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I would like to express 2*sin(x+Pi/4) in the form sqrt(2)*sin(x)+sqrt(2)*cos(x). I've tried many variations using simplify/expand/combine/etc. to no avail. Any ideas?

I have the  following simple code in Maple:

x:=2*y

save x, "file1.mpl";

This code works successfully in Maple 13 and 14. However, does not work in Maple 17.  I do not understand why this happens. Can anyone help me to save a procedure in Maple 17.

 

Dear Experts,

When I run this code in maple I am facing with "Error, (in dsolve/numeric/bvp) initial Newton iteration is not converging".

restart:
 
 unprotect('gamma');
 lambda:=5*10^5:
 mu:=0.003:
 beta:=4*10^(-10):
 delta:=0.2:
 alpha:=0.043:
 sigma:=alpha+delta:
 k:=6.24:
 gamma:=0.65:
 A[1]:=1:
 A[2]:=1:

ics := x[1](0)=1.7*10^8, x[2](0)=0,x[3](0)=400,psi[1](50)=0,psi[2](50)=0,psi[3](50)=0:

ode1:=diff(x[1](t), t)=lambda-mu*x[1](t)-(1-beta*x[1](t)*x[3](t)*(psi[1](t)-psi[2](t))/A[1])*beta*x[1](t)*x[3](t)+delta*x[2](t),
 diff(x[2](t), t) =(1-beta*x[1](t)*x[3](t)*(psi[1](t)-psi[2](t))/A[1])*beta*x[1](t)*x[3](t)-sigma*x[2](t),
 diff(x[3](t), t) =(1+psi[3](t)*k*x[2](t)/A[2])*k*x[2](t)-gamma*x[3](t),
 diff(psi[1](t), t) =-1+1/A[1]*beta^2*x[1](t)*x[3](t)^2*(psi[1](t)-psi[2](t))^2-psi[1](t)*(-mu+beta^2*x[3](t)^2*(psi[1](t)-psi[2](t))/A[1]*x[1](t)-(1-beta*x[1](t)*x[3](t)*(psi[1](t)-psi[2](t))/A[1])*beta*x[3](t))-psi[2](t)*(-beta^2*x[3](t)^2*(psi[1](t)-psi[2](t))/A[1]*x[1](t)+(1-beta*x[1](t)*x[3](t)*(psi[1](t)-psi[2](t))/A[1])*beta*x[3](t)),
> diff(psi[2](t), t) =1/A[2]*psi[3](t)^2*k^2*x[2](t)-psi[1](t)*delta+psi[2](t)*sigma-psi[3](t)*(psi[3](t)*k^2/A[2]*x[2](t)+(1+psi[3](t)*k*x[2](t)/A[2])*k),
> diff(psi[3](t), t) = 1/A[1]*beta^2*x[1](t)^2*x[3](t)*(psi[1](t)-psi[2](t))^2-psi[1](t)*(beta^2*x[1](t)^2*(psi[1](t)-psi[2](t))/A[1]*x[3](t)-(1-beta*x[1](t)*x[3](t)*(psi[1](t)-psi[2](t))/A[1])*beta*x[1](t))-psi[2](t)*(-beta^2*x[1](t)^2*(psi[1](t)-psi[2](t))/A[1]*x[3](t)+(1-beta*x[1](t)*x[3](t)*(psi[1](t)-psi[2](t))/A[1])*beta*x[1](t))+psi[3](t)*gamma;

sol:=dsolve([ode1,ics],numeric, method = bvp[midrich]);

Error, (in dsolve/numeric/bvp) initial Newton iteration is not converging

Please help me to solve this equation on Maple.




Hello,

I understand that the question is not really Maple related, but I still hope for some help.


See the worksheet below. I defined a pure sine wave and determined the complex Fourier coefficients for it which I used to plot the amplitude and power spectra. It is easy to see the relations in terms of amplitude and power between the time and frequency signal.

The Fourier Transform of the sine wave logically shows the Dirac distribution, but I can't see the relation in terms of amplitude and power to the original time signal. Taking the integral of the transformed signal (A) wil result in a step of Pi at w=-1 and again at w=1. What am I missing here?

Thanks

restart; with(inttrans); with(plots); with(DynamicSystems)

 

Define a signal:

 

T := 2*Pi;

2*Pi

 

sin(t)

(1)

 

Determine the waveform power:

 

F := (int(f^2, t))/T+C:

C := simplify(solve(subs(t = 0, F) = 0, C)):

eval((int(f^2, t = -(1/2)*T .. (1/2)*T))/T)

1/2

(2)

plot([f, f^2, F], t = -Pi .. Pi, gridlines = true)

 

 

Determine the complex Fourier series coefficients and plot the spectra:

 

q := proc (n) options operator, arrow; (int(f*exp(-(2*I)*n*Pi*t/T), t = -(1/2)*T .. (1/2)*T))/T end proc:

simplify(q(n))

I*sin(Pi*n)/(Pi*(n^2-1))

(3)

ComplexCoefficients := evalf(`<,>`(seq(q(n), n = -1 .. 1)))

ComplexCoefficients := Vector(3, {(1) = .5000000000*I, (2) = 0., (3) = -.5000000000*I})

(4)

B := evalf(`<,>`(seq(sqrt(Re(q(n))^2+Im(q(n))^2), n = -3 .. 3))):

 

C := evalf(`<,>`(seq(Re(q(n))^2+Im(q(n))^2, n = -3 .. 3))); -1; DiscretePlot(C, -3, 1, titlefont = ["ARIAL", "bold", 14], title = "Power Spectrum", color = "Red", gridlines = true, style = stem)

 

So, the signal power for f of 1/2 can be found directly within the power spectrum plot "(2*1/(4))."

 

I would expect to be able to directly see the amplitude and power relation to the time signal from the Fourier Transform of f but i can't.

 

A := fourier(f, t, w);

I*Pi*(Dirac(w+1)-Dirac(w-1))

(5)


Download 20140127MaplePrime.mw

 

 

I have to solve a system composed of a mass, a spring and a damper, represented by this equation :

m (d2x/dt2) + c (dx/dt) + k x(t) = F(t)

with m the mass, t the time, c the constant of the damper, k the constant of the spring, F an external force applied to the mass and x(t) the movement of the mass m at time t.

Please help me to solve this equation on Maple.

I am using Maple worksheets in a class. I have a student who finds it difficult to spend much time at the keyboard because of a joint disorder. I am looking for alternate input methods such as Dragon or the Dictate Facility on MacBooks which might help her out. Any suggestions would be appreciated. 

Thanks,

-Maury

Can anyone tell me how to use dsolve to find the solution to the problem in the attachment.  It is faily easy to do using substitution for homogeneous coefficients, but dsolve seems to put out a very complicated solution to the problem.

with(DEtools):

2*x*y(x)+(x^2+y(x)^2)*(diff(y(x), x))

2*x*y(x)+(x^2+y(x)^2)*(diff(y(x), x))

(1)

dsolve(%)

y(x) = ((1/2)*(4+4*(4*x^6*_C1^3+1)^(1/2))^(1/3)-2*x^2*_C1/(4+4*(4*x^6*_C1^3+1)^(1/2))^(1/3))/_C1^(1/2), y(x) = (-(1/4)*(4+4*(4*x^6*_C1^3+1)^(1/2))^(1/3)+x^2*_C1/(4+4*(4*x^6*_C1^3+1)^(1/2))^(1/3)-((1/2)*I)*3^(1/2)*((1/2)*(4+4*(4*x^6*_C1^3+1)^(1/2))^(1/3)+2*x^2*_C1/(4+4*(4*x^6*_C1^3+1)^(1/2))^(1/3)))/_C1^(1/2), y(x) = (-(1/4)*(4+4*(4*x^6*_C1^3+1)^(1/2))^(1/3)+x^2*_C1/(4+4*(4*x^6*_C1^3+1)^(1/2))^(1/3)+((1/2)*I)*3^(1/2)*((1/2)*(4+4*(4*x^6*_C1^3+1)^(1/2))^(1/3)+2*x^2*_C1/(4+4*(4*x^6*_C1^3+1)^(1/2))^(1/3)))/_C1^(1/2)

