Unanswered Questions

This page lists MaplePrimes questions that have not yet received an answer

I asked Maple AI what a glyph is. Then I prompted this

A kernel lost message was returned and the AI pannel became irresponsive.

Maple is still running well in exsisting and new tabs. 

Can the AI service be restarted from the user interface?

(Is that crash reproducible?)

 

Edit:

05-2-2.mws

Can you help me with this code?

restart: with(VectorCalculus):

assume(g>0,Omega>0,V0>0,theta>0,alpha>0,alpha<=Pi/2):

alias(omega=w,Omega=W,alpha=a):

w:=<-W*cos(a),0,W*sin(a)>;

Vector(3, {(1) = -W*cos(a), (2) = 0, (3) = W*sin(a)})

(1)

r:=<x(t),y(t),z(t)>; v:=diff(r,t);

Vector(3, {(1) = x(t), (2) = y(t), (3) = z(t)})

Vector(3, {(1) = diff(x(t), t), (2) = diff(y(t), t), (3) = diff(z(t), t)})

(2)

F[gravity]:=<0,0,-g>;

Vector(3, {(1) = 0, (2) = 0, (3) = -g})

(3)

F[Coriolis]:=-2*w &x v;

Vector(3, {(1) = 2*W*sin(a)*(diff(y(t), t)), (2) = -2*W*cos(a)*(diff(z(t), t))-2*W*sin(a)*(diff(x(t), t)), (3) = 2*W*cos(a)*(diff(y(t), t))})

(4)

F[centrifugal]:=-w &x (w &x r);

Vector(3, {(1) = W*sin(a)*(W*cos(a)*z(t)+W*sin(a)*x(t)), (2) = W^2*cos(a)^2*y(t)+W^2*sin(a)^2*y(t), (3) = W*cos(a)*(W*cos(a)*z(t)+W*sin(a)*x(t))})

(5)

F[resultant]:=F[gravity]+F[Coriolis]+F[centrifugal];

Vector(3, {(1) = 2*W*sin(a)*(diff(y(t), t))+W*sin(a)*(W*cos(a)*z(t)+W*sin(a)*x(t)), (2) = -2*W*cos(a)*(diff(z(t), t))-2*W*sin(a)*(diff(x(t), t))+W^2*cos(a)^2*y(t)+W^2*sin(a)^2*y(t), (3) = -g+2*W*cos(a)*(diff(y(t), t))+W*cos(a)*(W*cos(a)*z(t)+W*sin(a)*x(t))})

(6)

eq:=(u,i)->simplify(diff(u(t),t,t)=F[resultant][i]):

xeq:=eq(x,1); yeq:=eq(y,2); zeq:=eq(z,3);

xeq := diff(x(t), `$`(t, 2)) = Omega*sin(alpha)*(Omega*sin(alpha)*x(t)+Omega*cos(alpha)*z(t)+2*(diff(y(t), t)))

yeq := diff(y(t), `$`(t, 2)) = Omega*(y(t)*Omega-2*(diff(z(t), t))*cos(alpha)-2*(diff(x(t), t))*sin(alpha))

zeq := diff(z(t), `$`(t, 2)) = sin(alpha)*cos(alpha)*x(t)*Omega^2+cos(alpha)^2*z(t)*Omega^2+2*Omega*cos(alpha)*(diff(y(t), t))-g

(7)

ic:=x(0)=0,y(0)=0,z(0)=0,D(x)(0)=0,D(y)(0)=V0*cos(theta),D(z)(0)=V0*sin(theta);

ic := x(0) = 0, y(0) = 0, z(0) = 0, (D(x))(0) = 0, (D(y))(0) = V0*cos(theta), (D(z))(0) = V0*sin(theta)

(8)

sol:=dsolve({xeq,yeq,zeq,ic},{x(t),y(t),z(t)},method=laplace):

assign(sol):

f:=u->simplify(expand(u(t))): X:=f(x); Y:=f(y); Z:=f(z);

