以下是平面四連桿的運動學分析:
%%***************planner four links system**********%% function fourlinks clc; clear all; %% %輸入結構參數 global l1 l2 l3 l4 theta2 l1=0.4;l2=0.2;l3=0.4;l4=0.5; w2=50; pi=3.1415926; x0=[0.79 4.9]; n=500; %% for i=1:n theta2=pi/2+(i-1)*0.02; x=fsolve(@f3_4,x0,optimset('fsolve')); z34(i,:)=x; %角位移存儲矩陣 %% %**********位置分析************** x0=x; z2(i)=theta2; %曲柄角度存儲矩陣 %% %%**************速度分析********* c=l2*w2/(l3*l4*sin(x(2)-x(1))); w34(i,1)=c*l4*sin(theta2-x(2)); w34(i,2)=c*l3*sin(-theta2+x(1)); %% %*************加速度分析********* c1=l4*w34(i,2)^2*cos(x(2))+l2*w2^2*cos(theta2)... +l3*w34(i,1)^2*cos(x(1)); c2=l4*w34(i,2)^2*sin(x(2))+l2*w2^2*sin(theta2)... +l3*w34(i,1)^2*sin(x(1)); c3=l3*l4*sin(x(2)-x(1)); a34(i,1)=l4*(c1*cos(x(2))+c2*sin(x(2)))/c3; a34(i,2)=-l3*(c1*cos(x(1))+c2*sin(x(1)))/c3; %% end %% figure(1); plot(z2,z34) grid on; legend('theta_3','theta_4'); xlabel('theta2','color','r','fontsize',8); ylabel('theta3 theta4','color','y','fontsize',8); figure(2) plot(z2,w34) grid on legend('w_3','w_4'); xlabel('theta_2','color','b','fontsize',12,'linewidth',5); ylabel('w_3_4','color','b','fontsize',12,'linewidth',7); figure(3) plot(z2,a34) grid on legend('a_3','a_4'); xlabel('theta_2','color','b','fontsize',12,'linewidth',5); ylabel('a_3_4','color','b','fontsize',12,'linewidth',7); end %% function y=f3_4(x) clc; global theta2 l1=0.4; l2=0.2; l3=0.4; l4=0.5; y(1)=l3*cos(x(1))+l4*cos(x(2))-l1+l2*cos(theta2); y(2)=l3*sin(x(1))+l4*sin(x(2))+l2*sin(theta2); end
運行結果: