Is there information available about the improvements made up to the recent version of the Maple Physics Package?

Is there any way in maple to solve this to give answer back to plaintext from cipher-text.

toletter := proc (num) local cs, cn, sl, ltable, ans, ii; ltable := table([0 = "A", 1 = "B", 2 = "C", 3 = "D", 4 = "E", 5 = "F", 6 = "G", 7 = "H", 8 = "I", 9 = "J", 10 = "K", 11 = "L", 12 = "M", 13 = "N", 14 = "O", 15 = "P", 16 = "Q", 17 = "R", 18 = "S", 19 = "T", 20 = "U", 21 = "V", 22 = "W", 23 = "X", 24 = "Y", 25 = "Z"]); cn := num; sl := floor((1/2)*trunc(evalf(log10(cn))))+1; ans := " "; for ii to sl do cn := (1/100)*cn; cs := ltatble[100*frac(cn)]; ans := cat(cs, ans); cn := trunc(cn) end do; RETURN(ans) end proc

This is because of the answer that I get is not in letter form:

toletter(plaintext);
(ltatble[17]) || (ltatble[4]) || (ltatble[19]) || (ltatble[20]) || 

  (ltatble[17]) || (ltatble[13]) || (ltatble[19]) || (ltatble[14]

  ) || (ltatble[12]) || (ltatble[0]) || (ltatble[8]) || (ltatble[

  13]) || (ltatble[3]) || (ltatble[4]) || (ltatble[2]) || (

  ltatble[10]) || " "
 

Is there any way in maple to solve this;

diff(theta(eta), eta, eta)+Pr*f*(diff(theta(eta), eta)) = 0

To find the value of theta.

theta.mw

i've come across a confusing behavior where the same command (a copy/paste of another command) is giving an output in a a different form.

Attaching a screen shot that shows this. Eq 6.8 is executed just after 6.7.

(i know the command is weird, i.e. subs(beta=beta, ..), etc.. this is part of some larger code base and i just put this in when trying to undertand what's going on).

I would hope for the same command to spit out the same output in this case. (nothing else gets assigned/called in betwen).

any idea what's going on?

i'm on maple 2018.2 on linux.

thanks

I vaguely recall others complain about disappearing Code Edit Regions. Does anyone else recall that? I had one disappear from the very top of the attached worksheet (right after the restart), causing me to lose about 15-30 minutes of work. I've totally recreated the work, so I have no interest in this worksheet being repaired. I'm merely posting it in case anyone wants to do an autopsy on it.

Another issue that happened twice with this worksheet is that when I unchecked the "Expanded" box on the Code Edit Region menu (pull out from the right side of the screen) and copied the text to my clipboard (for posting on MaplePrimes), that copied text was missing my most-recent changes to the code. They reappeared when I expanded again. (But it's really difficult to copy-and-paste a multi-screen Code Edit Region when it's expanded.)

My final issue (and this has bothered me for years), is how the heck are you supposed to find the line with the syntax error in a several-hundred-line Code Edit Region? Unlike with inline code, the cursor is not placed near the error location._Binomial_missing_Code_region.mw

How do I remove infinity from a list

s:=[f(x) , exp(a), GAMMA(2x)-1 , infinity , 1, -infinity]

remove(has,%,infinity)

does not work.

It should yield

s:=[f(x) , exp(a), GAMMA(2x)-1 , 1]

How to solve the following second order ODE system? (I want to solve analytically and numerically and to compare the results) Thanks. Best regards.

where

Initial conditions:

Other symbols in the equation (v_0,a_0 etc.) are constant.

MY CODE TRY:  Code.mw

I tried to write a code for matrices in the question. ( I used x instead of gamma in the code)

restart:
n:=2:
  M:= tau -> Matrix
      ( n,
        n,
        shape=identity
      )
      +Matrix
      ( n,
        n,             (i,j)->2*x*sin(i*Pi*v_0*tau)*sin(j*Pi*v_0*tau)
            ):
  C:=tau -> Matrix
              ( n,
                n,
                (i,j)->4*(i*Pi*v_0*tau)*sin(i*Pi*v_0*tau)*cos(j*Pi*v_0*tau)
              ):
  K:=tau -> n^4*Pi^2* Matrix
      ( n,
        n,
        shape=identity
      )-Matrix
      ( n,
        n,
        (i,j)-> 2*mu*(i*Pi*v_0)^2*sin(i*Pi*v_0*tau)*sin(j*Pi*v_0*tau)+2*mu*(i*Pi*a_0)*sin(i*Pi*v_0*tau)*cos(j*Pi*v_0*tau)
      ):
f:=tau -> Vector
      ( n,
        (i,j)-> x*Pi^2*(Pi/2+v_0^2*sum(((1-(-1)^k)/k^3)*sin(k*Pi*v_0*tau),k=1..infinity)-a_0*sum(((1-(-1)^k)/k^4)*cos(k*Pi*v_0*tau),k=1..infinity))*sin(i*Pi*v_0*tau)
      ):
      
 
X:= Vector(n, i-> x[i](t)): 
sys:= M(tau).diff~(X, tau$2)+C(tau).diff~(X, tau)+K(tau).X=f(tau):

how I can determined time period?

thank you

period.mw
 

Download period.mw

How can we solve the following pde by Maple? 

where v is velocity, v with dot is acceleration. (So, I think we will assume that acceleration is fixed.) And \delta is Dirac distribution.  E,I,m, M , g are fixed numbers.

Boundary conditions are:

Initial conditions are:

You can find the equation in the code: question.mw

Hi,

this "sum(1/(1+x)^t, t=1..infinity)" is (in my opionon) one of the most standard infinity summation and has the closed form 1/x. 
i used maple 18 and it was executed and i got the closed form 1/x.

with maple 2018 i get the non executed form, also the same inert form as "Sum(1/(1+x)^t, t=1..infinity)".

if i try "sum(1/(1+2)^t, t=1..infinity)" i get 1/2 as result.

why does the version above not working? any ideas?

thank you.

Dear friends,

I'm trying to solve a linear system of PDEs. After applying the casesplit command Maple returns: 

diff(U, z, y, x, x) = 0; diff(G, y,y,z) = diff(U,x,y,z);  diff(G,x,y,z) = diff(U,x,x,z)     

(with U(x,y,z), G(x,y,z)) 

The solution to the first equation is U = F4(x, y)+ F3(x, z) + F2(y, z) + x*F1(y, z). 

However, given this solution, I cannot satisfy diff(G,x,y,z) = diff(U,x,x,z).  What could I be doing wrong? 

Many thanks for your help.  

Hi

I have a problem with my maple. 

corrupt file 

Is there anybody who can help me solve this problem. 

Casper