X := -(1/4)*(Omega^4*V0*sin(theta)*cos(alpha)*(sum(exp(_alpha1*t)/((Omega^2+_alpha1^2)*_alpha1), _alpha1 = RootOf(Omega^2+_Z^2)))+cos(alpha)*g*(sum(exp(_alpha1*t)*_alpha1^2/(Omega^2+_alpha1^2), _alpha1 = RootOf(Omega^2+_Z^2)))-sin(theta)*cos(alpha)*V0*(sum(exp(_alpha1*t)*_alpha1/(Omega^2+_alpha1^2), _alpha1 = RootOf(Omega^2+_Z^2)))*Omega^2+(-2*Omega^3*cos(theta)*V0+3*cos(alpha)*Omega^2*g)*(sum(exp(_alpha1*t)/(Omega^2+_alpha1^2), _alpha1 = RootOf(Omega^2+_Z^2)))+4*(Omega^2*t*V0*sin(theta)-(1/2)*Omega^2*t^2*g-g)*cos(alpha))*sin(alpha)/Omega^2

Y := (1/4)*(-V0*cos(theta)*Omega^2+2*cos(alpha)*Omega*g)*(sum(exp(_alpha1*t)/((Omega^2+_alpha1^2)*_alpha1), _alpha1 = RootOf(Omega^2+_Z^2)))-(1/2)*sin(theta)*cos(alpha)*V0*Omega*(sum(exp(_alpha1*t)/(Omega^2+_alpha1^2), _alpha1 = RootOf(Omega^2+_Z^2)))+(1/4)*V0*cos(theta)*(sum(exp(_alpha1*t)*_alpha1/(Omega^2+_alpha1^2), _alpha1 = RootOf(Omega^2+_Z^2)))

Z := (1/4)*(-Omega^4*cos(alpha)^2*V0*sin(theta)*(sum(exp(_alpha1*t)/((Omega^2+_alpha1^2)*_alpha1), _alpha1 = RootOf(Omega^2+_Z^2)))-cos(alpha)^2*g*(sum(exp(_alpha1*t)*_alpha1^2/(Omega^2+_alpha1^2), _alpha1 = RootOf(Omega^2+_Z^2)))+cos(alpha)^2*sin(theta)*V0*(sum(exp(_alpha1*t)*_alpha1/(Omega^2+_alpha1^2), _alpha1 = RootOf(Omega^2+_Z^2)))*Omega^2+(2*Omega^3*cos(alpha)*cos(theta)*V0-3*Omega^2*g*cos(alpha)^2)*(sum(exp(_alpha1*t)/(Omega^2+_alpha1^2), _alpha1 = RootOf(Omega^2+_Z^2)))+(-4*Omega^2*t*V0*sin(theta)+2*Omega^2*t^2*g+4*g)*cos(alpha)^2+4*Omega^2*t*V0*sin(theta)-2*Omega^2*t^2*g)/Omega^2

(9)

P:=(u,n)->convert(taylor(u,W=0,n),polynom):

Xexp:=P(X,4); Yexp:=P(Y,4); Zexp:=P(Z,4);  

Error, (in series/sum) unable to compute series

Error, (in series/sum) unable to compute series

Error, (in series/sum) unable to compute series

 

tt:=solve(Zexp=0,t);

tt :=

(10)

 T1:=P(tt[2],1); d[x]:=eval(Xexp,t=T1);  

Error, invalid subscript selector

d[x] := Xexp

 

T2:=P(tt[2],2); d[y]:=P(eval(Yexp,t=T2),2);

Error, invalid subscript selector

d[y] := Yexp

 

d[y]:=collect(d[y],[cos(a),1/g^2,V0^3,W]);

d[y] := Yexp

(11)

parameters:={a=Pi/4,theta=Pi/3,V0=500,W=7.27*10^(-5),g=9.8}:

d[x]:=eval(d[x],evalf(parameters));

d[x] := Xexp

(12)

d[y]:=eval(d[y],evalf(parameters));

d[y] := Yexp

(13)
 

 

Download 05-2-2.mws

Can anyone share additional information about the Maple conference to be held in 2026? I want to submit a talk and then submit a paper to the Maple Transactions journal based on the same.

