目录
- 0 专栏介绍
- 1 什么是样条?
- 2 三次样条曲线原理
- 2.1 曲线插值
- 2.2 边界条件
- 2.3 系数反解
- 3 算法仿真
- 3.1 ROS C++仿真
- 3.2 Python仿真
- 3.3 Matlab仿真
0 专栏介绍
🔥附C++/Python/Matlab全套代码🔥课程设计、毕业设计、创新竞赛必备!详细介绍全局规划(图搜索、采样法、智能算法等);局部规划(DWA、APF等);曲线优化(贝塞尔曲线、B样条曲线等)。
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1 什么是样条?
样条(Spline)早期来源于工程制图,为了将一些固定点连成一条光滑曲线,采用具有弹性的木条固定在这些点上,通过样条作出的曲线经过各固定点且连续光滑,如图所示
后来,样条发展成一种平滑曲线的数学表示方法。它通过连接一系列给定的数据点(节点)来构建曲线,以便在这些节点上产生平滑的过渡。通常情况下,样条曲线是由多个连续的二次或三次函数组成,每个函数都在相邻节点之间定义。这些连续的函数被称为样条段,它们共同组成了整个曲线
样条是在各个领域中广泛应用的一种技术,例如计算机图形学、物理学模拟、金融和经济分析等。在计算机图形学中,样条通常用于创建平滑的曲线和曲面,以便在三维场景中呈现出更真实的效果。在物理学模拟中,样条可用于描述物体的运动轨迹和变形过程。在金融和经济分析中,样条可用于拟合和预测时间序列数据,例如股票价格和货币汇率
本节介绍常见的三次样条曲线(Cubic Splines)原理
2 三次样条曲线原理
2.1 曲线插值
给定一系列插值点
X = { ( x 0 , y 0 ) , ( x 1 , y 1 ) , ⋯ , ( x n − 1 , y n − 1 ) } X=\left\{ \left( x_0,y_0 \right) ,\left( x_1,y_1 \right) ,\cdots ,\left( x_{n-1},y_{n-1} \right) \right\} X={(x0,y0),(x1,y1),⋯,(xn−1,yn−1)}
相邻两点间通过多项式曲线连接,因此共需要拼接 n − 1 n-1 n−1段曲线。定义三次多项式曲线为
f i ( x ) = a i + b i ( x − x i ) + c i ( x − x i ) 2 + d i ( x − x i ) 3 i = 0 , 1 , ⋯ , n − 1 f_i\left( x \right) =a_i+b_i\left( x-x_i \right) +c_i\left( x-x_i \right) ^2+d_i\left( x-x_i \right) ^3\,\,i=0,1,\cdots ,n-1 fi(x)=ai+bi(x−xi)+ci(x−xi)2+di(x−xi)3i=0,1,⋯,n−1
其中,当 i = n − 1 i=n-1 i=n−1时的曲线是辅助曲线,用于计算前 n − 1 n-1 n−1段曲线而不参与实际拼接。对于三次曲线,给出四个约束条件为
{ 过插值点 : f i ( x i ) = y i 曲线连续 : f i ( x i + 1 ) = y i + 1 一阶连续 : f ˙ i ( x i + 1 ) = f ˙ i + 1 ( x i + 1 ) 二阶连续 : f ¨ i ( x i + 1 ) = f ¨ i + 1 ( x i + 1 ) ⇒ h i = x i + 1 − x i { a i = y i a i + b i h i + c i h i 2 + d i h i 3 = y i + 1 b i + 2 c i h i + 3 d i h i 2 = b i + 1 c i + 3 d i h i = c i + 1 \begin{cases} \text{过插值点}: f_i\left( x_i \right) =y_i\\ \text{曲线连续}: f_i\left( x_{i+1} \right) =y_{i+1}\\ \text{一阶连续}: \dot{f}_i\left( x_{i+1} \right) =\dot{f}_{i+1}\left( x_{i+1} \right)\\ \text{二阶连续}: \ddot{f}_i\left( x_{i+1} \right) =\ddot{f}_{i+1}\left( x_{i+1} \right)\\\end{cases}\xRightarrow{h_i=x_{i+1}-x_i}\begin{cases} a_i=y_i\\ a_i+b_ih_i+c_ih_{i}^{2}+d_ih_{i}^{3}=y_{i+1}\\ b_i+2c_ih_i+3d_ih_{i}^{2}=b_{i+1}\\ c_i+3d_ih_i=c_{i+1}\\\end{cases} ⎩ ⎨ ⎧过插值点:fi(xi)=yi曲线连续:fi(xi+1)=yi+1一阶连续:f˙i(xi+1)=f˙i+1(xi+1)二阶连续:f¨i(xi+1)=f¨i+1(xi+1)hi=xi+1−xi⎩ ⎨ ⎧ai=yiai+bihi+cihi2+dihi3=yi+1bi+2cihi+3dihi2=bi+1ci+3dihi=ci+1
联立上式,用系数 统一表示其他参数可得
h i c i + 2 ( h i + h i + 1 ) c i + 1 + h i + 1 c i + 2 = 3 ( y i + 2 − y i + 1 h i + 1 − y i + 1 − y i h i ) h_ic_i+2\left( h_i+h_{i+1} \right) c_{i+1}+h_{i+1}c_{i+2}=3\left( \frac{y_{i+2}-y_{i+1}}{h_{i+1}}-\frac{y_{i+1}-y_i}{h_i} \right) hici+2(hi+hi+1)ci+1+hi+1ci+2=3(hi+1yi+2−yi+1−hiyi+1−yi)
其他参数表示为
