weierstrass substitution proofimperial armour compendium 9th edition pdf trove

q Required fields are marked *, \(\begin{array}{l}\sum_{k=0}^{n}f\left ( \frac{k}{n} \right )\begin{pmatrix}n \\k\end{pmatrix}x_{k}(1-x)_{n-k}\end{array} \), \(\begin{array}{l}\sum_{k=0}^{n}(f-f(\zeta))\left ( \frac{k}{n} \right )\binom{n}{k} x^{k}(1-x)^{n-k}\end{array} \), \(\begin{array}{l}\sum_{k=0}^{n}\binom{n}{k}x^{k}(1-x)^{n-k} = (x+(1-x))^{n}=1\end{array} \), \(\begin{array}{l}\left|B_{n}(x, f)-f(\zeta) \right|=\left|B_{n}(x,f-f(\zeta)) \right|\end{array} \), \(\begin{array}{l}\leq B_{n}\left ( x,2M\left ( \frac{x- \zeta}{\delta } \right )^{2}+ \frac{\epsilon}{2} \right ) \end{array} \), \(\begin{array}{l}= \frac{2M}{\delta ^{2}} B_{n}(x,(x- \zeta )^{2})+ \frac{\epsilon}{2}\end{array} \), \(\begin{array}{l}B_{n}(x, (x- \zeta)^{2})= x^{2}+ \frac{1}{n}(x x^{2})-2 \zeta x + \zeta ^{2}\end{array} \), \(\begin{array}{l}\left| (B_{n}(x,f)-f(\zeta))\right|\leq \frac{\epsilon}{2}+\frac{2M}{\delta ^{2}}(x- \zeta)^{2}+\frac{2M}{\delta^{2}}\frac{1}{n}(x- x ^{2})\end{array} \), \(\begin{array}{l}\left| (B_{n}(x,f)-f(\zeta))\right|\leq \frac{\epsilon}{2}+\frac{2M}{\delta ^{2}}\frac{1}{n}(\zeta- \zeta ^{2})\end{array} \), \(\begin{array}{l}\left| (B_{n}(x,f)-f(\zeta))\right|\leq \frac{\epsilon}{2}+\frac{M}{2\delta ^{2}n}\end{array} \), \(\begin{array}{l}\int_{0}^{1}f(x)x^{n}dx=0\end{array} \), \(\begin{array}{l}\int_{0}^{1}f(x)p(x)dx=0\end{array} \), \(\begin{array}{l}\int_{0}^{1}p_{n}f\rightarrow \int _{0}^{1}f^{2}\end{array} \), \(\begin{array}{l}\int_{0}^{1}p_{n}f = 0\end{array} \), \(\begin{array}{l}\int _{0}^{1}f^{2}=0\end{array} \), \(\begin{array}{l}\int_{0}^{1}f(x)dx = 0\end{array} \). How to handle a hobby that makes income in US. After setting. The Weierstrass substitution is the trigonometric substitution which transforms an integral of the form. A similar statement can be made about tanh /2. Mathematics Stack Exchange is a question and answer site for people studying math at any level and professionals in related fields. The attractor is at the focus of the ellipse at $O$ which is the origin of coordinates, the point of periapsis is at $P$, the center of the ellipse is at $C$, the orbiting body is at $Q$, having traversed the blue area since periapsis and now at a true anomaly of $\nu$. Follow Up: struct sockaddr storage initialization by network format-string. \). It is sometimes misattributed as the Weierstrass substitution. This is Kepler's second law, the law of areas equivalent to conservation of angular momentum. To subscribe to this RSS feed, copy and paste this URL into your RSS reader. {\displaystyle t} t If an integrand is a function of only \(\tan x,\) the substitution \(t = \tan x\) converts this integral into integral of a rational function. and then we can go back and find the area of sector $OPQ$ of the original ellipse as $$\frac12a^2\sqrt{1-e^2}(E-e\sin E)$$ x = From Wikimedia Commons, the free media repository. = So if doing an integral with a factor of $\frac1{1+e\cos\nu}$ via the eccentric anomaly was good enough for Kepler, surely it's good enough for us. Definition of Bernstein Polynomial: If f is a real valued function defined on [0, 1], then for n N, the nth Bernstein Polynomial of f is defined as . / Thus, the tangent half-angle formulae give conversions between the stereographic coordinate t on the unit circle and the standard angular coordinate . This follows since we have assumed 1 0 xnf (x) dx = 0 . Definition 3.2.35. 2 Trigonometric Substitution 25 5. The Weierstrass substitution parametrizes the unit circle centered at (0, 0). A line through P (except the vertical line) is determined by its slope. The substitution is: u tan 2. for < < , u R . Learn more about Stack Overflow the company, and our products. The integral on the left is $-\cot x$ and the one on the right is an easy $u$-sub with $u=\sin x$. p {\textstyle t=\tan {\tfrac {x}{2}}} We give a variant of the formulation of the theorem of Stone: Theorem 1. 3. $\qquad$ $\endgroup$ - Michael Hardy &=\text{ln}|u|-\frac{u^2}{2} + C \\ Geometrical and cinematic examples. If you do use this by t the power goes to 2n. Date/Time Thumbnail Dimensions User \frac{1}{a + b \cos x} &= \frac{1}{a \left (\cos^2 \frac{x}{2} + \sin^2 \frac{x}{2} \right ) + b \left (\cos^2 \frac{x}{2} - \sin^2 \frac{x}{2} \right )}\\ x {\textstyle du=\left(-\csc x\cot x+\csc ^{2}x\right)\,dx} The simplest proof I found is on chapter 3, "Why Does The Miracle Substitution Work?" So you are integrating sum from 0 to infinity of (-1) n * t 2n / (2n+1) dt which is equal to the sum form 0 to infinity of (-1) n *t 2n+1 / (2n+1) 2 . Weierstrass Trig Substitution Proof. weierstrass substitution proof. d 382-383), this is undoubtably the world's sneakiest substitution. . According to the Weierstrass Approximation Theorem, any continuous function defined on a closed interval can be approximated uniformly by a polynomial function. can be expressed as the product of \begin{aligned} What is the correct way to screw wall and ceiling drywalls? S2CID13891212. + u Denominators with degree exactly 2 27 . 2 Finally, as t goes from 1 to+, the point follows the part of the circle in the second quadrant from (0,1) to(1,0). Integrate $\int \frac{4}{5+3\cos(2x)}\,d x$. If tan /2 is a rational number then each of sin , cos , tan , sec , csc , and cot will be a rational number (or be infinite). 1 Instead of Prohorov's theorem, we prove here a bare-hands substitute for the special case S = R. When doing so, it is convenient to have the following notion of convergence of distribution functions. H goes only once around the circle as t goes from to+, and never reaches the point(1,0), which is approached as a limit as t approaches. My question is, from that chapter, can someone please explain to me how algebraically the $\frac{\theta}{2}$ angle is derived? and the natural logarithm: Comparing the hyperbolic identities to the circular ones, one notices that they involve the same functions of t, just permuted. Other trigonometric functions can be written in terms of sine and cosine. Why do we multiply numerator and denominator by $\sin px$ for evaluating $\int \frac{\cos ax+\cos bx}{1-2\cos cx}dx$? importance had been made. The Weierstrass substitution can also be useful in computing a Grbner basis to eliminate trigonometric functions from a system of equations (Trott To calculate an integral of the form \(\int {R\left( {\sin x} \right)\cos x\,dx} ,\) where \(R\) is a rational function, use the substitution \(t = \sin x.\), Similarly, to calculate an integral of the form \(\int {R\left( {\cos x} \right)\sin x\,dx} ,\) where \(R\) is a rational function, use the substitution \(t = \cos x.\). Draw the unit circle, and let P be the point (1, 0). Tangent line to a function graph. Styling contours by colour and by line thickness in QGIS. . Since, if 0 f Bn(x, f) and if g f Bn(x, f). cot t the \(X^2\) term (whereas if \(\mathrm{char} K = 3\) we can eliminate either the \(X^2\) Weierstrass' preparation theorem. Other resolutions: 320 170 pixels | 640 340 pixels | 1,024 544 pixels | 1,280 680 pixels | 2,560 1,359 . All Categories; Metaphysics and Epistemology Combining the Pythagorean identity with the double-angle formula for the cosine, Bestimmung des Integrals ". Now consider f is a continuous real-valued function on [0,1]. A point on (the right branch of) a hyperbola is given by(cosh , sinh ). This allows us to write the latter as rational functions of t (solutions are given below). \\ b File. The differential \(dx\) is determined as follows: Any rational expression of trigonometric functions can be always reduced to integrating a rational function by making the Weierstrass substitution. Especially, when it comes to polynomial interpolations in numerical analysis. &=-\frac{2}{1+\text{tan}(x/2)}+C. Now, add and subtract $b^2$ to the denominator and group the $+b^2$ with $-b^2\cos^2x$. x G a x \implies & d\theta = (2)'\!\cdot\arctan\left(t\right) + 2\!\cdot\!\big(\arctan\left(t\right)\big)' $$\int\frac{dx}{a+b\cos x}=\frac1a\int\frac{dx}{1+\frac ba\cos x}=\frac1a\int\frac{d\nu}{1+\left|\frac ba\right|\cos\nu}$$ 1. Can you nd formulas for the derivatives {\textstyle t=0} pp. This equation can be further simplified through another affine transformation. Given a function f, finding a sequence which converges to f in the metric d is called uniform approximation.The most important result in this area is due to the German mathematician Karl Weierstrass (1815 to 1897).. The steps for a proof by contradiction are: Step 1: Take the statement, and assume that the contrary is true (i.e. The best answers are voted up and rise to the top, Not the answer you're looking for? \). {\displaystyle dt} Why do academics stay as adjuncts for years rather than move around? Learn more about Stack Overflow the company, and our products. x \end{aligned} Weierstrass Substitution and more integration techniques on https://brilliant.org/blackpenredpen/ This link gives you a 20% off discount on their annual prem. \), \( In integral calculus, the tangent half-angle substitution - known in Russia as the universal trigonometric substitution, sometimes misattributed as the Weierstrass substitution, and also known by variant names such as half-tangent substitution or half-angle substitution - is a change of variables used for evaluating integrals, which converts a rational function of trigonometric functions . f p < / M. We also know that 1 0 p(x)f (x) dx = 0. What is the purpose of this D-shaped ring at the base of the tongue on my hiking boots? x Retrieved 2020-04-01. . File history. must be taken into account. x Transactions on Mathematical Software. Other sources refer to them merely as the half-angle formulas or half-angle formulae . @robjohn : No, it's not "really the Weierstrass" since call the tangent half-angle substitution "the Weierstrass substitution" is incorrect. If the integral is a definite integral (typically from $0$ to $\pi/2$ or some other variants of this), then we can follow the technique here to obtain the integral. Newton potential for Neumann problem on unit disk. Instead of + and , we have only one , at both ends of the real line. Finally, fifty years after Riemann, D. Hilbert . that is, |f(x) f()| 2M [(x )/ ]2 + /2 x [0, 1]. The complete edition of Bolzano's works (Bernard-Bolzano-Gesamtausgabe) was founded by Jan Berg and Eduard Winter together with the publisher Gnther Holzboog, and it started in 1969.Since then 99 volumes have already appeared, and about 37 more are forthcoming. Note that these are just the formulas involving radicals (http://planetmath.org/Radical6) as designated in the entry goniometric formulas; however, due to the restriction on x, the s are unnecessary. How to handle a hobby that makes income in US, Trying to understand how to get this basic Fourier Series. csc Stack Exchange network consists of 181 Q&A communities including Stack Overflow, the largest, most trusted online community for developers to learn, share their knowledge, and build their careers. Later authors, citing Stewart, have sometimes referred to this as the Weierstrass substitution, for instance: Jeffrey, David J.; Rich, Albert D. (1994). In trigonometry, tangent half-angle formulas relate the tangent of half of an angle to trigonometric functions of the entire angle. u-substitution, integration by parts, trigonometric substitution, and partial fractions. ) Are there tables of wastage rates for different fruit and veg? = Yet the fascination of Dirichlet's Principle itself persisted: time and again attempts at a rigorous proof were made. Changing \(u = t - \frac{2}{3},\) \(du = dt\) gives the final answer: Make the universal trigonometric substitution: we can easily find the integral:we can easily find the integral: To simplify the integral, we use the Weierstrass substitution: As in the previous examples, we will use the universal trigonometric substitution: Since \(\sin x = {\frac{{2t}}{{1 + {t^2}}}},\) \(\cos x = {\frac{{1 - {t^2}}}{{1 + {t^2}}}},\) we can write: Making the \({\tan \frac{x}{2}}\) substitution, we have, Then the integral in \(t-\)terms is written as. 2 Example 15. Follow Up: struct sockaddr storage initialization by network format-string, Linear Algebra - Linear transformation question. A geometric proof of the Weierstrass substitution In various applications of trigonometry , it is useful to rewrite the trigonometric functions (such as sine and cosine ) in terms of rational functions of a new variable t {\displaystyle t} . tan It only takes a minute to sign up. csc Weierstrass Approximation theorem provides an important result of approximating a given continuous function defined on a closed interval to a polynomial function, which can be easily computed to find the value of the function. t As with other properties shared between the trigonometric functions and the hyperbolic functions, it is possible to use hyperbolic identities to construct a similar form of the substitution, (This substitution is also known as the universal trigonometric substitution.) Chain rule. According to the theorem, every continuous function defined on a closed interval [a, b] can approximately be represented by a polynomial function. Then Kepler's first law, the law of trajectory, is 2 The trigonometric functions determine a function from angles to points on the unit circle, and by combining these two functions we have a function from angles to slopes. Does a summoned creature play immediately after being summoned by a ready action? , However, I can not find a decent or "simple" proof to follow. ) Let \(K\) denote the field we are working in. The Weierstrass substitution is very useful for integrals involving a simple rational expression in \(\sin x\) and/or \(\cos x\) in the denominator. &=\text{ln}|\text{tan}(x/2)|-\frac{\text{tan}^2(x/2)}{2} + C. are easy to study.]. For a proof of Prohorov's theorem, which is beyond the scope of these notes, see [Dud89, Theorem 11.5.4]. To compute the integral, we complete the square in the denominator: &=\int{(\frac{1}{u}-u)du} \\ One of the most important ways in which a metric is used is in approximation. &=-\frac{2}{1+u}+C \\ It turns out that the absolute value signs in these last two formulas may be dropped, regardless of which quadrant is in. sin Weierstrass Approximation Theorem is given by German mathematician Karl Theodor Wilhelm Weierstrass. Why do academics stay as adjuncts for years rather than move around? (c) Finally, use part b and the substitution y = f(x) to obtain the formula for R b a f(x)dx. But I remember that the technique I saw was a nice way of evaluating these even when $a,b\neq 1$. 2 However, the Bolzano-Weierstrass Theorem (Calculus Deconstructed, Prop. Other sources refer to them merely as the half-angle formulas or half-angle formulae. Typically, it is rather difficult to prove that the resulting immersion is an embedding (i.e., is 1-1), although there are some interesting cases where this can be done. In the case = 0, we get the well-known perturbation theory for the sine-Gordon equation. Finally, it must be clear that, since \(\text{tan}x\) is undefined for \(\frac{\pi}{2}+k\pi\), \(k\) any integer, the substitution is only meaningful when restricted to intervals that do not contain those values, e.g., for \(-\pi\lt x\lt\pi\). 