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Jun 13, 2026
miniyuan

非线性方程及非线性方程组的解法


题 8.1

设方程 x3−x2−1=0x^3-x^2-1=0x3−x2−1=0 在 x0=1.5x_0=1.5x0​=1.5 附近的根为 x∗x^*x∗。

先由 f(x)=x3−x2−1f(x)=x^3-x^2-1f(x)=x3−x2−1 有:

f(1.4)<0,f(1.5)>0f(1.4)<0,\quad f(1.5)>0f(1.4)<0,f(1.5)>0

故 x∗∈(1.4,1.5)x^*\in(1.4,1.5)x∗∈(1.4,1.5)。

  • 对于 φ1(x)=1+1x2\displaystyle \varphi_1(x)=1+\frac{1}{x^2}φ1​(x)=1+x21​,则:

    ∣φ1′(x∗)∣=2(x∗)3<21.43<1|\varphi_1'(x^*)| =\frac{2}{(x^*)^3} \lt \frac{2}{1.4^3} \lt 1∣φ1′​(x∗)∣=(x∗)32​<1.432​<1

    故在 x0=1.5x_0=1.5x0​=1.5 邻近局部收敛。

  • 对于 φ2(x)=(x−1)−1/2\displaystyle \varphi_2(x)=(x-1)^{-1/2}φ2​(x)=(x−1)−1/2,则:

    ∣φ2′(x∗)∣=12(x∗−1)3/2>12(1.5−1)3/2>1|\varphi_2'(x^*)| =\frac{1}{2(x^*-1)^{3/2}} \gt \frac{1}{2(1.5-1)^{3/2}} \gt 1∣φ2′​(x∗)∣=2(x∗−1)3/21​>2(1.5−1)3/21​>1

    故在 x0=1.5x_0=1.5x0​=1.5 邻近局部发散。

  • 对于 φ3(x)=(1+x2)1/3\displaystyle \varphi_3(x)=(1+x^2)^{1/3}φ3​(x)=(1+x2)1/3,则:

    ∣φ3′(x∗)∣=2x∗3[1+(x∗)2]2/3|\varphi_3'(x^*)| =\frac{2x^*}{3[1+(x^*)^2]^{2/3}}∣φ3′​(x∗)∣=3[1+(x∗)2]2/32x∗​

    注意到在不动点处有 1+(x∗)2=(x∗)31+(x^*)^2=(x^*)^31+(x∗)2=(x∗)3,因此

    ∣φ3′(x∗)∣=2x∗3(x∗)2=23x∗<23×1.4<1|\varphi_3'(x^*)| =\frac{2x^*}{3(x^*)^2} =\frac{2}{3x^*} \lt \frac{2}{3\times 1.4} \lt 1∣φ3′​(x∗)∣=3(x∗)22x∗​=3x∗2​<3×1.42​<1

    故在 x0=1.5x_0=1.5x0​=1.5 邻近局部收敛。

题 8.2

记:

F(x,y)=(f1(x,y)f2(x,y))=(x2+y2−5(x+1)y−3x−1)F(x,y)=\begin{pmatrix} f_1(x,y)\\ f_2(x,y)\end{pmatrix} =\begin{pmatrix} x^2+y^2-5\\ (x+1)y-3x-1\end{pmatrix}F(x,y)=(f1​(x,y)f2​(x,y)​)=(x2+y2−5(x+1)y−3x−1​)

Jacobi 矩阵为:

J(x,y)=(2x2yy−3x+1)J(x,y)=\begin{pmatrix}2x&2y\\ y-3&x+1\end{pmatrix}J(x,y)=(2xy−3​2yx+1​)

行列式:

det⁡J(x,y)=2(x2+x−y2+3y)\det J(x,y)=2(x^2+x-y^2+3y)detJ(x,y)=2(x2+x−y2+3y)

从而逆矩阵为:

J−1(x,y)=12(x2+x−y2+3y)(x+1−2y3−y2x)J^{-1}(x,y)=\frac{1}{2(x^2+x-y^2+3y)} \begin{pmatrix} x+1&-2y \\ 3-y&2x \end{pmatrix}J−1(x,y)=2(x2+x−y2+3y)1​(x+13−y​−2y2x​)

Newton 迭代式中的增量:

(δxδy)=−J−1(xk,yk) F(xk,yk)\begin{pmatrix}\delta x\\ \delta y\end{pmatrix} =-J^{-1}(x_k,y_k)\,F(x_k,y_k)(δxδy​)=−J−1(xk​,yk​)F(xk​,yk​)

代入 (x0,y0)=(1,1)(x_0,y_0)=(1,1)(x0​,y0​)=(1,1) 得:

(δxδy)=−18(2−222)(−3−2)=(1/45/4)\begin{pmatrix}\delta x\\ \delta y\end{pmatrix} =-\frac{1}{8}\begin{pmatrix}2&-2\\ 2&2\end{pmatrix}\begin{pmatrix}-3\\ -2\end{pmatrix} =\begin{pmatrix}1/4\\ 5/4\end{pmatrix}(δxδy​)=−81​(22​−22​)(−3−2​)=(1/45/4​)

从而:

(x1,y1)=(54,94)(x_1, y_1)=(\frac{5}{4}, \frac{9}{4})(x1​,y1​)=(45​,49​)

继续代入得:

(δxδy)=−19(9/4−9/23/45/2)(13/85/16)=(−1/4−2/9)\begin{pmatrix}\delta x\\ \delta y\end{pmatrix} =-\frac{1}{9} \begin{pmatrix} 9/4& -9/2\\ 3/4& 5/2 \end{pmatrix} \begin{pmatrix} 13/8\\ 5/16 \end{pmatrix} =\begin{pmatrix} -1/4\\ -2/9 \end{pmatrix}(δxδy​)=−91​(9/43/4​−9/25/2​)(13/85/16​)=(−1/4−2/9​)

从而:

(x2,y2)=(1,7336)≈(1,2.0278)(x_2, y_2)=(1, \frac{73}{36}) \approx (1, 2.0278)(x2​,y2​)=(1,3673​)≈(1,2.0278)

题 8.3

假设 x∗x^{*}x∗ 为 f(x)=0f(x)=0f(x)=0 的单根,记 e=x−x∗e=x-x^{*}e=x−x∗。将 fff 在 x∗x^{*}x∗ 处 Taylor 展开可得:

f(x)=ae+b2e2+c6e3+O(e4)f(x) = ae+\frac{b}{2}e^{2}+\frac{c}{6}e^{3}+O(e^{4})f(x)=ae+2b​e2+6c​e3+O(e4) f′(x)=a+be+c2e2+O(e3)f'(x) = a+be+\frac{c}{2}e^{2}+O(e^{3})f′(x)=a+be+2c​e2+O(e3) f′′(x)=b+ce+O(e2)f''(x) = b+ce+O(e^{2})f′′(x)=b+ce+O(e2)

其中 a=f′(x∗),  b=f′′(x∗),  c=f′′′(x∗)a=f'(x^{*}),\; b=f''(x^{*}),\; c=f'''(x^{*})a=f′(x∗),b=f′′(x∗),c=f′′′(x∗)。从而:

f(x)f′(x)=ae+b2e2+c6e3+O(e4)a+be+c2e2+O(e3)=[e+b2ae2+c6ae3+O(e4)]⋅[1−bae+(b2a2−c2a)e2+O(e3)]=e−b2ae2+(b22a2−c3a)e3+O(e4)\begin{aligned} \frac{f(x)}{f'(x)} &=\frac{ae+\frac{b}{2}e^{2}+\frac{c}{6}e^{3}+O(e^4)}{a+be+\frac{c}{2}e^{2}+O(e^3)} \\ &=[e+\frac{b}{2a}e^2+\frac{c}{6a}e^3+O(e^4)]\cdot[1-\frac{b}{a}e+(\frac{b^2}{a^2}-\frac{c}{2a})e^2+O(e^3)] \\ &=e-\frac{b}{2a}e^{2}+\left(\frac{b^{2}}{2a^{2}}-\frac{c}{3a}\right)e^{3}+O(e^{4}) \end{aligned}f′(x)f(x)​​=a+be+2c​e2+O(e3)ae+2b​e2+6c​e3+O(e4)​=[e+2ab​e2+6ac​e3+O(e4)]⋅[1−ab​e+(a2b2​−2ac​)e2+O(e3)]=e−2ab​e2+(2a2b2​−3ac​)e3+O(e4)​ [f(x)f′(x)]2=(e−b2ae2+O(e3))2=e2−bae3+O(e4)\left[\frac{f(x)}{f'(x)}\right]^{2}=\left(e-\frac{b}{2a}e^{2}+O(e^{3})\right)^{2} =e^{2}-\frac{b}{a}e^{3}+O(e^{4})[f′(x)f(x)​]2=(e−2ab​e2+O(e3))2=e2−ab​e3+O(e4) f′′(x)2f′(x)=b+ce+O(e2)2(a+be+O(e2))=[b2a+c2ae+O(e2)]⋅[1−bae+O(e2)]=b2a+(c2a−b22a2)e+O(e2)\begin{aligned} \frac{f''(x)}{2f'(x)} &=\frac{b+ce+O(e^2)}{2(a+be+O(e^2))} \\ &=[\frac{b}{2a}+\frac{c}{2a}e+O(e^2)]\cdot[1-\frac{b}{a}e+O(e^2)] \\ &=\frac{b}{2a}+\left(\frac{c}{2a}-\frac{b^2}{2a^2}\right)e+O(e^{2}) \end{aligned}2f′(x)f′′(x)​​=2(a+be+O(e2))b+ce+O(e2)​=[2ab​+2ac​e+O(e2)]⋅[1−ab​e+O(e2)]=2ab​+(2ac​−2a2b2​)e+O(e2)​