(2)

NULL

 

Download DEprob.mw

I have 2 problem with my jacobian matrix:

first: i can not evaluate 11*11 jacobian matrix. at last i can evaluate 10*10 matrix. can i solve this?
second: i want to export my matrix for matlab but i see this error : {export matrix"cannot convert matrix element to float[8] data type"}
so how i can use this matrix in my matlab code?
 my jacobian matrix:


with(VectorCalculus); Jacobian([VectorCalculus:-`+`(VectorCalculus:-`+`(VectorCalculus:-`+`(VectorCalculus:-`*`(2.68, ex), VectorCalculus:-`-`(VectorCalculus:-`*`(2, vx))), VectorCalculus:-`*`(VectorCalculus:-`*`(VectorCalculus:-`*`(VectorCalculus:-`*`(VectorCalculus:-`*`(3.500000001, e^VectorCalculus:-`*`(1.666666667, sqrt(VectorCalculus:-`+`(VectorCalculus:-`-`(VectorCalculus:-`+`(sqrt(VectorCalculus:-`+`(rx^2, ry^2)), sqrt(VectorCalculus:-`+`(VectorCalculus:-`+`(rx, VectorCalculus:-`-`(VectorCalculus:-`*`(2, vb(ex))))^2, VectorCalculus:-`+`(ry, VectorCalculus:-`-`(VectorCalculus:-`*`(2, vb(ey))))^2)))^2), VectorCalculus:-`-`(VectorCalculus:-`*`(4, vb^2)))))), VectorCalculus:-`+`(sqrt(VectorCalculus:-`+`(rx^2, ry^2)), sqrt(VectorCalculus:-`+`(VectorCalculus:-`+`(rx, VectorCalculus:-`-`(VectorCalculus:-`*`(2, vb(ex))))^2, VectorCalculus:-`+`(ry, VectorCalculus:-`-`(VectorCalculus:-`*`(2, vb(ey))))^2)))), VectorCalculus:-`+`(VectorCalculus:-`*`(rx, 1/sqrt(VectorCalculus:-`+`(rx^2, ry^2))), VectorCalculus:-`*`(1/2, VectorCalculus:-`*`(VectorCalculus:-`+`(VectorCalculus:-`*`(2, rx), VectorCalculus:-`-`(VectorCalculus:-`*`(4, vb(ex)))), 1/sqrt(VectorCalculus:-`+`(VectorCalculus:-`+`(rx, VectorCalculus:-`-`(VectorCalculus:-`*`(2, vb(ex))))^2, VectorCalculus:-`+`(ry, VectorCalculus:-`-`(VectorCalculus:-`*`(2, vb(ey))))^2)))))), ln(e)), 1/sqrt(VectorCalculus:-`+`(VectorCalculus:-`-`(VectorCalculus:-`+`(sqrt(VectorCalculus:-`+`(rx^2, ry^2)), sqrt(VectorCalculus:-`+`(VectorCalculus:-`+`(rx, VectorCalculus:-`-`(VectorCalculus:-`*`(2, vb(ex))))^2, VectorCalculus:-`+`(ry, VectorCalculus:-`-`(VectorCalculus:-`*`(2, vb(ey))))^2)))^2), VectorCalculus:-`-`(VectorCalculus:-`*`(4, vb^2)))))), VectorCalculus:-`*`(VectorCalculus:-`*`(VectorCalculus:-`*`(VectorCalculus:-`*`(50.00000000, e^VectorCalculus:-`-`(VectorCalculus:-`*`(5.000000000, sqrt(VectorCalculus:-`+`(Rx^2, Ry^2))))), Rx), ln(e)), 