Maple Questions and Posts

How to remove the username from Maple output...

Asked by: C_R 3412

November 06 2024

1 6

On some occasions I have seen output like this

where the user name is replaced by a placeholder.
How to achieve this?

Implicitdiff(P(u,v),v,u,u) at a point u0, v0 such ...

Asked by: Jesús Guillera 75

November 06 2024

1 17

Let P(u,v) = -u⁴+88u³v-146u²v²+88uv³-v⁴+2u²+40uv+2v²-1, with P(u,v)=0,

and u0 = sqrt(2)/6 i, v0 = -sqrt(2)/6 i. We see that P(u0,v0)=0.

Direct substitution of implicitdiff(P(u,v),v,u) at u0, v0 leads to 0/0.

For obtaining the true value of dv/du at (u0,v0) we have written in Maple:

solve(limit(subs(v=v0+k*(u-u0), implicitdiff(P(u,v),v,u)), u=u0)-k, k);

There are two solutions: 49/113 - 72*sqrt(2)/113*I, and 49/113 + 72*sqrt(2)/113*I.

However we were unable to determine the true value of d²v/du² at (u0,v0).

QUESTION: How to determine it?

How to find common members...

Asked by: brian bovril 914

November 06 2024

2 4

Hi. I'm comparing two 7x3-man teams lists. I can see there are at least 2 teams that have common members, new[1] and past[4], new[4] and past[3]. There may be others but the chat gpt code below doesn't definitively find any of them.

common.mw

Library size distribution...

Asked by: Anthrazit 885

November 05 2024

3 3

The company library with all the good stuff has passed a 100 Mb size, and I wonder if it is possible to find out, which parts of the library that use most of the storage space?

Nice recursion to solve...

Asked by: Alfred_F 330

November 05 2024

0 2

After exertion with ordinary differential equations now relaxation:

Determine the formation law, limit and sum limit for
u_n+3=(13/12)*u_n+2 - (3/8)*u_n+1 + (1/24)*u_n .
Starting values u_1=0, u_2=1, u_3=1.

Introducing the Student Success Platform

by: Karishma 805 Products: Maple , Maple Calculator , Maple Learn

November 05 2024

6 2

We’re thrilled to announce the launch of our new Student Success Platform! Over the past several months, our academic team has dedicated itself to understanding how we can better support institutions in addressing their concerns around student retention rates. The numbers tell a concerning story: In the U.S., nearly 25% of first-year undergraduates don’t complete their studies, and in STEM fields, the numbers are even higher. In both STEM programs and non-STEM programs with math gateway courses, struggles with math are often a key reason students do not, or cannot, continue their studies. This has a profound impact on both the students’ futures and the institution’s revenue and funding.

From what we’re hearing from institutions and instructors, one of the most pressing issues is the lack of readiness among first-year students, particularly in math courses. With larger class sizes and students arriving with varying levels of preparedness, instructors face challenges in providing the personalized support that is essential. Additionally, many students don’t fully utilize existing resources, such as office hours or TA sessions, which increases their risk of falling behind and ultimately dropping out.

Our new Student Success Platform is designed to tackle these issues head-on. It combines all of our existing tools with exciting new features to help students succeed on their own terms—without adding to instructors' already busy workloads. The early feedback has been fantastic, and we can’t wait for you to see the impact it can make.

You can read more about the Student Success Platform here: https://www.maplesoft.com/student-success-platform/

How make a table for numerical results between exa...

Asked by: salim-barzani 1560

November 05 2024

0 2

If we calculating it take to much time but if we make a procedure it will be more effectable for such example, i want the exact and approximat and error

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laplace(y(x, t), t, s) = 1/s-laplace(diff(y(x, t), x), t, s)*x/s^2+1/s^2+laplace(diff(y(x, t), x), t, s)/s^2+2*laplace(y(x, t)^3, t, s)/s^2+laplace(y(x, t), t, s)/s^2

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for j from 0 to 3 do A[j] := subs(lambda = 0, (diff(f(seq(sum(lambda^i*u[i](x), i = 0 .. 20), m = 1 .. 2)), [`$`(lambda, j)]))/factorial(j)) end do

(12)

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y[1] := invlaplace(2*laplace(A[0], x, s)/s^2, s, x)-invlaplace(x*laplace(diff(y[0], x), x, s)/s^2, s, x)+invlaplace(laplace(y[0], x, s)/s^2, s, x)-invlaplace(laplace(diff(y[0], x), x, s)/s^2, s, x)

(15)

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y[2] := invlaplace(2*laplace(A[1], x, s)/s^2, s, x)-invlaplace(x*laplace(diff(y[1], x), x, s)/s^2, s, x)+invlaplace(laplace(y[1], x, s)/s^2, s, x)-invlaplace(laplace(diff(y[1], x), x, s)/s^2, s, x)

(1/840)*x^4*(7*x^5+63*x^4+212*x^3+476*x^2+672*x+420)-(1/60)*x^4*(x^3+6*x^2+10*x+20)+(1/420)*x^4*(x^3+7*x^2+14*x+35)-(1/60)*x^3*(x^3+6*x^2+10*x+20)

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3*(1+x)*((1/10)*x^5+(1/2)*x^4+(2/3)*x^3+x^2)^2+3*(1+x)^2*((1/120)*x^9+(3/40)*x^8+(5/21)*x^7+(7/15)*x^6+(17/30)*x^5+(1/12)*x^4-(1/3)*x^3)

(22)

>

y[3] := invlaplace(2*laplace(A[2], x, s)/s^2, s, x)-invlaplace(x*laplace(diff(y[2], x), x, s)/s^2, s, x)+invlaplace(laplace(y[2], x, s)/s^2, s, x)-invlaplace(laplace(diff(y[2], x), x, s)/s^2, s, x)

(1/10810800)*x^5*(7623*x^8+99099*x^7+518778*x^6+1634490*x^5+3647930*x^4+5167305*x^3+4221360*x^2+900900*x-1081080)-(1/25200)*x^5*(21*x^6+210*x^5+750*x^4+1680*x^3+2380*x^2+420*x-2100)+(1/831600)*x^5*(63*x^6+693*x^5+2750*x^4+6930*x^3+11220*x^2+2310*x-13860)-(1/25200)*x^4*(21*x^6+210*x^5+750*x^4+1680*x^3+2380*x^2+420*x-2100)

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1+x+(37/60)*x^5+(2/3)*x^4+(1/3)*x^3+x^2+(2351/7560)*x^9+(781/1680)*x^8+(101/210)*x^7+(53/120)*x^6+(1/7)*x^10+(1091/23100)*x^11+(11/15600)*x^13+(11/1200)*x^12

(25)

Download aproximate_and_exact_solution.mw

a table like that

How calculate Adomian polynomial by different algo...

Asked by: salim-barzani 1560

November 04 2024

0 22

there is four formula for calculate them which i know them by name of author the first one is adomian second one is (BiazarShafiofAdomian) which one member of mableprimes write code for me,but i don't know how use for all kind function maybe in future i upload this program for fix this issue, the third one is by zhao which is i think i easy for calculate just i need someone one to wite the program and do some test for some example i upload some picture in case for getting algorithm to writting and have some example for testing so lets see who can do this algorithm is very usfule when we solve ODE or PDE by LDM, also last method is by taking integral have a good method, in this question this algorithm is zhao which is usfull one

Error integrating a procedure...

Asked by: Gonzalo Garcia 155

November 04 2024

1 2

Hi!

I am using a proceure to conpute de integral of a function by he Simpson's rule. My function is defined from a function and a procedure, but I am getting the error "Error, (in w) invalid input: hfun2 expects its 1st argument, t, to be of type numeric, but received (1/10)*i+1/20"

As you can see in the attaxhed file, I have tried several ways to compute the integral but always returns the above error. Please, can yo help me?

Thanks

forum.mw

Exploring Oscillators: A Simple Pendulum Worksheet...

by: Paras31 245 Product: Maple 2024

November 03 2024

1 0

Over the last few days, I’ve been creating worksheets on oscillators to support my class’s understanding of these fundamental physics concepts. I wanted to share one of these worksheets that I found particularly useful for illustrating energy exchange and motion dynamics.

A simple pendulum is a classic physics example that exhibits periodic motion. It consists of a mass m (called a bob) attached to a string or rod of length L, which swings back and forth under the influence of gravity. When the bob is displaced from its equilibrium position and released, it swings back and forth under the influence of gravity.
To derive the equation of motion, we can examine the forces acting on the pendulum bob and use Newton’s second law.

Period of a Pendulum:

•	Frequency () the number of cycles the pendulum completes in one second. Measued in hertz (

•	Period ( the time it takes the pendulum to complete one cycle. Measued in seconds ().

This period depends only on the length and gravitational acceleration meaning it is independent of the amplitude for small oscillations.

What is the period and the frequency of a single pendulum that is 70 cm long on the earth and on the moon?

>

L := .7; g__earth := 9.8; g__moon := 1.6

(1)

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T__earth := 2*Pi*sqrt(L/g__earth); f__earth := L/T__earth

(2)

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T__moon := 2*Pi*sqrt(L/g__moon); f__moon := L/T__moon

(3)

The above image is taken from https://www.researchgate.net/publication/365297210_Scientific_counterfactuals_as_make-believe

1.	Forces on the Pendulum Bob:

The main forces acting on the bob are:

•	The gravitational forceacting vertically downward.

