2(1+2xk+1​−xk​x−xk​​),0,​x∈[xk−1​,xk​](k=0)x∈[xk​,xk+1​](k=n)其他区间​

β k ( x ) \beta_k(x) βk​(x) 的分段表达式
β k ( x ) = { ( x − x k − 1 x k − x k − 1 ) 2 ( x − x k ) , x ∈ [ x k − 1 , x k ] ( k ≠ 0 ) ( x − x k + 1 x k − x k + 1 ) 2 ( x − x k ) , x ∈ [ x k , x k + 1 ] ( k ≠ n ) 0 , 其他区间 \beta_k(x) = \begin{cases} \left( \dfrac{x - x_{k-1}}{x_k - x_{k-1}} \right)^2 (x - x_k), & x \in [x_{k-1}, x_k] \quad (k \neq 0) \\ \left( \dfrac{x - x_{k+1}}{x_k - x_{k+1}} \right)^2 (x - x_k), & x \in [x_k, x_{k+1}] \quad (k \neq n) \\ 0, & \text{其他区间} \end{cases} βk​(x)=⎩ ⎨ ⎧​(xk​−xk−1​x−xk−1​​)2(x−xk​),(xk​−xk+1​x−xk+1​​)2(x−xk​),0,​x∈[xk−1​,xk​](k=0)x∈[xk​,xk+1​](k=n)其他区间​

样条插值

样条插值的概念

对于给定节点 a = x 0 < x 1 < ⋯ < x n = b a = x_0 < x_1 < \cdots < x_n = b a=x0​<x1​<⋯<xn​=b,若存在函数 s ( x ) s(x) s(x) 满足:

  1. 在每个小区间 [ x j , x j + 1 ] [x_j, x_{j+1}] [xj​,xj+1​] 上是一个次数不超过3的多项式;
  2. 在每一个内节点上具有直到二阶的连续导数,
    则称 s ( x ) s(x) s(x) 是节点 x 0 , x 1 , ⋯   , x n x_0, x_1, \cdots, x_n x0​,x1​,⋯,xn​ 上的三次样条函数。

若在节点上给定函数值 f ( x j ) = y j   ( j = 0 , ⋯   , n ) f(x_j) = y_j \ (j = 0, \cdots, n) f(xj​)=yj​ (j=0,⋯,n),并满足
3. s ( x j ) = y j ,   j = 0 , ⋯   , n s(x_j) = y_j, \ j = 0, \cdots, n s(xj​)=yj​, j=0,⋯,n
则称 s ( x ) s(x) s(x) 是三次样条插值函数。

三次样条插值函数 s ( x ) s(x) s(x) 的确定:

s ( x ) = { s 1 ( x ) , x 0 ≤ x ≤ x 1 , ⋮ s n ( x ) , x n − 1 ≤ x ≤ x n . s(x) = \begin{cases} s_1(x), & x_0 \leq x \leq x_1, \\ \vdots \\ s_n(x), & x_{n-1} \leq x \leq x_n. \end{cases} s(x)=⎩ ⎨ ⎧​s1​(x),⋮sn​(x),​x0​≤x≤x1​,xn−1​≤x≤xn​.​
在每个 [ x j , x j + 1 ] [x_j, x_{j+1}] [xj​,xj+1​] 上要确定4个待定系数,共 4 n 4n 4n 个参数。因二阶导数连续,故在内节点 x j x_j xj​ 上满足连续性条件:
s ( x j − 0 ) = s ( x j + 0 ) , s ′ ( x j − 0 ) = s ′ ( x j + 0 ) , s ′ ′ ( x j − 0 ) = s ′ ′ ( x j + 0 ) , ( j = 1 , ⋯   , n − 1 ) \begin{gathered} s(x_j - 0) = s(x_j + 0), \quad s'(x_j - 0) = s'(x_j + 0), \\ s''(x_j - 0) = s''(x_j + 0), \quad (j = 1, \cdots, n-1) \end{gathered} s(xj​−0)=s(xj​+0),s′(xj​−0)=s′(xj​+0),s′′(xj​−0)=s′′(xj​+0),(j=1,⋯,n−1)​
再加上插值条件,共 4 n − 2 4n - 2 4n−2 个条件。还需2个条件,通常在两个端点加上边界条件。