1/sqrt(VectorCalculus:-`+`(Rx^2, Ry^2)))), VectorCalculus:-`+`(VectorCalculus:-`+`(VectorCalculus:-`+`(VectorCalculus:-`*`(2.68, ey), VectorCalculus:-`-`(VectorCalculus:-`*`(2, vy))), VectorCalculus:-`*`(VectorCalculus:-`*`(VectorCalculus:-`*`(VectorCalculus:-`*`(VectorCalculus:-`*`(3.500000001, e^VectorCalculus:-`*`(1.666666667, sqrt(VectorCalculus:-`+`(VectorCalculus:-`-`(VectorCalculus:-`+`(sqrt(VectorCalculus:-`+`(rx^2, ry^2)), sqrt(VectorCalculus:-`+`(VectorCalculus:-`+`(rx, VectorCalculus:-`-`(VectorCalculus:-`*`(2, vb(ex))))^2, VectorCalculus:-`+`(ry, VectorCalculus:-`-`(VectorCalculus:-`*`(2, vb(ey))))^2)))^2), VectorCalculus:-`-`(VectorCalculus:-`*`(4, vb^2)))))), VectorCalculus:-`+`(sqrt(VectorCalculus:-`+`(rx^2, ry^2)), sqrt(VectorCalculus:-`+`(VectorCalculus:-`+`(rx, VectorCalculus:-`-`(VectorCalculus:-`*`(2, vb(ex))))^2, VectorCalculus:-`+`(ry, VectorCalculus:-`-`(VectorCalculus:-`*`(2, vb(ey))))^2)))), VectorCalculus:-`+`(VectorCalculus:-`*`(ry, 1/sqrt(VectorCalculus:-`+`(rx^2, ry^2))), VectorCalculus:-`*`(1/2, VectorCalculus:-`*`(VectorCalculus:-`+`(VectorCalculus:-`*`(2, ry), VectorCalculus:-`-`(VectorCalculus:-`*`(4, vb(ey)))), 1/sqrt(VectorCalculus:-`+`(VectorCalculus:-`+`(rx, VectorCalculus:-`-`(VectorCalculus:-`*`(2, vb(ex))))^2, VectorCalculus:-`+`(ry, VectorCalculus:-`-`(VectorCalculus:-`*`(2, vb(ey))))^2)))))), ln(e)), 1/sqrt(VectorCalculus:-`+`(VectorCalculus:-`-`(VectorCalculus:-`+`(sqrt(VectorCalculus:-`+`(rx^2, ry^2)), sqrt(VectorCalculus:-`+`(VectorCalculus:-`+`(rx, VectorCalculus:-`-`(VectorCalculus:-`*`(2, vb(ex))))^2, VectorCalculus:-`+`(ry, VectorCalculus:-`-`(VectorCalculus:-`*`(2, vb(ey))))^2)))^2), VectorCalculus:-`-`(VectorCalculus:-`*`(4, vb^2)))))), VectorCalculus:-`*`(VectorCalculus:-`*`(VectorCalculus:-`*`(VectorCalculus:-`*`(50.00000000, e^VectorCalculus:-`-`(VectorCalculus:-`*`(5.000000000, sqrt(VectorCalculus:-`+`(Rx^2, Ry^2))))), Ry), ln(e)), 1/sqrt(VectorCalculus:-`+`(Rx^2, Ry^2)))), 1, 1, 1, 1, 1, 1, 1, 1, 1], [vx, vy, ex, ey, rx, ry, Ex, Ey, vb, Rx, Ry])

