In mathematics, an integral assigns numbers to functions in a way that describes displacement, area, volume, and other concepts that arise by combining infinitesimal data. The process of finding integrals is called integration. Along with differentiation, integration is a fundamental, essential operation of calculus, and serves as a tool to solve problems in mathematics and physics involving the area of an arbitrary shape, the length of a curve, and the volume of a solid, among others.
The integrals enumerated here are those termed definite integrals, which can be interpreted formally as the signed area of the region in the plane that is bounded by the graph of a given function between two points in the real line. Conventionally, areas above the horizontal axis of the plane are positive while areas below are negative. Integrals also refer to the concept of an antiderivative, a function whose derivative is the given function. In this case, they are called indefinite integrals. The fundamental theorem of calculus relates definite integrals with differentiation and provides a method to compute the definite integral of a function when its antiderivative is known.
Although methods of calculating areas and volumes dated from ancient Greek mathematics, the principles of integration were formulated independently by Isaac Newton and Gottfried Wilhelm Leibniz in the late 17th century, who thought of the area under a curve as an infinite sum of rectangles of infinitesimal width. Bernhard Riemann later gave a rigorous definition of integrals, which is based on a limiting procedure that approximates the area of a curvilinear region by breaking the region into thin vertical slabs.
Integrals may be generalized depending on the type of the function as well as the domain over which the integration is performed. For example, a line integral is defined for functions of two or more variables, and the interval of integration is replaced by a curve connecting the two endpoints of the interval. In a surface integral, the curve is replaced by a piece of a surface in three-dimensional space.
I need help with a derivation of an equation given in a journal paper. My question is related to the third paragraph of this paper: https://doi.org/10.1007/BF00619826. Although it is about fibre coupling my problem is purely mathematical. It is about solving a complex double integral. The...
I can't understand how this approximation works ##\sum_{k=0}^m\left(\frac{k}{m}\right)^n\approx\int_0^m\left(\frac{x}{m}\right)^ndx\tag{1}##Can you please help me
I need a help in the following problem. I feel that the question is stupid.
Take a function ##f\in C(\mathbb{R}^3)\cap L^1(\mathbb{R}^3)## and a number ##\alpha\in(0,3)##.
Prove that
$$\lim_{|x|\to\infty}\int_{\mathbb{R}^3}\frac{f(y)dy}{|x-y|^\alpha}=0.$$
I can prove this fact by the Uniform...
I start by parametarize the surface with two variables:
$$r(u,v) = (u, v, \frac {d -au -bv} c)$$
The I can get the normal vector by
$$dr/du \times dr/dv$$
What limits should I use to integrate this only within the elipse?
I could redo the whole thing and try write r(u, v) as u being the...
The following problem we considered with the students. Perhaps it would also be interesting for PF
A homogeneous rod can rotate freely in a plane about its (fixed) center of mass O . The corresponding moment of inertia is equal to J. Two identical particles of mass m can slide along the rod...
Let ##f:[0;1)\to\mathbb{R}## and ##f\in C^1([0;1))## and ##\lim_{x\to1^-}f(x)=+\infty## and ##\forall_{x\in[0;1)}-\infty<f(x)<+\infty##. Define $$A:=\int_0^1f(x)\, dx\,.$$ Assuming ##A## exists and is finite, is it possible that ##\text{sgn}(A)=-1##?
##\int \frac{\csc{x}\cot{x}}{1+\csc^2{x}}dx##
Let ##u = \csc{x}##
then
##-du = \csc{x}\cot{x}dx##
So,
##\int \frac{\csc{x}\cot{x}}{1+\csc^2{x}}dx##
##-\int \frac{1}{1+u^2}du = -\arctan{u} + C##
##-\arctan{\csc{x}} + C##
This answer was wrong. The actual answer involved fully simplifying...
Greetings All!
I have a problem finding the correct solution at first glance
My error was to determine the region of integration , for doing so I had to the intersection between y= sqrt(x) and y=2-x
to do so
x=(2-x)^2
to find at the end that x=1 or x=5
while graphically we can see that the...
Greetings!
The exercice ask to calculate the circuitation of the the vector field F on the border of the set omega
I do understand the solution very well
my problem is the region!
I m used to work with a region delimitated clearly by two intersecting function here the upper one stop a y=3 and...
I am aware that one usually starts from the Maxwell equations and then derives the masslessness of a photon. But can one do it the other way round? The action of photon would be ##S = \hbar \int \nu (1 - \dot{x}^2) \mbox{d}t##, where ##\nu## is the frequency acting as a Lagrange multiplier...
In an article written by Richard Rollleigh, published in 2010 entitled The Double Slit Experiment and Quantum Mechanics, he argues as follows:
"For something to be predictable, it must be a consistent measurement result. The positions at which individual particles land on the screen are not...