常见三种边界条件:

  1. 第一种边界条件: s ′ ( x 0 ) = y 0 ′ , s ′ ( x n ) = y n ′ s'(x_0) = y_0', \quad s'(x_n) = y_n' s′(x0​)=y0′​,s′(xn​)=yn′​。
  2. 第二种边界条件: s ′ ′ ( x 0 ) = y 0 ′ ′ , s ′ ′ ( x n ) = y n ′ ′ s''(x_0) = y_0'', \quad s''(x_n) = y_n'' s′′(x0​)=y0′′​,s′′(xn​)=yn′′​。
    特别地,自然边界条件: s ′ ′ ( x 0 ) = 0 , s ′ ′ ( x n ) = 0 s''(x_0) = 0, \quad s''(x_n) = 0 s′′(x0​)=0,s′′(xn​)=0。
  3. 第三种边界条件(周期边界条件):
    s ′ ( x 0 + 0 ) = s ′ ( x n − 0 ) , s ′ ′ ( x 0 + 0 ) = s ′ ′ ( x n − 0 ) . s'(x_0 + 0) = s'(x_n - 0), \quad s''(x_0 + 0) = s''(x_n - 0). s′(x0​+0)=s′(xn​−0),s′′(x0​+0)=s′′(xn​−0).
    注意:因插值条件 y 0 = y n y_0 = y_n y0​=yn​,故 s ( x 0 + 0 ) = s ( x n − 0 ) s(x_0 + 0) = s(x_n - 0) s(x0​+0)=s(xn​−0) 已经成立。

三次样条插值函数的建立

求三次样条插值函数常用三弯矩法和三转角法。

三转角法:假定 s ′ ( x j ) = m j   ( j = 0 , ⋯   , n ) s'(x_j) = m_j \ (j = 0, \cdots, n) s′(xj​)=mj​ (j=0,⋯,n),根据分段三次埃尔米特插值多项式,
s ( x ) = ∑ j = 0 n [ f j α j ( x ) + m j β j ( x ) ] s(x) = \sum_{j=0}^n \left[ f_j \alpha_j(x) + m_j \beta_j(x) \right] s(x)=j=0∑n​[fj​αj​(x)+mj​βj​(x)]
由插值条件、连续性条件和边界条件,可得关于 m j m_j mj​ 的三对角方程组,求出 m j m_j mj​,得到三次样条插值函数。