•	The tension in the string, acting along the string toward the pivot point.

2.	Components of the Gravitational Force:

Since the pendulum swings in an arc, it’s helpful to resolve the gravitational force into two components:

•	Radial Component (along the string): This component, is countered by the tension in the string and does not contribute to the pendulum’s motion.

•	Tangential Component (perpendicular to the string): This component, (restoring force), acts along the arc of the pendulum’s swing and is responsible for its motion.

3.	Applying Newton's Second Law Since the tangential component of the gravitational force causes the pendulum’s motion, we can apply Newton's second law in the tangential direction:

Substituting for and the tangential acceleration

where diff(s(t), t, t) = a__x and a__x = diff(x, t, t)

Now, we want to write everything in terms of θ

we obtain:

Small-Angle Approximation

For small angles (typically) , the approximation

(where is in radians) can be used. This simplifies the equation:

This equation is now in the form of a simple harmonic oscillator

where is the angular frequency of the pendulum.

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L := 1; m := .2; g := 9.8

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ODE__1 := diff(theta(t), t, t)+omega^2*theta = 0; IC := theta(0) = A, (D(theta))(0) = 0

diff(diff(theta(t), t), t)+9.799999997*theta(t) = 0

(7)

>	$sol := dsolve({IC, ODE__1}, theta(t))$

(8)

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plot_1 := subs(A = 0.873e-1, sol); plotsresult := plot([rhs(plot_1)], t = 0 .. 2, color = [red])

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`θ_t` := rhs(subs(A = 0.873e-1, sol)); v_t := diff(`θ_t`, t)

(9)

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T := (1/2)*m*L^2*v_t^2; V := m*g*L*(1-cos(`θ_t`)); H := T+V

0.7468864200e-2*sin((1/100000)*97999999970^(1/2)*t)^2

0.7468864200e-2*sin((1/100000)*97999999970^(1/2)*t)^2+1.96-1.96*cos(0.873e-1*cos((1/100000)*97999999970^(1/2)*t))

(10)

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energy_plot := plot([eval(T), eval(V), eval(H)], t = 0 .. 5, color = [red, blue, green], legend = ["Kinetic Energy", "Potential Energy", "Total Energy"], title = "Energy Exchange in Simple Pendulum", labels = ["Time (s)", "Energy (Joules)"])

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directionfield := DEplot([diff(theta(t), t) = v(t), diff(v(t), t) = -omega^2*theta(t)], [theta(t), v(t)], t = 0 .. 20, theta = -20 .. 20, v = -40 .. 40, arrows = medium, title = "Direction Field for Simple Harmonic Oscillator", axes = boxed, color = navy)

>	$sol1 := dsolve({ODE__1, theta(0) = 3, (D(theta))(0) = 0}, theta(t)); sol2 := dsolve({ODE__1, theta(0) = 6.5, (D(theta))(0) = 0}, theta(t)); sol3 := dsolve({ODE__1, theta(0) = -8, (D(theta))(0) = 0}, theta(t)); sol4 := dsolve({ODE__1, theta(0) = 9.7, (D(theta))(0) = 2.5}, theta(t))$

theta(t) = (13/2)*cos((1/100000)*97999999970^(1/2)*t)

theta(t) = (25000/9799999997)*97999999970^(1/2)*sin((1/100000)*97999999970^(1/2)*t)+(97/10)*cos((1/100000)*97999999970^(1/2)*t)

(11)

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theta1 := rhs(sol1); theta2 := rhs(sol2); theta3 := rhs(sol3); theta4 := rhs(sol4)

(13/2)*cos((1/100000)*97999999970^(1/2)*t)

(25000/9799999997)*97999999970^(1/2)*sin((1/100000)*97999999970^(1/2)*t)+(97/10)*cos((1/100000)*97999999970^(1/2)*t)

(12)

>

v1 := diff(theta1, t); v2 := diff(theta2, t); v3 := diff(theta3, t); v4 := diff(theta4, t)

-(3/100000)*97999999970^(1/2)*sin((1/100000)*97999999970^(1/2)*t)

-(13/200000)*97999999970^(1/2)*sin((1/100000)*97999999970^(1/2)*t)

(1/12500)*97999999970^(1/2)*sin((1/100000)*97999999970^(1/2)*t)

(5/2)*cos((1/100000)*97999999970^(1/2)*t)-(97/1000000)*97999999970^(1/2)*sin((1/100000)*97999999970^(1/2)*t)

(13)

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theta_at_1_sec := subs(t = 1, A = 0.873e-1, rhs(sol)); evalf(theta_at_1_sec)

(14)

Download Simple_Pendulum.mw

How to solve this equation?...