I am not seeing how the v goes away in the third equal sign of equation (1.8). It seems to be that it must be cos(z*sinh(u+v)), not cos(z*sinh(u)).
In the defined equations (1.7), the variable "v" can become imaginary, so a simple change of variables would change the integration sign by adding...
From Feynman lectures on physics: https://www.feynmanlectures.caltech.edu/I_08.html
Page 8-7 (Ch 8 Motion)
“ To be more precise, it is the sum of the velocity at a certain time, let us say the ith time, multiplied by deltat.
##s=\sum_{i} v({t_i})\Delta t##”
Now I suppose ##{t_i}## is some time...
Let ##u=\int_1^{u}2xdx##.
\begin{align}u=& \int_1^{u}2xdx=\big[x^2\big]_1^u\\
u=&u^2-1\end{align}
Which leads to ##u=\frac{1\pm\sqrt{1+4}}{2}##
Assuming that the upper boundary of integration is greater than ##1##, or less than ##-1##, leads to ##u=\frac{1+\sqrt{5}}{2}\approx 1.61##. the second...
Is it possible to solve this integral? I think the substitution ##x=-u## does not help at all since it only changes variable ##x## to ##u## without changing the integrand much.
Using that substitution:
$$\int \frac{6x^2+5}{1+2^x}dx=-\int \frac{6u^2+5}{1+2^{-u}}du$$
Then how to continue?
Thanks
Hello guys. I was trying to evaluate the integral of sine of x^2 from - infinity to + infinity and ran into some inconsistencies. I know this integral converges to sqrt(pi/2). Can someone help me to figure out why I am getting a divergent answer?
$$ I = \int_{-\infty}^{+\infty} sin(x^2) dx =...
why does it say transforms? is there more than one Fourier transform?? we learned in class that the inverse Fourier transform of the Fourier transform of ##f## is ##f##, so there should be just one right? I'm uncertain of how to calulate this integral though.. Mr Wolfram showed me an indefinite...
I also don't understand how to get the descending factorials for this hypergeometric series, I also know that there is another way to write it with gamma functions, but in any case how am I supposed to do this?
If I write it as a general term, wolfram will give me the result
which leaves me...
Attempt:
Note we must have that
## f>0 ## and ## g>0 ## from some place
or
## f<0 ## and ## g<0 ## from some place
or
## g ,f ## have the same sign in ## [ 1, +\infty) ##.
Otherwise, we'd have that there are infinitely many ##x's ## where ##g,f ## differ and sign so we can chose a...
I would like to solve the integral underneath:
$$\displaystyle \int_{0}^{x}\!-{\frac {\lambda\,{{\rm e}^{-\lambda\,t}}{\beta}^{\alpha} \left( -\lambda+\beta \right) ^{-\alpha} \left( -\Gamma \left( \alpha \right) +\Gamma \left( \alpha, \left( -\lambda+\beta \right) t \right) \right)}{\Gamma...
$$\int \frac y {x^2+y^2} dx$$
$$\frac 1 y * \int \frac 1 {\frac {x^2}{y^2} + 1} dx = \frac 1 y * atan(x/y)$$
The answer is just atan(x/y), which you get using u-substitution but I honestly don't see why I don't get it doing it the normal way.
Problem statement : As a part of the problem, the diagram shows the contour ##C##above on the left. The contour ##C## is divided into three parts, ##C_1, C_2, C_3## which make up the sides of the right triangle.
Required to prove : ##\boxed{\oint_C x^2 y \mathrm{d} s = -\frac{\sqrt{2}}{12}}##...
Hi there, I've been stuck on this issue for two days. I'm hoping someone knowledgeable can explain.
I'm working through the construction of the quantum path integral for the free electrodynamic theory. I've been following a text by Fujikawa ("Path Integrals and Quantum Anomalies") and also...
I am trying to integrate a cross product and I wonder if the following is true. It does not feel like it is true but it would be very nice if it was since otherwise I have a problem with the signs...
This is my first time posting here, so I just pasted in the LaTeX code and hope that it is...
Problem : We are required to show that ##I = \int_C x^2y\;ds = \frac{1}{3}##.
Attempt : Before I begin, let me post an image of the problem situation, on the right. I would like to do this problem in three ways, starting with the simplest way - using (plane) polar coordinates.
(1) In (plane)...
I am asked to compute ##[\phi(x), \phi^\dagger(y)]## , with
##\phi = \int \frac{dp^3}{(2\pi)^3}e^{-ipx}\hat{a}(\vec{p})## and with z=x-y a spacelike vector. And show that this commutator does not vanish, which means that for this non-relativsitic field i.e. with ##p^0 = \frac{\vec{p}^2}{2m}##...