三弯矩法:令 s ′ ′ ( x j ) = M j , j = 0 , ⋯   , n , h j = x j + 1 − x j s''(x_j) = M_j, \quad j = 0, \cdots, n, \quad h_j = x_{j+1} - x_j s′′(xj​)=Mj​,j=0,⋯,n,hj​=xj+1​−xj​
则 s ′ ′ ( x ) = x j + 1 − x h j M j + x − x j h j M j + 1 , x ∈ [ x j , x j + 1 ] s''(x) = \frac{x_{j+1} - x}{h_j} M_j + \frac{x - x_j}{h_j} M_{j+1}, \quad x \in [x_j, x_{j+1}] s′′(x)=hj​xj+1​−x​Mj​+hj​x−xj​​Mj+1​,x∈[xj​,xj+1​]
s ′ ( x ) = − ( x j + 1 − x ) 2 2 h j M j + ( x − x j ) 2 2 h j M j + 1 + c 1 , s ( x ) = ( x j + 1 − x ) 3 6 h j M j + ( x − x j ) 3 6 h j M j + 1 + c 1 x + c 2 , s ( x j ) = 1 6 h j 2 M j + c 1 x j + c 2 = y j , s ( x j + 1 ) = 1 6 h j 2 M j + 1 + c 1 x j + 1 + c 2 = y j + 1 , c 1 = y j + 1 − y j h j − 1 6 h j ( M j + 1 − M j ) , c 2 = y j x j + 1 − y j + 1 x j h j − 1 6 h j ( x j + 1 M j − x j M j + 1 ) . \begin{aligned} s'(x) &= -\frac{(x_{j+1} - x)^2}{2 h_j} M_j + \frac{(x - x_j)^2}{2 h_j} M_{j+1} + c_1, \\ s(x) &= \frac{(x_{j+1} - x)^3}{6 h_j} M_j + \frac{(x - x_j)^3}{6 h_j} M_{j+1} + c_1 x + c_2, \\ s(x_j) &= \frac{1}{6} h_j^2 M_j + c_1 x_j + c_2 = y_j, \\ s(x_{j+1}) &= \frac{1}{6} h_j^2 M_{j+1} + c_1 x_{j+1} + c_2 = y_{j+1}, \\ c_1 &= \frac{y_{j+1} - y_j}{h_j} - \frac{1}{6} h_j (M_{j+1} - M_j), \\ c_2 &= \frac{y_j x_{j+1} - y_{j+1} x_j}{h_j} - \frac{1}{6} h_j (x_{j+1} M_j - x_j M_{j+1}). \end{aligned} s′(x)s(x)s(xj​)s(xj+1​)c1​c2​​=−2hj​(xj+1​−x)2​Mj​+2hj​(x−xj​)2​Mj+1​+c1​,=6hj​(xj+1​−x)3​Mj​+6hj​(x−xj​)3​Mj+1​+c1​x+c2​,=61​hj2​Mj​+c1​xj​+c2​=yj​,=61​hj2​Mj+1​+c1​xj+1​+c2​=yj+1​,=hj​yj+1​−yj​​−61​hj​(Mj+1​−Mj​),=hj​yj​xj+1​−yj+1​xj​​−61​hj​(xj+1​Mj​−xj​Mj+1​).​

s ( x ) = ( x j + 1 − x ) 3 6 h j M j + ( x − x j ) 3 6 h j M j + 1 + ( y j − M j h j 2 6 ) x j + 1 − x h j + ( y j + 1 − M j + 1 h j 2 6 ) x − x j h j s(x) = \frac{(x_{j+1} - x)^3}{6 h_j} M_j + \frac{(x - x_j)^3}{6 h_j} M_{j+1} + \left( y_j - \frac{M_j h_j^2}{6} \right) \frac{x_{j+1} - x}{h_j} + \left( y_{j+1} - \frac{M_{j+1} h_j^2}{6} \right) \frac{x - x_j}{h_j} s(x)=6hj​(xj+1​−x)3​Mj​+6hj​(x−xj​)3​Mj+1​+(yj​−6Mj​hj2​​)hj​xj+1​−x​+(yj+1​−6Mj+1​hj2​​)hj​x−xj​​

s ′ ( x ) = − ( x j + 1 − x ) 2 2 h j M j + ( x − x j ) 2 2 h j M j + 1 + y j + 1 − y j h j − M j + 1 − M j 6 h j . s'(x) = -\frac{(x_{j+1} - x)^2}{2 h_j} M_j + \frac{(x - x_j)^2}{2 h_j} M_{j+1} + \frac{y_{j+1} - y_j}{h_j} - \frac{M_{j+1} - M_j}{6} h_j. s′(x)=−2hj​(xj+1​−x)2​Mj​+2hj​(x−xj​)2​Mj+1​+hj​yj+1​−yj​​−6Mj+1​−Mj​​hj​.