Asked by: mary120 75

November 03 2024

0 3

Hi,
I have an equation and I want to solve it parametrically to find x , but I couldn't do that with "solve" command. (I know x should be real and positive). What should I do?
Root_of.mw

How collect series solution of PDE?...

Asked by: salim-barzani 1560

November 02 2024

1 31

this example is easiest one for getting solution but i can't collect each part and do like elite i can do each part seperatly but it take to much time i want collect solution and do by easier way if possible this is a laplace adomian decomposition methd which contain adomian polynomial too i want upgrade the code, can any one help the process for get better vision of this topic
i do upload some picture and my mw. for more undrestanding

and please can any one explan why when i take laplace why is write D[2](u)(x, 0) must be D[1]?

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${laplace(u(x, t), t, s) = (s*u(x, 0)+(D[2](u))(x, 0)-laplace(u(x, t)^2, t, s)+laplace((diff(u(x, t), x))^2, t, s))/s^2}$

(6)

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${laplace(u(x, t), t, s) = (exp(x)-laplace(u(x, t)^2, t, s)+laplace((diff(u(x, t), x))^2, t, s))/s^2}$

(7)

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${u(x, t) = exp(x)*t-(int(u(x, _U1)^2*(t-_U1), _U1 = 0 .. t))+int((diff(u(x, _U1), x))^2*(t-_U1), _U1 = 0 .. t)}$

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for j from 0 to 3 do A[j] := subs(lambda = 0, (diff(f(seq(sum(lambda^i*u[i](x, t), i = 0 .. 20), m = 1 .. 2)), [`$`(lambda, j)]))/factorial(j)) end do

(13)

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for j from 0 to 3 do B[j] := subs(lambda = 0, (diff(f(seq(sum(lambda^i*u[i](x, t), i = 0 .. 20), m = 1 .. 2)), [`$`(lambda, j)]))/factorial(j)) end do

(17)

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"#` know we need find all term of u[0]=exp(x)*t` #` u`[1]=-invlaplace(1/(s^(2))(`A__0`+`B__0`)) u[2]=-invlaplace(1/(s^(2))(`A__1`+`B__1`)) ans so on ... at end i want collect all of them and find final result even if is aproximate and want do test of pde too "

>

NULL

Download explananing_of_get_solution.mw

Typesetting internal error when Physics update is ...

Asked by: nm 11353

November 02 2024

0 3

[moderator: The Physics update Library fixes this bug with the same error generated and reported by the same Mapleprimes member on another ODESteps example.]

I have removed Physics update from libname path.

Now I find I get error calling latex command. When Physics update is on libname, no error.

The error is

Error, (in Typesetting:-Parse) too many levels of recursion

I am using worksheet with typesetting extended. But also when I change it to typesetting standard, same error.

Does this mean one must keep Physics update on libname path for Maple to work OK?

Is this error expected if Physics update is not on libname?

Worksheet below that shows this problem

>

restart;

>	interface(version);

CASE 1. With Physics update in libname path, no error

>

restart;

>

libname;

$"C:\Users\Owner\maple\toolbox\2024\Physics Updates\lib", "C:\Program Files\Maple 2024\lib"$

>	ode:=[diff(x__1(t),t)=2x__1(t)+x__2(t),diff(x__2(t),t)=2x__1(t)+3*x__2(t)];

>	the_output:=Student:-ODEs:-ODESteps(ode,output=typeset):

>	latex(the_output,'output'=string):

>

CASE 2. Removing Physics from libname path, gives internal error

>

restart;

>	libname:=libname[2];

$"C:\Program Files\Maple 2024\lib"$

>	ode:=[diff(x__1(t),t)=2x__1(t)+x__2(t),diff(x__2(t),t)=2x__1(t)+3*x__2(t)];

>	the_output:=Student:-ODEs:-ODESteps(ode,output=typeset):

>	latex(the_output,'output'=string):

Error, (in Typesetting:-Parse) too many levels of recursion

>

Download internal_error_from_latex_when_libname_changed_nov_2_2024.mw

plotting numerically solved PDE at specific range ...

Asked by: alfarunner 90

November 02 2024

0 1

it's easy to plot a numeric solution of a pde, e.g u(x,t) at a specific time but it's more difficult to plot a solution for a specific x-value as a function of time. How do I do that in Maple?

I find an error...

Asked by: Yuri Zamorano 30

November 01 2024

0 1

I find an error when calculating ExponentialFit(X, Y, x, summarize = embed) function. It's have an error in R-squared and Adjusted R-squared.

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