{ a i = y i b i = y i + 1 − y i h i − c i + 1 + 2 c i 3 h i d i = c i + 1 − c i 3 h i \begin{cases} a_i=y_i\\ b_i=\frac{y_{i+1}-y_i}{h_i}-\frac{c_{i+1}+2c_i}{3}h_i\\ d_i=\frac{c_{i+1}-c_i}{3h_i}\\\end{cases} ⎩ ⎨ ⎧ai=yibi=hiyi+1−yi−3ci+1+2cihidi=3hici+1−ci
2.2 边界条件
注意到关于 c i c_i ci的线性方程仅有 n − 2 n-2 n−2个,而未知向量
c = [ c 0 c 1 ⋯ c n − 2 c n − 1 ] T \boldsymbol{c}=\left[ \begin{matrix} c_0& c_1& \cdots& c_{n-2}& c_{n-1}\\\end{matrix} \right] ^T c=[c0c1⋯cn−2cn−1]T
共有 n n n个元素,欠定方程组不足以进行求解。这是因为曲线首末处没有拼接约束,需要人为设定边界条件,常用的边界条件有
- 自然边界(Natural Spline):令端点二阶导为零,即
f 0 ′ ′ ( x 0 ) = f n − 1 ′ ′ ( x n − 1 ) = 0 f_{0}^{''}\left( x_0 \right) =f_{n-1}^{''}\left( x_{n-1} \right) =0 f0′′(x0)=fn−1′′(xn−1)=0 - 固定边界(Clamped Spline):令端点一阶导为常数,即
f 0 ′ ( x 0 ) = A , f n − 1 ′ ( x n − 1 ) = B f_{0}^{'}\left( x_0 \right) =A,f_{n-1}^{'}\left( x_{n-1} \right) =B f0′(x0)=A,fn−1′(xn−1)=B - 非扭结边界(Not-A-Knot Spline):令前两个点与最后两个点的三阶导值相等,即
f 0 ′ ′ ′ ( x 0 ) = f 1 ′ ′ ′ ( x 1 ) , f n − 2 ′ ′ ′ ( x n − 2 ) = f n − 1 ′ ′ ′ ( x n − 1 ) f_{0}^{'''}\left( x_0 \right) =f_{1}^{'''}\left( x_1 \right) , f_{n-2}^{'''}\left( x_{n-2} \right) =f_{n-1}^{'''}\left( x_{n-1} \right) f0′′′(x0)=f1′′′(x1),fn−2′′′(xn−2)=fn−1′′′(xn−1)
2.3 系数反解
本节选择自然边界,则 c 0 = c n − 1 = 0 c_0=c_{n-1}=0 c0=cn−1=0,将关于 c i c_i ci的线性方程改写为矩阵形式
[ 1 h 0 2 ( h 0 + h 1 ) h 1 h 1 2 ( h 1 + h 2 ) h 2 h 2 2 ( h 2 + h 3 ) h 3 ⋱ 1 ] [ c 0 c 1 c 2 c 3 ⋮ c n − 1 ] = 3 [ 0 y 2 − y 1 h 1 − y 1 − y 0 h 0 y 3 − y 2 h 2 − y 2 − y 1 h 1 y 4 − y 3 h 3 − y 3 − y 2 h 2 ⋮ 0 ] \left[ \begin{matrix} 1& & & & & \\ h_0& 2\left( h_0+h_1 \right)& h_1& & & \\ & h_1& 2\left( h_1+h_2 \right)& h_2& & \\ & & h_2& 2\left( h_2+h_3 \right)& h_3& \\ & & & & \ddots& \\ & & & & & 1\\\end{matrix} \right] \left[ \begin{array}{c} c_0\\ c_1\\ c_2\\ c_3\\ \vdots\\ c_{n-1}\\\end{array} \right] =3\left[ \begin{array}{c} 0\\ \frac{y_2-y_1}{h_1}-\frac{y_1-y_0}{h_0}\\ \frac{y_3-y_2}{h_2}-\frac{y_2-y_1}{h_1}\\ \frac{y_4-y_3}{h_3}-\frac{y_3-y_2}{h_2}\\ \vdots\\ 0\\\end{array} \right] 1h02(h0+h1)h1h12(h1+h2)h2h22(h2+h3)h3⋱1 c0c1c2c3⋮cn−1 =3 0h1y2−y1−h0y1−y0h2y3−y2−h1y2−y1h3y4−y3−h2y3−y2⋮0
该方程组有唯一解
3 算法仿真
3.1 ROS C++仿真
核心代码如下所示
std::vector<double> CubicSpline::spline(std::vector<double> s_list, std::vector<double> dir_list, std::vector<double> t)
{// cubic polynomial functionsstd::vector<double> a = dir_list;std::vector<double> b, d;size_t num = s_list.size();std::vector<double> h;for (size_t i = 0; i < num - 1; i++)h.push_back(s_list[i + 1] - s_list[i]);// calculate coefficient matrixEigen::MatrixXd A = Eigen::MatrixXd::Zero(num, num);for (size_t i = 1; i < num - 1; i++){A(i, i - 1) = h[i - 1];A(i, i) = 2.0 * (h[i - 1] + h[i]);A(i, i + 1) = h[i];}A(0, 0) = 