System integration is defined in engineering as the process of bringing together the component sub-systems into one system (an aggregation of subsystems cooperating so that the system is able to deliver the overarching functionality) and ensuring that the subsystems function together as a system, and in information technology as the process of linking together different computing systems and software applications physically or functionally, to act as a coordinated whole.
The system integrator integrates discrete systems utilizing a variety of techniques such as computer networking, enterprise application integration, business process management or manual programming.System integration involves integrating existing, often disparate systems in such a way "that focuses on increasing value to the customer" (e.g., improved product quality and performance) while at the same time providing value to the company (e.g., reducing operational costs and improving response time). In the modern world connected by Internet, the role of system integration engineers is important: more and more systems are designed to connect, both within the system under construction and to systems that are already deployed.
Can someone please tell me the book that contain integration using hyperbolic substitution for beginner?
I know that hyperbolic functions is taught in Calculus book but most of them is only some identities and inverses of hyperbolic functions.
Thought it could be fun to have a sort of "PF Integral Bee"... if you know some interesting/quirky/etc. integrals then post them here! 🤓
To get the ball rolling...
1. ##\displaystyle{\int_0^1} \dfrac{\ln{(x+1)}}{x^2+1} dx##
$$x(t)=\int \dot{x}(t)\mathrm dt=vt+c$$
That's what I did. But, book says
$$x(t)=\int \dot{x}(t)\mathrm dt=x_0+v_0 t+ \frac{F_0}{2m}t^2$$
Seems like, $$x_0 + \dfrac{a_0}{2}t^2$$ is constant. How to find constant is equal to what?
My trial :
I think ## \int ~ dy ~ e^{-2 \alpha(y)} ## dose not simply equal: ## - \frac{1}{2}e^{-2 \alpha(y)} ## cause ##\alpha## is a function in ##y ##.
So any help about the right answer is appreciated!
I realized I never actually derived the kinematic equations of motion for the exact Newtonian gravitational force. For an object falling near the surface of the earth, how do we handle integrating the equation of motion to derive the kinematics equations without using the approximation of...
Does anyone have experience with such strange behavior in Monte-Carlo methods? I think it is a conceptional problem and I am just missing a key point in how to set up the integration instead of a error in my code itself. I use data files from LHAPDF and also checked that my variables give the...
I'm going to type out my LaTeX solution later on. But in the meantime, can anyone check my work? I know it's sloppy, disorganized, and skips far more steps than I care to count, but I'd very much appreciate it. I'm not getting the answer as given in the book. I think I failed this time because I...
If I have a force that behaves according to the formula ##F(x)=\alpha x-\beta x^3##, how can I get the potential energy from it? I know that:
$$-\frac{\mathrm{d}V(x)}{\mathrm{d}x}=F(x),$$
but what about the limits of the integration?
I’ve always struggled with integration and I don’t know how to do this question, I’m not sure what I’m being asked to calculate. I tried to calculate this as a definite integral but there is no boundary conditions for the distance the object has traveled which is confusing any help would be...
Greetings
While solving the following exercice, ( the method used is the integration by filaments and I have no problem doing it this way)
here is the solution
My question is the following:
I want to do the integration by strate and here is my proposition
is that even correct?
I would like...
Greetings!
As mentionned my aim is to change the order of integral, and I totally agree with the solution I just have one question:
as you can see they have put
0<=y<=1 and 0<=x<=y^2
but would it be wrong if I put
0<=y<=1 and y^2<=x<=1?
Thank you!
I'm trying to pass through some parameters of a function to the gsl integration routine but my code is currently not returning correct values. I attach a version of my code using dummy example functions and names.
struct myStruct_t {
double a;
};
double func(double z, void* params)...
I simply plugged \phi = \phi_0 (\eta) + \delta \phi (\eta, \vec x) into the given action to get
\begin{align}
S &= \int d^4 x \left[ \frac{a^2}{2}\left(\dot \phi^2 -(\nabla \phi)^2\right)-a^4V(\phi) \right] \nonumber \\
&= \int d^4 x \left[ \frac{a^2}{2}\left(\dot \phi_0^2 + (\delta...