6. x where $a$ and $e$ are the semimajor axis and eccentricity of the ellipse. The general statement is something to the eect that Any rational function of sinx and cosx can be integrated using the . where $\ell$ is the orbital angular momentum, $m$ is the mass of the orbiting body, the true anomaly $\nu$ is the angle in the orbit past periapsis, $t$ is the time, and $r$ is the distance to the attractor. Among these formulas are the following: From these one can derive identities expressing the sine, cosine, and tangent as functions of tangents of half-angles: Using double-angle formulae and the Pythagorean identity How can this new ban on drag possibly be considered constitutional? James Stewart wasn't any good at history. How to solve the integral $\int\limits_0^a {\frac{{\sqrt {{a^2} - {x^2}} }}{{b - x}}} \mathop{\mathrm{d}x}\\$? Proof by contradiction - key takeaways. &=\int{\frac{2du}{1+2u+u^2}} \\ Then we can find polynomials pn(x) such that every pn converges uniformly to x on [a,b]. The technique of Weierstrass Substitution is also known as tangent half-angle substitution. = 2 + sin cornell application graduate; conflict of nations: world war 3 unblocked; stone's throw farm shelbyville, ky; words to describe a supermodel; navy board schedule fy22 Is there a way of solving integrals where the numerator is an integral of the denominator? Weierstrass Approximation theorem in real analysis presents the notion of approximating continuous functions by polynomial functions. d Find $\int_0^{2\pi} \frac{1}{3 + \cos x} dx$. x |x y| |f(x) f(y)| /2 for every x, y [0, 1]. An irreducibe cubic with a flex can be affinely has a flex Integration of Some Other Classes of Functions 13", "Intgration des fonctions transcendentes", "19. Definition of Bernstein Polynomial: If f is a real valued function defined on [0, 1], then for n N, the nth Bernstein Polynomial of f is defined as, Proof: To prove the theorem on closed intervals [a,b], without loss of generality we can take the closed interval as [0, 1]. sines and cosines can be expressed as rational functions of A related substitution appears in Weierstrasss Mathematical Works, from an 1875 lecture wherein Weierstrass credits Carl Gauss (1818) with the idea of solving an integral of the form With the objective of identifying intrinsic forms of mathematical production in complex analysis (CA), this study presents an analysis of the mathematical activity of five original works that . 2 File usage on Commons. Die Weierstra-Substitution (auch unter Halbwinkelmethode bekannt) ist eine Methode aus dem mathematischen Teilgebiet der Analysis. 2 Is there a single-word adjective for "having exceptionally strong moral principles"? The Weierstrass elliptic functions are identified with the famous mathematicians N. H. Abel (1827) and K. Weierstrass (1855, 1862). The singularity (in this case, a vertical asymptote) of cos cos So as to relate the area swept out by a line segment joining the orbiting body to the attractor Kepler drew a little picture. We have a rational expression in and in the denominator, so we use the Weierstrass substitution to simplify the integral: and. But here is a proof without words due to Sidney Kung: \(\text{sin}\theta=\frac{AC}{AB}=\frac{2u}{1+u^2}\) and [7] Michael Spivak called it the "world's sneakiest substitution".