Para_1.mw.  please help to correct this error.

It seems that in Maple 2025+ on Windows 11, the SMTLIB package is not working. For example:

SMTLIB:-Satisfiable( {x^2+y^2+z^2<1, x*y*z>1} ) assuming real;

complains about error loading external library mplsmtlib.dll.

Is there an explanation, or a workaround?

Hi,

I need to run the following procedure a couple of million times. Although it works, Maple sometimes chokes for no apparent reason (if there is a reason, please let me know). I was wondering whether an expert could help me tweak the procedure (or possibly rewrite it) to achieve the best possible performance. I am planning to use Grid:-Map or, if possible, Threads:-Map.

 

generateNonlinearModelsPlus := proc(model::list,fullmodel::list,vars::list:=[x,y,z])
description "This function generates a list of all models with one more monomial from the full model":
local tab::table(),n:=nops(model),i,j,k:=1,ans,terms,aaa,allmoncoefThreads:
# local procedure
allmoncoefThreads := proc(f::list,vars::list)
description "This function finds the monomials multipled by their coefficients for each expression (equation) of a list.":
local n:=numelems(f),i,mon:=[seq](0,i=1..n),M,cc:=[seq](0,i=1..n),ans:
for i from 1 to n do
  cc[i]:=[coeffs](expand(f[i]),vars, 'M'):
  mon[i]:=[M]:
end do:
ans:=[seq](zip((ww,vv)->ww*vv,cc[i],mon[i]),i=1..n):
return(ans)
end proc:
# main part
ans:=zip((w,v)->expand(simplify(v-w)),model,fullmodel): # Find the monomials that are not in model
terms:=allmoncoefThreads(ans,vars): # Separate the monomials
#
for i from 1 to n do
   aaa:=model:
   for j from 1 to nops(terms[i]) do
       aaa[i]:=model[i]+terms[i,j]:
       tab[k]:=aaa:
       k:=k+1:
   end do:
end do:
tab:=convert(tab,list):
return(tab):
end proc:

Here is an example of how I run it: 

model:=[y*alpha[1, 2], z*alpha[2, 3], x^3*alpha[3, 10] + x*alpha[3, 1] + alpha[3, 0]]:

fullmodel:=[x^3*alpha[1, 10] + x^2*y*alpha[1, 11] + x^2*z*alpha[1, 12] + x*y^2*alpha[1, 13] + x*y*z*alpha[1, 14] + x*z^2*alpha[1, 15] + y^3*alpha[1, 16] + y^2*z*alpha[1, 17] + y*z^2*alpha[1, 18] + z^3*alpha[1, 19] + x^2*alpha[1, 4] + x*y*alpha[1, 5] + x*z*alpha[1, 6] + y^2*alpha[1, 7] + y*z*alpha[1, 8] + z^2*alpha[1, 9] + x*alpha[1, 1] + y*alpha[1, 2] + z*alpha[1, 3] + alpha[1, 0], x^3*alpha[2, 10] + x^2*y*alpha[2, 11] + x^2*z*alpha[2, 12] + x*y^2*alpha[2, 13] + x*y*z*alpha[2, 14] + x*z^2*alpha[2, 15] + y^3*alpha[2, 16] + y^2*z*alpha[2, 17] + y*z^2*alpha[2, 18] + z^3*alpha[2, 19] + x^2*alpha[2, 4] + x*y*alpha[2, 5] + x*z*alpha[2, 6] + y^2*alpha[2, 7] + y*z*alpha[2, 8] + z^2*alpha[2, 9] + x*alpha[2, 1] + y*alpha[2, 2] + z*alpha[2, 3] + alpha[2, 0], x^3*alpha[3, 10] + x^2*y*alpha[3, 11] + x^2*z*alpha[3, 12] + x*y^2*alpha[3, 13] + x*y*z*alpha[3, 14] + x*z^2*alpha[3, 15] + y^3*alpha[3, 16] + y^2*z*alpha[3, 17] + y*z^2*alpha[3, 18] + z^3*alpha[3, 19] + x^2*alpha[3, 4] + x*y*alpha[3, 5] + x*z*alpha[3, 6] + y^2*alpha[3, 7] + y*z*alpha[3, 8] + z^2*alpha[3, 9] + x*alpha[3, 1] + y*alpha[3, 2] + z*alpha[3, 3] + alpha[3, 0]]:

vars:=[x,y,z]:

ans:=generateNonlinearModelsPlus(model,fullmodel,vars)

Many thanks.

For quite some time, I have wanted to solve the system attached in "test" using Maple. The smallest solution in natural numbers x, y, and z test.mw

restart

kernelopts(version)

`Maple 2026.0, X86 64 WINDOWS, Apr 28 2026, Build ID 2011354`

(1)

interface(version)

`Standard Worksheet Interface, Maple 2026.1, Windows 11, April 28 2026 Build ID 2011354`

(2)

with(NumberTheory)

isolve({x*y*z = w^2, x+y+z = u^2, x*y+x*z+y*z = v^2})

{u = _Z1, v = 0, w = 0, x = _Z1^2, y = 0, z = 0}

(3)

"(->)"

{u = _Z1, v = 0, w = 0, x = _Z1^2, y = 0, z = 0}

(4)

``

Download test.mw

is known, and all these numbers are less than 4 × 10¹². Is this possible in Maple?

(x=1633780814400; y=252782198228; z=3474741058973)

Currently I have Maple versions 2023,2025, and 2026 installed on Windows 11. Today I installed a workbook package containing a module that I just completed using the PackageTools installer in Maple 2026.. To my surprise, I found that a package installed from Maple 2026 was also available in Maple 2023 and, conversely, a package installed in Maple 2023 was automatically available in Maple 2026. i noticed that, with the exception of the Maple Customer Support Updates, the toolbox directory is no longer broken down by versions. I also noticed that the directory containing the module installed by Maple 2026 was named by the workbook instead of the module name (ie. hopfwords.maple). As I recall, the toolboxes used to be version dependent. 

The question is to what extent can one assume that a package created in Maple 2026 will be compatible with at least the more recent versions of Maple, I am also wondering why the directory name is now the workbook name instead of the module name. 

restart;

with(plots): with(LinearAlgebra):

 

# TFSB Coefficients (symbolic in u)

beta0 := u -> (sin(u)*u^3 - 12*u^2 - 24*cos(u) + 24)/(12*(sin(u)*u + 2*cos(u) - 2)*u^2):

beta1 := u -> (5*sin(u)*u^3 + 12*cos(u)*u^2 + 24*cos(u) - 24)/(6*(sin(u)*u + 2*cos(u) - 2)*u^2):

beta2 := u -> beta0(u):

rho0 := u -> ((-u^2-12)*cos(u) - 5*u^2 + 12)/(12*(sin(u)*u + 2*cos(u) - 2)*u^2):

rho1 := u -> (-7*cos(u)*u^3 + 27*sin(u)*u^2 + 120*sin(u) - 120*u)/(60*u^2*(cos(u)*u + 2*u - 3*sin(u))):

rho2 := u -> -rho0(u):

 

# Secondary coefficients (simplified versions)

beta00 := u -> 13/42 - 9*u^2/7840:

beta10 := u -> 1/6 + u^2/720:

beta20 := u -> 1/42 - 17*u^2/70560:

beta01 := u -> 187/1680 + 611*u^2/705600:

beta11 := u -> 11/30 - 29*u^2/25200:

beta21 := u -> 37/1680 + 67*u^2/235200:

beta02 := u -> 11/70 + 491*u^2/352800:

beta12 := u -> 9/10 - 31*u^2/8400:

beta22 := u -> 31/70 + 811*u^2/352800:

 

rho01 := u -> 2/105 + 407*u^2/1058400:

rho11 := u -> -19/210 + 41*u^2/105840:

rho21 := u -> -1/168 - 101*u^2/529200:

rho02 := u -> 53/1680 + 1633*u^2/2116800:

rho12 := u -> 8/105 - 4*u^2/6615:

rho22 := u -> -101/1680 - 2273*u^2/2116800:

 

# Problem definition

omega := 1:

epsilon := 3*Pi/2:

phi := x -> 3*sin(x) - 5*cos(x):  # history function

 

f := (x, v, vp, vd) -> -v - vd + 3*cos(x) + 5*sin(x):

g := proc(x, v, vp, vd, vdp)

    local fx, fv, fvp, fvd;

    fx := -3*sin(x) + 5*cos(x);

    fv := -1;

    fvp := 0;

    fvd := -1;

    return fx + fv*vp + fvp*0 + fvd*vdp;

end proc:

 

# Initial conditions

a := 0: b := 10:

v0 := -5: vp0 := 3:

 

# Variable step-size parameters

tol := 1e-10:

h_min := 0.01:

h_max := 0.5:

h_init := Pi/8:

 

# Store results

X := [a]: V := [v0]: Vp := [vp0]:

h_curr := h_init:

x_curr := a:

v_curr := v0:

vp_curr := vp0:

 

# For history: need v at x-epsilon

get_v_delayed := proc(xx)

    if xx < a then return phi(xx);

    else

        # Interpolate from stored solution

        idx := 1;

        while idx < nops(X) and X[idx] < xx do idx := idx+1; end do;

        if idx = 1 then return phi(xx);

        elif X[idx] = xx then return V[idx];

        else

            # Linear interpolation

            return V[idx-1] + (V[idx]-V[idx-1])*(xx-X[idx-1])/(X[idx]-X[idx-1]);

        end if;

    end if;

end proc:

 

# Newton solver for block

solve_block := proc(x0, v0, vp0, h, omega)

    local u, bet0, bet1, bet2, rho0, rho1, rho2, bet00, bet10, bet20, bet01, bet11, bet21, bet02, bet12, bet22,

          rho01, rho11, rho21, rho02, rho12, rho22, F, J, V0, V1, V2, Vp0, Vp1, Vp2, tolN, iter, dv, dV;

   

    u := omega*h;

    bet0 := beta0(u); bet1 := beta1(u); bet2 := beta2(u);

    rho0 := rho0(u); rho1 := rho1(u); rho2 := rho2(u);

    bet00 := beta00(u); bet10 := beta10(u); bet20 := beta20(u);

    bet01 := beta01(u); bet11 := beta11(u); bet21 := beta21(u);

    bet02 := beta02(u); bet12 := beta12(u); bet22 := beta22(u);

    rho01 := rho01(u); rho11 := rho11(u); rho21 := rho21(u);

    rho02 := rho02(u); rho12 := rho12(u); rho22 := rho22(u);

   

    # Initial guesses

    V1 := v0 + h*vp0;

    V2 := v0 + 2*h*vp0;

    Vp1 := vp0;

    Vp2 := vp0;

   

    tolN := 1e-12;

    for iter from 1 to 10 do

        # Compute delayed values

        vd0 := get_v_delayed(x0 - epsilon);

        vd1 := get_v_delayed(x0 + h - epsilon);

        vd2 := get_v_delayed(x0 + 2*h - epsilon);

        vdp0 := (get_v_delayed(x0 - epsilon + 1e-8) - vd0)/1e-8;

        vdp1 := (get_v_delayed(x0 + h - epsilon + 1e-8) - vd1)/1e-8;

        vdp2 := (get_v_delayed(x0 + 2*h - epsilon + 1e-8) - vd2)/1e-8;

       

        # Compute gamma and g

        gam0 := f(x0, v0, vp0, vd0);

        gam1 := f(x0+h, V1, Vp1, vd1);

        gam2 := f(x0+2*h, V2, Vp2, vd2);

        g0 := g(x0, v0, vp0, vd0, vdp0);

        g1 := g(x0+h, V1, Vp1, vd1, vdp1);

        g2 := g(x0+2*h, V2, Vp2, vd2, vdp2);

       

        # Residuals

        F1 := h*vp0 - (V1 - v0 + h^2*(bet00*gam0 + bet10*gam1 + bet20*gam2)

              + h^3*(rho01*g0 + rho11*g1 + rho21*g2));

        F2 := h*Vp1 - (V1 - v0 + h^2*(bet01*gam0 + bet11*gam1 + bet21*gam2)

              + h^3*(rho01*g0 + rho11*g1 + rho21*g2));

        F3 := h*Vp2 - (V1 - v0 + h^2*(bet02*gam0 + bet12*gam1 + bet22*gam2)

              + h^3*(rho02*g0 + rho12*g1 + rho22*g2));

        F4 := V2 - (2*V1 - v0 + h^2*(bet0*gam0 + bet1*gam1 + bet2*gam2)

              + h^3*(rho0*g0 + rho1*g1 + rho2*g2));

       

        F := Vector([F1, F2, F3, F4]);

        if LinearAlgebra:-Norm(F) < tolN then break; end if;

       

        # Approximate Jacobian (finite differences)

        J := Matrix(4,4);

        delta := 1e-6;

        for j from 1 to 4 do

            V_pert := Vector([V1, V2, Vp1, Vp2]);

            V_pert[j] := V_pert[j] + delta;

            V1p := V_pert[1]; V2p := V_pert[2]; Vp1p := V_pert[3]; Vp2p := V_pert[4];

            gam1p := f(x0+h, V1p, Vp1p, get_v_delayed(x0+h-epsilon));

            gam2p := f(x0+2*h, V2p, Vp2p, get_v_delayed(x0+2*h-epsilon));

            g1p := g(x0+h, V1p, Vp1p, get_v_delayed(x0+h-epsilon),

                     (get_v_delayed(x0+h-epsilon+1e-8)-get_v_delayed(x0+h-epsilon))/1e-8);

            g2p := g(x0+2*h, V2p, Vp2p, get_v_delayed(x0+2*h-epsilon),

                     (get_v_delayed(x0+2*h-epsilon+1e-8)-get_v_delayed(x0+2*h-epsilon))/1e-8);

           

            F1p := h*vp0 - (V1p - v0 + h^2*(bet00*gam0 + bet10*gam1p + bet20*gam2p)

                   + h^3*(rho01*g0 + rho11*g1p + rho21*g2p));

            F2p := h*Vp1p - (V1p - v0 + h^2*(bet01*gam0 + bet11*gam1p + bet21*gam2p)

                   + h^3*(rho01*g0 + rho11*g1p + rho21*g2p));

            F3p := h*Vp2p - (V1p - v0 + h^2*(bet02*gam0 + bet12*gam1p + bet22*gam2p)

                   + h^3*(rho02*g0 + rho12*g1p + rho22*g2p));

            F4p := V2p - (2*V1p - v0 + h^2*(bet0*gam0 + bet1*gam1p + bet2*gam2p)

                   + h^3*(rho0*g0 + rho1*g1p + rho2*g2p));

           

            Fp := Vector([F1p, F2p, F3p, F4p]);

            J[1..4, j] := (Fp - F)/delta;

        end do;

       

        dV := LinearAlgebra:-LinearSolve(J, -F);

        V1 := V1 + dV[1]; V2 := V2 + dV[2]; Vp1 := Vp1 + dV[3]; Vp2 := Vp2 + dV[4];

    end do;

   

    return [V1, V2, Vp1, Vp2];

end proc:

 

# Main variable step-size loop

printf("Variable step-size integration for Example 1\n");

printf("tol = %e, h_init = %f\n", tol, h_init);

 

while x_curr < b - 1e-12 do

    # Try current step

    sol := solve_block(x_curr, v_curr, vp_curr, h_curr, omega);

    V1 := sol[1]; V2 := sol[2]; Vp1 := sol[3]; Vp2 := sol[4];

   

    # Compute with two half-steps

    sol_half1 := solve_block(x_curr, v_curr, vp_curr, h_curr/2, omega);

    V_mid := sol_half1[2]; Vp_mid := sol_half1[4];

    sol_half2 := solve_block(x_curr + h_curr/2, V_mid, Vp_mid, h_curr/2, omega);

    V2_half := sol_half2[2];

   

    # Error estimate

    err := abs(V2 - V2_half) / (2^6 - 1);

   

    if err < tol then

        # Accept step

        x_next := x_curr + 2*h_curr;

        X := [op(X), x_curr + h_curr, x_next];

        V := [op(V), V1, V2];

        Vp := [op(Vp), Vp1, Vp2];

        x_curr := x_next;

        v_curr := V2;

        vp_curr := Vp2;

        printf("x = %7.4f, h = %8.5f, err = %12.5e\n", x_curr, h_curr, err);

       

        # Adjust step size

        if err < tol/2 then

            h_curr := min(2*h_curr, h_max);

        end if;

    else

        # Reject step, reduce h

        h_curr := max(h_curr/2, h_min);

        printf("  Rejecting, new h = %8.5f\n", h_curr);

    end if;

end do:

 

# Exact solution for comparison

exact := x -> 3*sin(x) - 5*cos(x);

errors := [seq(abs(V[i] - exact(X[i])), i=1..nops(X))];

 

# Visualization

p1 := pointplot([seq([X[i], errors[i]], i=1..nops(X))], color=red, symbol=circle,

                title="Example 1: Variable Step-Size TFSB - Absolute Errors",

                labels=["x", "Error"], labeldirections=[horizontal,vertical]);

p2 := plot([[x_curr, h_curr]], x=a..b, style=point, color=blue,

            title="Step-size evolution", labels=["x", "h"]);

display(p1);

display(p2);

 

printf("\nFinal results for Example 1:\n");

printf("Number of steps: %d\n", nops(X)-1);

printf("Maximum error: %e\n", max(errors));

printf("Final step-size: %f\n", h_curr);

Since Maple version 2026, I have noticed that the orientation option with the contourplot3d command has no effect.

It is easy to control by using the example provided in the online help and adding, for example, orientation=[20,10,10].

Thank you for your help.

Best regards.

On my system (Windows 11) I can only remove an entry from the favorites when a document is open. With all documents closed removing does not work.

Can someone confirm?

Color option in Context Panel does not work

Steps to Reproduce:
1. Create or open a histogram.
2. Try to change its color using the Color option in the Context Panel.
3. Observe that the color does not change.
4. Click outside the histogram.
5. Click back on the histogram.
6. Try the Color option again — now it works.

Expected Behavior:  
The Color option should work immediately when applied to the histogram, without requiring extra clicks.

Actual Behavior:  
The Color option only works after clicking outside the histogram and then reselecting it.

Just for my interest.
Why is the following not working

one := ``(1);
                           one := (1)

 lprint(`%`);
Error, Got internal error in Typesetting:-Parse:-Preprocess : "invalid subscript selector"
Typesetting:-mambiguous(Typesetting:-mambiguous( lprint(%), 

  Typesetting:-merror("Got internal error in Typesetting:-Parse:\

  -Preprocess : "invalid subscript selector"")))

but this works

lprint(one);
``(1)

I was atttempting to ask a question about I problem with styles in the editor in Maple 2026. When I attempted to upload a worksheet  showing the problem, my upload was blocked (SQL injection detected). The worksheet is question was, so far as I know, a standard Maple Worksheet containing a module in the start up code editor. How do I successfully upload a maple worksheet?

I do not understand why a once entered prompt cannot be copied from the AI pannel.

I also do not understand that a text passage from an answer (e.g. a proposed help topic) cannot be selected and copied to the clipboard with crtl-c.

It does not make sense to me to unnecessarily restrict a new program feature. This somehow spoils the show.

Is that a restriction to Windows or my local setting or something imposed on Maplesoft from a third party supplier?

Has anybody seen similar AI implementations in other products?

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