First, I calculated the inverse of ##y=e^x## since we're talking about y-axis rotations, which is of course ##x=lny##.
Then, helping myself out with a drawing, I concluded that the total volume of the solid must've been:
$$V=\pi\int_{0}^{1}1^2 \ dy \ +(\pi\int_{1}^{e}1^2 \ dy \ - \pi...
I was trying to look for something that works a lot of examples of integrals over surfaces, volumes etc. in general relativity. Tong's notes and some others are good on the abstract/theoretical side but it'd really be better at this stage to get some practice with concrete examples in order to...
There's an integral over a 2-sphere ##S## with unit normal ##N^a## within a hypersurface orthogonal to a Killing field ##\xi^a##$$F = \int_S N^b (\xi^a / V) \nabla_a \xi_b dA = \frac{1}{2} \int_S N^{ab} \nabla_a \xi_b dA, \quad N^{ab} := 2V^{-1} \xi^{[a} N^{b]}$$which follows because the Killing...
I began this solution by assuming a = x+iy since a is a complex number.
So I wrote expressions of <a| and |a> in which |n><n| = I.
I got the following integral:
Σ 1/πn! ∫∫ dx dy exp[-(x^2 + y^2)] (x^2 + y^2)^n I
I tried solving it using Integration by Parts but got stuck in the (x^2 + y^2)^n...
Split the integral
$$\frac{Aa}{\sqrt{2\pi}}\int^{\infty}_{-\infty}e^{ikx}dk - \frac{A}{\sqrt{2\pi}}\int^{\infty}_{-\infty}|k|e^{ikx}dk$$
Apply the boundary conditions, this is where my biggest source of uncertainty comes from I doubled the integral and integrated from 0 to a instead of from -a...
Hi I'm having troubles with integration specially by substitution, I'm going to read a calculus textbook and i need recommendations of books with a good treatment on the different techniques of integration. I'd like a book with good exercises for self study and a exposure to integration of...
Is it possible to do the integration? That is the full question
I don't know where to start, try to use ##u=\cos x## and also ##\cos^2 (x) = \frac{1}{2} + \frac{1}{2} \cos (2x)## but failed.
Thanks
Good day !
I have a problem with the solution of the floowing integrals
Indeed i don't understand why they choose such borders for integral
b/a<c
y<c
doesn't mean that y<b/a !
many thanks in advance!
As we all know, integration by parts can be defined as follows: $$\int u dv = uv - \int v du$$ And the usual strategy for solving problems of these types is to intelligently define ##u## and ##dv## such that the RHS integral can easily be evaluated. However, something that is never addressed is...
This question arose while studying Cosmology (section 38.2 in Lecture Notes in GR) but it is purely mathematical, that is why I ask it here.
I do not see why the equation
$$H^2 = H_0^2 \left[\left( \frac{a_0}{a}\right)^3 (\Omega_M)_0 + (\Omega_{\Lambda})_0 \right] \tag{1}$$
Has the following...
In Griffith’s section 10.3.1, when proving why there is an extra factor in integrating over the charge density when it depends on the retarded time, he makes the argument that there can only ever be one point along the trajectory of the particle that “communicates” with the field point. Because...
I am reading a proof in Feedback Systems by Astrom, for the Bode Sensitivity Integral, pg 339. I am stuck on a specific part of the proof.
He is evaluating an integral along a contour which makes up the imaginary axis. He has the following:
$$ -i\int_{-iR}^{iR}...
I can calculate the value of the integration, it will be ##\frac{\sqrt{3}}{2}##
But if I draw the function and consider the area bounded by the curve and x-axis from x = 0.5 to x = 1, it seems that the area will be infinite because x = 1 is vertical asymptote.
Why can't I consider from "area...
my thinking was to have everything changed to a function that has cosine only...