为了求 M 0 , ⋯   , M n M_0, \cdots, M_n M0​,⋯,Mn​,要用导数连续条件: s ′ ( x j + 0 ) = s ′ ( x j − 0 ) s'(x_j + 0) = s'(x_j - 0) s′(xj​+0)=s′(xj​−0)。
s ′ ( x j + 0 ) = − h j 3 M j − h j 6 M j + 1 + y j + 1 − y j h j , s ′ ( x j + 1 − 0 ) = h j 6 M j + h j 3 M j + 1 + y j + 1 − y j h j , s ′ ( x j − 0 ) = h j − 1 6 M j − 1 + h j − 1 3 M j + y j − y j − 1 h j − 1 . h j − 1 6 M j − 1 + h j − 1 + h j 3 M j + h j 6 M j + 1 = y j − y j − 1 h j − 1 − y j + 1 − y j h j , j = 1 , ⋯   , n − 1 , \begin{align*} s'(x_j + 0) &= -\frac{h_j}{3} M_j - \frac{h_j}{6} M_{j+1} + \frac{y_{j+1} - y_j}{h_j}, \\ s'(x_{j+1} - 0) &= \frac{h_j}{6} M_j + \frac{h_j}{3} M_{j+1} + \frac{y_{j+1} - y_j}{h_j}, \\ s'(x_j - 0) &= \frac{h_{j-1}}{6} M_{j-1} + \frac{h_{j-1}}{3} M_j + \frac{y_j - y_{j-1}}{h_{j-1}}. \\ \frac{h_{j-1}}{6} M_{j-1} + \frac{h_{j-1} + h_j}{3} M_j + \frac{h_j}{6} M_{j+1} &= \frac{y_j - y_{j-1}}{h_{j-1}} - \frac{y_{j+1} - y_j}{h_j}, \quad j = 1, \cdots, n-1, \end{align*} s′(xj​+0)s′(xj+1​−0)s′(xj​−0)6hj−1​​Mj−1​+3hj−1​+hj​​Mj​+6hj​​Mj+1​​=−3hj​​Mj​−6hj​​Mj+1​+hj​yj+1​−yj​​,=6hj​​Mj​+3hj​​Mj+1​+hj​yj+1​−yj​​,=6hj−1​​Mj−1​+3hj−1​​Mj​+hj−1​yj​−yj−1​​.=hj−1​yj​−yj−1​​−hj​yj+1​−yj​​,j=1,⋯,n−1,​

μ j M j − 1 + 2 M j + λ j M j + 1 = d j , j = 1 , ⋯   , n − 1 , \mu_j M_{j-1} + 2 M_j + \lambda_j M_{j+1} = d_j, \quad j = 1, \cdots, n-1, μj​Mj−1​+2Mj​+λj​Mj+1​=dj​,j=1,⋯,n−1,
其中 d j = 6 f [ x j − 1 , x j , x j + 1 ] d_j = 6 f[x_{j-1}, x_j, x_{j+1}] dj​=6f[xj−1​,xj​,xj+1​],
λ j = h j h j − 1 + h j , μ j = h j − 1 h j − 1 + h j . \lambda_j = \frac{h_j}{h_{j-1} + h_j}, \quad \mu_j = \frac{h_{j-1}}{h_{j-1} + h_j}. λj​=hj−1​+hj​hj​​,μj​=hj−1​+hj​hj−1​​.

在第一边界条件下:
[ 2 1 μ 1 2 λ 1 ⋱ ⋱ ⋱ μ n − 1 2 λ n − 1 1 2 ] [ M 0 M 1 ⋮ M n − 1 M n ] = \begin{bmatrix} 2 & 1 & & & \\ \mu_1 & 2 & \lambda_1 & & \\ & \ddots & \ddots & \ddots & \\ & & \mu_{n-1} & 2 & \lambda_{n-1} \\ & & & 1 & 2 \end{bmatrix} \begin{bmatrix} M_0 \\ M_1 \\ \vdots \\ M_{n-1} \\ M_n \end{bmatrix} = ​2μ1​​12⋱​λ1​⋱μn−1​​⋱21​λn−1​2​ ​ ​M0​M1​⋮Mn−1​Mn​​ ​=
$ [ d 0 d 1 ⋮ d n − 1 d n ] \begin{bmatrix} d_0 \\ d_1 \\ \vdots \\ d_{n-1} \\ d_n \end{bmatrix} ​d0​d1​⋮dn−1​dn​​ ​

