RobotStudio/robot/Octave/@SerialLink/ikine6s.m
%SerialLink.ikine6s Inverse kinematics for 6-axis robot with spherical wrist
%
% Q = R.ikine6s(T) is the joint coordinates corresponding to the robot
% end-effector pose T represented by the homogenenous transform.  This
% is a analytic solution for a 6-axis robot with a spherical wrist (such as
% the Puma 560).
%
% Q = R.IKINE6S(T, CONFIG) as above but specifies the configuration of the arm in
% the form of a string containing one or more of the configuration codes:
%
% 'l'   arm to the left (default)
% 'r'   arm to the right
% 'u'   elbow up (default)
% 'd'   elbow down
% 'n'   wrist not flipped (default)
% 'f'   wrist flipped (rotated by 180 deg)
%
% Notes::
% - The inverse kinematic solution is generally not unique, and 
%   depends on the configuration string.
%
% Reference::
%
% Inverse kinematics for a PUMA 560 based on the equations by Paul and Zhang
% From The International Journal of Robotics Research
% Vol. 5, No. 2, Summer 1986, p. 32-44
%
%
% Author::
% Robert Biro with Gary Von McMurray,
% GTRI/ATRP/IIMB,
% Georgia Institute of Technology
% 2/13/95
%
% See also SerialLink.FKINE, SerialLink.IKINE.

function theta = ikine6s(robot, T, varargin)

    if robot.n ~= 6,
        error('Solution only applicable for 6DOF manipulator');
    end

    if robot.mdh ~= 0,
        error('Solution only applicable for standard DH conventions');
    end

    if ndims(T) == 3,
        theta = [];
        for k=1:size(T,3),
            th = ikine6s(robot, T(:,:,k), varargin{:});
            theta = [theta; th];
        end

        return;
    end
    L = robot.links;
    a1 = L(1).a;
    a2 = L(2).a;
    a3 = L(3).a;

    if ~isspherical(robot)
        error('wrist is not spherical')
    end

    d1 = L(1).d;
    d2 = L(2).d;
    d3 = L(3).d;
    d4 = L(4).d;

    if ~ishomog(T),
        error('T is not a homog xform');
    end

    % undo base transformation
    T = inv(robot.base) * T;

    % The following parameters are extracted from the Homogeneous 
    % Transformation as defined in equation 1, p. 34

    Ox = T(1,2);
    Oy = T(2,2);
    Oz = T(3,2);

    Ax = T(1,3);
    Ay = T(2,3);
    Az = T(3,3);

    Px = T(1,4);
    Py = T(2,4);
    Pz = T(3,4);

    % The configuration parameter determines what n1,n2,n4 values are used
    % and how many solutions are determined which have values of -1 or +1.

    if nargin < 3,
        configuration = '';
    else
        configuration = lower(varargin{1});
    end

    % default configuration

    n1 = -1;    % L
    n2 = -1;    % U
    n4 = -1;    % N
    if ~isempty(findstr(configuration, 'l')),
        n1 = -1;
    end
    if ~isempty(findstr(configuration, 'r')),
        n1 = 1;
    end
    if ~isempty(findstr(configuration, 'u')),
        if n1 == 1,
            n2 = 1;
        else
            n2 = -1;
        end
    end
    if ~isempty(findstr(configuration, 'd')),
        if n1 == 1,
            n2 = -1;
        else
            n2 = 1;
        end
    end
    if ~isempty(findstr(configuration, 'n')),
        n4 = 1;
    end
    if ~isempty(findstr(configuration, 'f')),
        n4 = -1;
    end


    %
    % Solve for theta(1)
    % 
    % r is defined in equation 38, p. 39.
    % theta(1) uses equations 40 and 41, p.39, 
    % based on the configuration parameter n1
    %

    r=sqrt(Px^2 + Py^2);
    if (n1 == 1),
        theta(1)= atan2(Py,Px) + asin(d3/r);
    else
        theta(1)= atan2(Py,Px) + pi - asin(d3/r);
    end

    %
    % Solve for theta(2)
    %
    % V114 is defined in equation 43, p.39.
    % r is defined in equation 47, p.39.
    % Psi is defined in equation 49, p.40.
    % theta(2) uses equations 50 and 51, p.40, based on the configuration 
    % parameter n2
    %

    V114= Px*cos(theta(1)) + Py*sin(theta(1));
    r=sqrt(V114^2 + Pz^2);
    Psi = acos((a2^2-d4^2-a3^2+V114^2+Pz^2)/(2.0*a2*r));
    if ~isreal(Psi),
        warning('point not reachable');
        theta = [NaN NaN NaN NaN NaN NaN];
        return
    end
    theta(2) = atan2(Pz,V114) + n2*Psi;

    %
    % Solve for theta(3)
    %
    % theta(3) uses equation 57, p. 40.
    %

    num = cos(theta(2))*V114+sin(theta(2))*Pz-a2;
    den = cos(theta(2))*Pz - sin(theta(2))*V114;
    theta(3) = atan2(a3,d4) - atan2(num, den);

    %
    % Solve for theta(4)
    %
    % V113 is defined in equation 62, p. 41.
    % V323 is defined in equation 62, p. 41.
    % V313 is defined in equation 62, p. 41.
    % theta(4) uses equation 61, p.40, based on the configuration 
    % parameter n4
    %

    V113 = cos(theta(1))*Ax + sin(theta(1))*Ay;
    V323 = cos(theta(1))*Ay - sin(theta(1))*Ax;
    V313 = cos(theta(2)+theta(3))*V113 + sin(theta(2)+theta(3))*Az;
    theta(4) = atan2((n4*V323),(n4*V313));
    %[(n4*V323),(n4*V313)]

    %
    % Solve for theta(5)
    %
    % num is defined in equation 65, p. 41.
    % den is defined in equation 65, p. 41.
    % theta(5) uses equation 66, p. 41.
    %
     
    num = -cos(theta(4))*V313 - V323*sin(theta(4));
    den = -V113*sin(theta(2)+theta(3)) + Az*cos(theta(2)+theta(3));
    theta(5) = atan2(num,den);
    %[num den]

    %
    % Solve for theta(6)
    %
    % V112 is defined in equation 69, p. 41.
    % V122 is defined in equation 69, p. 41.
    % V312 is defined in equation 69, p. 41.
    % V332 is defined in equation 69, p. 41.
    % V412 is defined in equation 69, p. 41.
    % V432 is defined in equation 69, p. 41.
    % num is defined in equation 68, p. 41.
    % den is defined in equation 68, p. 41.
    % theta(6) uses equation 70, p. 41.
    %

    V112 = cos(theta(1))*Ox + sin(theta(1))*Oy;
    V132 = sin(theta(1))*Ox - cos(theta(1))*Oy;
    V312 = V112*cos(theta(2)+theta(3)) + Oz*sin(theta(2)+theta(3));
    V332 = -V112*sin(theta(2)+theta(3)) + Oz*cos(theta(2)+theta(3));
    V412 = V312*cos(theta(4)) - V132*sin(theta(4));
    V432 = V312*sin(theta(4)) + V132*cos(theta(4));
    num = -V412*cos(theta(5)) - V332*sin(theta(5));
    den = - V432;
    theta(6) = atan2(num,den);

    % remove the link offset angles
    for i=1:6
        theta(i) = theta(i) - L(i).offset;
    end