THE FOLLOWING CODE 

restart;

A:=Matrix([[ a , b ], [ c , d ]]);

a:=1; b:=0; c:=0; d:=1;

A; 

produces differents results under MAPLE 16  linux i386 and under MAPLE 16  linux amd64

in the first case the last evalution has the following printed output:

Matrix([[a,b],[c,d]])

on the second machine the printed output is

Matrix([[1,0],[0,1]])

Does anybody has an explication; I thought that the "coorect behaviour was the first one since tables use last-name evalutation. But now I am puzzled.

 

how to decompose a matrix into time invariant and time variant 

is it possible to make time invariant and time variant template and then decompose into it

 

i mean decomposition can be 

 time invariant matrix + time variant matrix

or

 time invariant matrix * time variant matrix

 dsolve([Diff(f, t) = f, Diff(f,t) + g = h], f);

 dsolve([Diff(f, t) = f, Diff(f,t)*g = h], f);

where h is orthogonal matrix, f,g,h are matrix

would like to find g and f from h

 

can dsolve solve differential equation of matrix ? how?

 

dsolve([Diff(f(t), t) = f(t), Diff(f(t),t) + g(t) = h1(x)*h2(x), int(h1(x)*h2(x),x=-1..1) = 0], [f(t),g(t),h1(x),h2(x)]);


dsolve([Diff(f(t), t) = f(t), Diff(f(t),t)*g(t) = h1(x)*h2(x), int(h1(x)*h2(x),x=-1..1) = 0], [f(t),g(t),h1(x),h2(x)]);

 

assume x^2 + 1 is from interpolation of polynomial

pdsolve([Diff(f(t), t) = f(t), Diff(f(t),t) + g(t) = h1(x,t)*h2(x,t), h1(x,t)*h2(x,t)= x^2+1], [f(t),g(t),h1(x,t),h2(x,t)]);
pdsolve([Diff(f(t), t) = f(t), Diff(f(t),t)*g(t) = h1(x,t)*h2(x,t), h1(x,t)*h2(x,t) = x^2+1], [f(t),g(t),h1(x,t),h2(x,t)]);

these system can not be solved

 

hope no real number any more after decomposition and only have iinteger in I time invariant function

The matrix:

<3,-2,-1,2,0>;

<11,4,-8,2,7>;

<0,0,2,0,0>;

<3,3,-4,3,3>;

<-8,4,5,-4,-1>;

 

has eigenvector:

<2,0,-1,0,1>

 

Find its corresponding eigenvalue.

(Hint: you don't need to find all the eigenvalues and eigenvectors to answer this question.)

 

Steps and the solution will be greatly appreciated. thanks!

number10:=`466d06ece998b7a2fb1d464fed2ced7641ddaa3cc31c9941cf110abbf409ed39598005b3399ccfafb61d0315fca0a314be138a9f32503bedac8067f03adbf3575c3b8edc9ba7f537530541ab0f9f3cd04ff50d66f1d559ba520e89a2cb2a83`:

number8:=`315c4eeaa8b5f8bffd11155ea506b56041c6a00c8a08854dd21a4bbde54ce56801d943ba708b8a3574f40c00fff9e00fa1439fd0654327a3bfc860b92f89ee04132ecb9298f5fd2d5e4b45e40ecc3b9d59e9417df7c

I first define

f:=x->convert(x, decimal, hex):

with(Bits):
str1:=convert( `Xor(f(number8), f(number10))`, bytes);

now how can I get back the alphabets, since again use of convert with bytes return the inital argument.

Moreover, I would really appreciate if someone could explain the difference between 

convert(`expr`, bytes)

convert( [expr], bytes)

 

Many regards!!

 

if kernel is solve(A*x, x);

then , what is cokernel of a numeric matrix ?

I'd like to pay attention to an application "Periodicity of Sunspots " by Samir Khan, where a real data is analysed. That application can be used in teaching statistics.

PS. The code by Samir Khan works well for me.

Hi everyone

I am currently trying to make my own simple package including a few procedures. So far I have been able to write some "code" that actually works when I open the document and hit "enter". I would, however, like to save the package so it can be accessed during any Maple session using the command "with". I have unsuccesfully tried to comprehend the Maple help pages regarding this question but I definitely don't want to mess things up.

This is what I have written:

mat := module ()
description "useful procedures for mathematics, physics and chemistry";
export AtomicWeight;
option package;

   AtomicWeight := proc (x) description "returns the average atomic mass of the naturally ocurring element";
   Units:-AddSystem(NewSystem, Units:-GetSystem(SI), u);
   return evalf(ScientificConstants:-Element(x, atomicweight, system = NewSystem, units))
   end proc

end module;

What should I do to save it correctly?

Thank in advance,
Mads


 

 

 

 

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