1.0;A(num - 1, num - 1) = 1.0;Eigen::MatrixXd B = Eigen::MatrixXd::Zero(num, 1);for (size_t i = 1; i < num - 1; i++)B(i, 0) = 3.0 * (a[i + 1] - a[i]) / h[i] - 3.0 * (a[i] - a[i - 1]) / h[i - 1];Eigen::MatrixXd c = A.lu().solve(B);for (size_t i = 0; i < num - 1; i++){b.push_back((a[i + 1] - a[i]) / h[i] - h[i] * (c(i + 1) + 2.0 * c(i)) / 3.0);d.push_back((c(i + 1) - c(i)) / (3.0 * h[i]));}// calculate spline value and its derivativestd::vector<double> p;for (const auto it : t){auto iter = std::find_if(s_list.begin(), s_list.end(), [it](double val) { return val > it; });if (iter != s_list.end()){size_t idx = std::distance(s_list.begin(), iter) - 1;double ds = it - s_list[idx];p.push_back(a[idx] + b[idx] * ds + c(idx) * std::pow(ds, 2) + d[idx] * std::pow(ds, 3));}}return p;
}
3.2 Python仿真
核心代码如下所示
def spline(self, x_list: list, y_list: list, t: list):# cubic polynomial functionsa, b, c, d = y_list, [], [], []h = np.diff(x_list)num = len(x_list)# calculate coefficient matrixA = np.zeros((num, num))for i in range(1, num - 1):A[i, i - 1] = h[i - 1]A[i, i] = 2.0 * (h[i - 1] + h[i])A[i, i + 1] = h[i]A[0, 0] = 1.0A[num - 1, num - 1] = 1.0B = np.zeros(num)for i in range(1, num - 1):B[i] = 3.0 * (a[i + 1] - a[i]) / h[i] - \3.0 * (a[i] - a[i - 1]) / h[i - 1]c = np.linalg.solve(A, B)for i in range(num - 1):d.append((c[i + 1] - c[i]) / (3.0 * h[i]))b.append((a[i + 1] - a[i]) / h[i] - h[i] * (c[i + 1] + 2.0 * c[i]) / 3.0)# calculate spline value and its derivativep, dp = [], []for it in t:if it < x_list[0] or it > x_list[-1]:continuei = bisect.bisect(x_list, it) - 1dx = it - x_list[i]p.append(a[i] + b[i] * dx + c[i] * dx**2 + d[i] * dx**3)dp.append(b[i] + 2.0 * c[i] * dx + 3.0 * d[i] * dx**2)return p, dp
3.3 Matlab仿真
核心代码如下所示
function p = spline(s_list, dir_list, t)% cubic polynomial functionsa = dir_list;[num, ~] = size(s_list);h = diff(s_list);% calculate coefficient matrixA = zeros(num, num);for i=2:num - 1A(i, i - 1) = h(i - 1);A(i, i) = 2.0 * (h(i - 1) + h(i));A(i, i + 1) = h(i);endA(1, 1) = 1.0;A(num, num) = 1.0;B = zeros(num, 1);for i=2:num - 1B(i, 1) = 3.0 * (a(i + 1) - a(i)) / h(i) - 3.0 * (a(i) - a(i - 1)) / h(i - 1);endc = A \ B;b = zeros(num - 1, 1); d = zeros(num - 1, 1);for i=1:num - 1b(i) = (a(i + 1) - a(i)) / h(i) - h(i) * (c(i + 1) + 2.0 * c(i)) / 3.0;d(i) = (c(i + 1) - c(i)) / (3.0 * h(i));end% calculate spline value and its derivativep = [];for i =1:length(t)idx = find(s_list > t(i));if ~isempty(idx)id = idx(1) - 1;ds = t(i) - s_list(id);p = [p; a(id) + b(id) * ds + c(id) * power(ds, 2) + d(id) * power(ds, 3)];endend
end
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