λ 0 = 1 , μ n = 1 , d 0 = 6 h 0 ( f [ x 0 , x 1 ] − f 0 ′ ) , d j = 6 f [ x j , x j + 1 ] − f [ x j − 1 , x j ] h j − 1 + h j = 6 f [ x j − 1 , x j , x j + 1 ] , j = 1 , 2 , … , n − 1 , d n = 6 h n − 1 ( f n ′ − f [ x n − 1 , x n ] ) . \lambda_0 = 1, \quad \mu_n = 1, \\ d_0 = \frac{6}{h_0} \left( f[x_0, x_1] - f'_0 \right), \\ d_j = 6 \frac{f[x_j, x_{j+1}] - f[x_{j-1}, x_j]}{h_{j-1} + h_j} = 6 f[x_{j-1}, x_j, x_{j+1}], \quad j = 1, 2, \dots, n-1, \\ d_n = \frac{6}{h_{n-1}} \left( f'_n - f[x_{n-1}, x_n] \right). λ0​=1,μn​=1,d0​=h0​6​(f[x0​,x1​]−f0′​),dj​=6hj−1​+hj​f[xj​,xj+1​]−f[xj−1​,xj​]​=6f[xj−1​,xj​,xj+1​],j=1,2,…,n−1,dn​=hn−1​6​(fn′​−f[xn−1​,xn​]).
第二边界条件矩阵方程
[ 2 λ 1 μ 2 2 λ 2 ⋱ ⋱ ⋱ μ n − 1 2 ] \begin{bmatrix} 2 & \lambda_1 & & \\ \mu_2 & 2 & \lambda_2 & \\ & \ddots & \ddots & \ddots \\ & & \mu_{n-1} & 2 \end{bmatrix} ​2μ2​​λ1​2⋱​λ2​⋱μn−1​​⋱2​ ​
[ M 1 M 2 ⋮ M n − 1 ] = \begin{bmatrix} M_1 \\ M_2 \\ \vdots \\ M_{n-1} \end{bmatrix} = ​M1​M2​⋮Mn−1​​ ​=

[ d 1 − μ 1 f 0 ′ ′ d 2 ⋮ d n − 1 − λ n − 1 f n ′ ′ ] \begin{bmatrix} d_1 - \mu_1 f''_0 \\ d_2 \\ \vdots \\ d_{n-1} - \lambda_{n-1} f''_n \end{bmatrix} ​d1​−μ1​f0′′​d2​⋮dn−1​−λn−1​fn′′​​ ​
边界条件约束:
{ M 0 = f 0 ′ ′ , M n = f n ′ ′ . \begin{cases} M_0 = f''_0, \\ M_n = f''_n. \end{cases} {M0​=f0′′​,Mn​=fn′′​.​

第三边界条件(周期边界条件)矩阵方程
[ 2 λ 1 μ 1 μ 2 2 λ 2 ⋱ ⋱ ⋱ μ n − 1 2 λ n − 1 λ n μ n 2 ] [ M 1 M 2 ⋮ M n − 1 M n ] = \begin{bmatrix} 2 & \lambda_1 & & & \mu_1 \\ \mu_2 & 2 & \lambda_2 & & \\ & \ddots & \ddots & \ddots & \\ & & \mu_{n-1} & 2 & \lambda_{n-1} \\ \lambda_n & & & \mu_n & 2 \end{bmatrix} \begin{bmatrix} M_1 \\ M_2 \\ \vdots \\ M_{n-1} \\ M_n \end{bmatrix} = ​2μ2​λn​​λ1​2⋱​λ2​⋱μn−1​​⋱2μn​​μ1​λn−1​2​ ​ ​M1​M2​⋮Mn−1​Mn​​ ​=