故:

g(x)−x∗=e−ff′−f′′2f′(ff′)2=e−[e−b2ae2+(b22a2−c3a)e3]−[b2ae2+(c2a−b2a2)e3]+O(e4)=(b22a2−c6a)e3+O(e4)\begin{aligned} g(x)-x^{*} &=e-\frac{f}{f'}-\frac{f''}{2f'}\left(\frac{f}{f'}\right)^{2}\\[4pt] &=e-\left[e-\frac{b}{2a}e^{2}+\left(\frac{b^{2}}{2a^{2}}-\frac{c}{3a}\right)e^{3}\right] -\left[\frac{b}{2a}e^{2}+\left(\frac{c}{2a}-\frac{b^{2}}{a^{2}}\right)e^{3}\right]+O(e^{4})\\ &=\left(\frac{b^{2}}{2a^{2}}-\frac{c}{6a}\right)e^{3}+O(e^{4}) \end{aligned}g(x)−x∗​=e−f′f​−2f′f′′​(f′f​)2=e−[e−2ab​e2+(2a2b2​−3ac​)e3]−[2ab​e2+(2ac​−a2b2​)e3]+O(e4)=(2a2b2​−6ac​)e3+O(e4)​

也即:

g(x)−x∗=(f′′(x∗)22f′(x∗)2−f′′′(x∗)6f′(x∗))(x−x∗)3+O((x−x∗)4)g(x)-x^{*}=\left(\frac{f''(x^{*})^{2}}{2f'(x^{*})^{2}}-\frac{f'''(x^{*})}{6f'(x^{*})}\right)(x-x^{*})^{3}+O((x-x^{*})^{4})g(x)−x∗=(2f′(x∗)2f′′(x∗)2​−6f′(x∗)f′′′(x∗)​)(x−x∗)3+O((x−x∗)4)

令 ek=xk−x∗e_k=x_k-x^{*}ek​=xk​−x∗,则 ek+1=g(xk)−x∗e_{k+1}=g(x_k)-x^{*}ek+1​=g(xk​)−x∗。从而:

lim⁡x→x∗ek+1ek3=lim⁡x→x∗g(xk)−x∗(xk−x∗)3=f′′(x∗)22f′(x∗)2−f′′′(x∗)6f′(x∗)\lim_{x\to x^{*}}\frac{e_{k+1}}{e_k^{3}} =\lim_{x\to x^{*}}\frac{g(x_k)-x^{*}}{(x_k-x^{*})^{3}} =\frac{f''(x^{*})^{2}}{2f'(x^{*})^{2}}-\frac{f'''(x^{*})}{6f'(x^{*})}x→x∗lim​ek3​ek+1​​=x→x∗lim​(xk​−x∗)3g(xk​)−x∗​=2f′(x∗)2f′′(x∗)2​−6f′(x∗)f′′′(x∗)​

在一般情形下该极限常数非零,故根据收敛阶定义,该方法为 3 阶收敛。

目录
  • 题 8.1
  • 题 8.2
  • 题 8.3
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