##\int_0^{0.5π} \frac {1-cos^2x}{sin x + cos x}dx##
##\int_0^{0.5π} \frac {(1-cos x)(1+cos x)}{(1-cos^2x)^{0.5} + cos x}dx## ...
first of all is this integration possible? if so then let me know if i am on the...
So I am confused about a proof in which the formula for expected value of velocity, ##\frac{d\langle x \rangle}{dt} ##, is derived.
Firstly, because the expected value of the position of wave function is $$\langle x \rangle =\int_{-\infty}^{+\infty} x|\Psi(x,t)|^2 dx$$Therefore...
Hello,
I would like to is it possible to solve such a differential equation (I would like to know the z(x) function):
\displaystyle{ \frac{z}{z+dz}= \frac{(x+dx)d(x+dx)}{xdx}}
I separated variables z,x to integrate it some way. Then I would get this z(x) function.
My idea is to find such...
Homework Statement:: The magnetic field at every point on the path of integration
Relevant Equations:: The scenarios/situations are shown in the attached photo.
"Any conductors present that are not enclosed by a particular path may still contribute to the value of B field at every point, but...
Details of Question:
ds/dt= v which becomes ds=v dt, where s=displacement, t =time, and v=velocity
Then we can integrate both sides of this equation, and do a little algebra, and turn the above equation into:
s − s0 = v0t + ½at2
My main question is about the integration of...
I am confused as to how exactly we integrate differential forms. I know how to integrate them in the sense that I can perform the computations and I can prove statements, but I don't understand how it makes sense. Let's integrate a 1-form over a curve for example:
Let ##M## be a smooth...
I'm reading Coleman's "Aspects of symmetry" chap 7.
On the topic of the SU(2) winding number on ##S^3##on page 288, three parameters on ##S^3## are defined ##\theta_1,\theta_2,\theta_3##. Afterwards, it defines the winding number and to show it's invariant under continuous deformation of gauge...
Anyone have any idea how to perform the following two integrals?
##\int d\Omega n_{i}n_{j}## and ##\int d\Omega n_{i}n_{j}n_{k}n_{l}##
where the n is a unit vector.
I think in the case of "n da" you can see the denominator (1+x^2) as a constant, so
∫ ( sin(a) + M^2 ) / ( 1 + x^2 ) da
= ( 1 / ( 1 + x^2 ) ) * ∫ (sin(a) + M^2 ) da
= ( 1 / ( 1 + x^2 ) ) * ( -cos(a) + (M^2)a )
= ( - cos(a) + (M^2)a ) / ( 1 + x^2 )
---
Is this the way to go? This is my...
Want to integrate the total energy density over all photon energies between two
temperature values from 500K to 5800K, but not sure how to proceed.
Here is some examples to help:
Hi,
I have this formula ## f(\theta, \phi) = \frac{sin \theta}{4\pi}##
I have this statement that say if I integrate this formula above on a sphere then p = 1.
what does integrate on a sphere means? I know ##\int_0^{2\pi} ## is used for the circle.
Familiar with basics of stochastic calculus and integration over a Brownian motion. Trying to get a sense of Ambit Fields https://en.wikipedia.org/wiki/Ambit_field
which mention an integration over a Lévy basis:
Curious if anyone familiar with this? A Brownian motion is a Levy process...
The detailed list of the concepts I should master
I'm attending the last year of high school and I'm currently studying limits.
For university test reasons I'll need to study on my own topics such as differentiation and integration... and I have just 14 days to do so!
Firstly, do you think it's...
Performing the x-integration first the limit are x=y2 and x= -y2 and then the y limits are 0 to 1. This gives the final answer 2/5
But i am getting confused when trying to reverse the order of integration. My attempt is that i have to divide the region in 2 equal halfs and then double my answer...
Hi,
I'm wondering how can I get ## \phi(t) = A sin(\omega t) + B cos(\omega t)##
I know I have to integrate 2 times ##\ddot\phi = -\omega^2\phi##. However, I don't have any more explanation in my book.
I know A and B are the constants of integration.