[ d 1 d 2 ⋮ d n − 1 d n ] \begin{bmatrix} d_1 \\ d_2 \\ \vdots \\ d_{n-1} \\ d_n \end{bmatrix} ​d1​d2​⋮dn−1​dn​​ ​

特殊约束条件
{ x 0 = x n ( 周期条件 ) , M 0 = M n ( 弯矩周期约束 ) , μ n M n − 1 + 2 M n + λ n M 1 = d n ( 闭环方程 ) . \begin{cases} x_0 = x_n \quad (\text{周期条件}), \\ M_0 = M_n \quad (\text{弯矩周期约束}), \\ \mu_n M_{n-1} + 2M_n + \lambda_n M_1 = d_n \quad (\text{闭环方程}). \end{cases} ⎩ ⎨ ⎧​x0​=xn​(周期条件),M0​=Mn​(弯矩周期约束),μn​Mn−1​+2Mn​+λn​M1​=dn​(闭环方程).​

参数定义
μ n = h n − 1 h n − 1 + h 0 ( 末节点弯矩传递系数 ) , λ n = h 0 h n − 1 + h 0 ( 首节点弯矩传递系数 ) , d n = 6 f [ x n − 1 , x n , x 1 ] ( 三阶差商计算 ) . \begin{aligned} \mu_n &= \frac{h_{n-1}}{h_{n-1} + h_0} \quad (\text{末节点弯矩传递系数}), \\ \lambda_n &= \frac{h_0}{h_{n-1} + h_0} \quad (\text{首节点弯矩传递系数}), \\ d_n &= 6f[x_{n-1}, x_n, x_1] \quad (\text{三阶差商计算}). \end{aligned} μn​λn​dn​​=hn−1​+h0​hn−1​​(末节点弯矩传递系数),=hn−1​+h0​h0​​(首节点弯矩传递系数),=6f[xn−1​,xn​,x1​](三阶差商计算).​

误差界与收敛性

设 f ( x ) ∈ C 4 [ a , b ] f(x) \in C^4[a,b] f(x)∈C4[a,b], S ( x ) S(x) S(x) 满足第一或第二边界条件,
令 h = max ⁡ 0 ≤ i ≤ n − 1 h i h = \max\limits_{0 \leq i \leq n-1} h_i h=0≤i≤n−1max​hi​,其中 h i = x i + 1 − x i h_i = x_{i+1} - x_i hi​=xi+1​−xi​,则有估计式:
max ⁡ a ≤ x ≤ b ∣ f ( k ) ( x ) − s ( k ) ( x ) ∣ ≤ C k ( max ⁡ a ≤ x ≤ b ∣ f ( 4 ) ( x ) ∣ ) h 4 − k \max_{a \leq x \leq b} \left| f^{(k)}(x) - s^{(k)}(x) \right| \leq C_k \left( \max_{a \leq x \leq b} \left| f^{(4)}(x) \right| \right) h^{4-k} a≤x≤bmax​ ​f(k)(x)−s(k)(x) ​≤Ck​(a≤x≤bmax​ ​f(4)(x) ​)h4−k
其中常数项系数为:
{ C 0 = 5 384 , C 1 = 1 24 , C 2 = 3 8 ( k = 0 , 1 , 2 ) . \begin{cases} C_0 = \dfrac{5}{384}, \\ C_1 = \dfrac{1}{24}, \\ C_2 = \dfrac{3}{8} \end{cases} \quad (k = 0, 1, 2). ⎩ ⎨ ⎧​C0​=3845​,C1​=241​,C2​=83​​(k=0,1,2).


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