$\begin{array}{lll}
I&=\displaystyle\int{\frac{dx}{x^2\sqrt{x^2-16}}}
\quad x=4\sec\theta
\quad dx=4\tan \theta\sec \theta
\end{array}$
just seeing if I started with the right x and dx or is there better
Mahalo
Hello,
To first clarify what I want to know : I read the answer proposed from the solution manual and I understand it. What I want to understand is how they came up with the solution, and if there is a way to get better at this.
I have to show that, given a vector field ##F## such that ## F ...
Hi,
I am trying to find open-form solutions to the integrals attached below. Lambda and Eta are positive, known constants, smaller than 10 (if it helps). I would appreciate any help! Thank you!
My TI 89 Platinum is returning ln(abs(cos(x))/abs(sin(x)-1)) for integral sec(x)dx. It's supposed to return ln(abs(tan(x)+sec(x)) or ln(abs(sin(x)+1)/abs(cos(x))). If you enter x=0, you get 'undefined' the way my TI 89 is doing it. It's supposed to return 0. Is this a computation error or...
Mentor note: Moved from technical section, so missing the homework template.
How do you integrate this?
$$\int \frac{1}{x^2 + 2} dx$$
My attempt is $$\ln |x^2 + 2| + C$$
On page 344 of "A First Course in GR" he writes the following:
When I do the integration I get the following: ##\int_0^{\chi^2}d\chi^2= \int_0^{r^2}\frac{dr^2}{1-r^2}= \chi^2 = -\ln (1-r^2)##, after I invert the last relation I get: ##r=\sqrt{1-\exp(-\chi^2)}##, where did I go wrong in my...
The vector equation is ## v(x)=(e^x cos(2x), e^x sin(2x), e^x) ##
I know the arc-length formula is ## S=\int_a^b \|v(x)\| \,dx ##
I found the derivative from a previous question dealing with this same function, but the when I plug it into the arc-length function I get an integral that I've...
In Richard Feynman's book "The Strange Theory of Light and Matter", in chapter 2, he explains how to calculate the probability that light from some source will be reflected by a mirror and be detected at some location. He explains how you sum up all of the probability amplitudes (represented...
Hi all,
Consider a system of ##N## noninteracting, identical electric point dipoles (dipole moment ##\vec{\mu}##) subjected to an external field ##\vec{E}=E\hat{z}##. The Lagrangian for this system is...
I have the following integration -
$$\int \frac{2}{x - b \frac{x^{m - n + 1}}{(-x + 1)^m}} \, dx $$
To solve this I did the following -
$$\int \frac{1 - b \frac{x^{m - n}}{(-x + 1)^m}+1 + b \frac{x^{m - n}}{(-x + 1)^m}}{x(1 - b \frac{x^{m - n}}{(-x + 1)^m})} \, dx $$
Which gives me -...
Solving integrals by hand is difficult and prone to errors, and the techniques such as integration by parts, partial fraction decomposition, and trig substitutions only work for a small subset of integrals and I do not see the point of avoiding technology like Wolfram Mathematica for...
Hey! 😊
I want to calculate the integral $$\int\frac{1}{(x+4)(x^2-8x+19)}\, dx$$ I have done the following : $$\frac{1}{(x+4)(x^2-8x+19)}=\frac{1}{67}\frac{1}{x+4}+\frac{1}{67}\frac{12-x}{x^2-8x+19}$$ and so we get \begin{align*}\int\frac{1}{(x+4)(x^2-8x+19)}\, dx&=\frac{1}{67}\int...
Greetings
here is my integral
Compute the volume of the solid
and here is the solution (that I don't agree with)
So as you can see they started integrating sinx from 0 to pi and then multiplied everything by two! for me sin(x) is an odd function and it's integral should be 0 over symmetric...
Greetings!
I have the following integral
and here is the solution of the book (which I understand perfectly)
I have an altenative method I want to apply that does not seems to gives me the final resultMy method
which doesn't give me the final results!
where is my mistake?
thank you!
Hello!
The integral in equation (16), at the paper, is:
##I = r \int_{-\pi}^{\pi} e^{-2kr\phi} ~d\phi ##
My integration is as the following :
## I = - \frac{1}{2 k} e^{-2kr\phi} ~|_{-\pi}^{\pi} + C ##, so
## I = - \frac{1}{2 k} ( e^{-2kr\pi} -e^{2kr\pi})+ C ##
Now how to use the initial...
Hi! Some help with this problem would be much appreciated.
The overlap integral is defined as ##S = \int \phi_A (\mathbf{r}_A) \phi_B (\mathbf{r}_B) \,d\mathbf{r}##. For the two orbitals, I have that
$$\phi_A = \frac{1}{\sqrt{\pi}} \Big( \frac{1}{a_0} \Big)^{3/2} e^{-r_A / a_0}$$
for the 1s...
I'm trying to see if I can calculate the peak draw weight of my bow based on the draw length and the velocity of the arrow and a known shape of a curve, but I'm not quite sure how to make such a function, if there even is such a way.
This is the shape of the draw weight plotted against...