[8]. $$d E=\frac{\sqrt{1-e^2}}{1+e\cos\nu}d\nu$$ A standard way to calculate \(\int{\frac{dx}{1+\text{sin}x}}\) is via a substitution \(u=\text{tan}(x/2)\). In Ceccarelli, Marco (ed.). Metadata. , Elementary functions and their derivatives. {\textstyle t=\tan {\tfrac {x}{2}},} Linear Algebra - Linear transformation question. My code is GPL licensed, can I issue a license to have my code be distributed in a specific MIT licensed project? There are several ways of proving this theorem. Do roots of these polynomials approach the negative of the Euler-Mascheroni constant? Moreover, since the partial sums are continuous (as nite sums of continuous functions), their uniform limit fis also continuous. Then by uniform continuity of f we can have, Now, |f(x) f()| 2M 2M [(x )/ ]2 + /2. So to get $\nu(t)$, you need to solve the integral , For a special value = 1/8, we derive a . According to Spivak (2006, pp. WEIERSTRASS APPROXIMATION THEOREM TL welll kroorn Neiendsaas . ( Fact: Isomorphic curves over some field \(K\) have the same \(j\)-invariant. = As x varies, the point (cos x . "1.4.6. Furthermore, each of the lines (except the vertical line) intersects the unit circle in exactly two points, one of which is P. This determines a function from points on the unit circle to slopes. \begin{align} (d) Use what you have proven to evaluate R e 1 lnxdx. d 2 As t goes from 1 to0, the point follows the part of the circle in the fourth quadrant from (0,1) to(1,0). These identities are known collectively as the tangent half-angle formulae because of the definition of {\displaystyle t,} Use the universal trigonometric substitution: \[dx = d\left( {2\arctan t} \right) = \frac{{2dt}}{{1 + {t^2}}}.\], \[{\cos ^2}x = \frac{1}{{1 + {{\tan }^2}x}} = \frac{1}{{1 + {t^2}}},\;\;\;{\sin ^2}x = \frac{{{{\tan }^2}x}}{{1 + {{\tan }^2}x}} = \frac{{{t^2}}}{{1 + {t^2}}}.\], \[t = \tan \frac{x}{2},\;\; \Rightarrow x = 2\arctan t,\;\;\; dx = \frac{{2dt}}{{1 + {t^2}}}.\], \[\int {\frac{{dx}}{{1 + \sin x}}} = \int {\frac{{\frac{{2dt}}{{1 + {t^2}}}}}{{1 + \frac{{2t}}{{1 + {t^2}}}}}} = \int {\frac{{2dt}}{{1 + {t^2} + 2t}}} = \int {\frac{{2dt}}{{{{\left( {t + 1} \right)}^2}}}} = - \frac{2}{{t + 1}} + C = - \frac{2}{{\tan \frac{x}{2} + 1}} + C.\], \[x = \arctan t,\;\; \sin x = \frac{{2t}}{{1 + {t^2}}},\;\; dx = \frac{{2dt}}{{1 + {t^2}}},\], \[I = \int {\frac{{dx}}{{3 - 2\sin x}}} = \int {\frac{{\frac{{2dt}}{{1 + {t^2}}}}}{{3 - 2 \cdot \frac{{2t}}{{1 + {t^2}}}}}} = \int {\frac{{2dt}}{{3 + 3{t^2} - 4t}}} = \int {\frac{{2dt}}{{3\left( {{t^2} - \frac{4}{3}t + 1} \right)}}} = \frac{2}{3}\int {\frac{{dt}}{{{t^2} - \frac{4}{3}t + 1}}} .\], \[{t^2} - \frac{4}{3}t + 1 = {t^2} - \frac{4}{3}t + {\left( {\frac{2}{3}} \right)^2} - {\left( {\frac{2}{3}} \right)^2} + 1 = {\left( {t - \frac{2}{3}} \right)^2} - \frac{4}{9} + 1 = {\left( {t - \frac{2}{3}} \right)^2} + \frac{5}{9} = {\left( {t - \frac{2}{3}} \right)^2} + {\left( {\frac{{\sqrt 5 }}{3}} \right)^2}.\], \[I = \frac{2}{3}\int {\frac{{dt}}{{{{\left( {t - \frac{2}{3}} \right)}^2} + {{\left( {\frac{{\sqrt 5 }}{3}} \right)}^2}}}} = \frac{2}{3}\int {\frac{{du}}{{{u^2} + {{\left( {\frac{{\sqrt 5 }}{3}} \right)}^2}}}} = \frac{2}{3} \cdot \frac{1}{{\frac{{\sqrt 5 }}{3}}}\arctan \frac{u}{{\frac{{\sqrt 5 }}{3}}} + C = \frac{2}{{\sqrt 5 }}\arctan \frac{{3\left( {t - \frac{2}{3}} \right)}}{{\sqrt 5 }} + C = \frac{2}{{\sqrt 5 }}\arctan \frac{{3t - 2}}{{\sqrt 5 }} + C = \frac{2}{{\sqrt 5 }}\arctan \left( {\frac{{3\tan \frac{x}{2} - 2}}{{\sqrt 5 }}} \right) + C.\], \[t = \tan \frac{x}{4},\;\; \Rightarrow d\left( {\frac{x}{2}} \right) = \frac{{2dt}}{{1 + {t^2}}},\;\; \Rightarrow \cos \frac{x}{2} = \frac{{1 - {t^2}}}{{1 + {t^2}}}.\], \[\int {\frac{{dx}}{{1 + \cos \frac{x}{2}}}} = \int {\frac{{d\left( {\frac{x}{2}} \right)}}{{1 + \cos \frac{x}{2}}}} = 2\int {\frac{{\frac{{2dt}}{{1 + {t^2}}}}}{{1 + \frac{{1 - {t^2}}}{{1 + {t^2}}}}}} = 4\int {\frac{{dt}}{{1 + \cancel{t^2} + 1 - \cancel{t^2}}}} = 2\int {dt} = 2t + C = 2\tan \frac{x}{4} + C.\], \[t = \tan x,\;\; \Rightarrow x = \arctan t,\;\; \Rightarrow dx = \frac{{dt}}{{1 + {t^2}}},\;\; \Rightarrow \cos 2x = \frac{{1 - {t^2}}}{{1 + {t^2}}},\], \[\int {\frac{{dx}}{{1 + \cos 2x}}} = \int {\frac{{\frac{{dt}}{{1 + {t^2}}}}}{{1 + \frac{{1 - {t^2}}}{{1 + {t^2}}}}}} = \int {\frac{{dt}}{{1 + \cancel{t^2} + 1 - \cancel{t^2}}}} = \int {\frac{{dt}}{2}} = \frac{t}{2} + C = \frac{1}{2}\tan x + C.\], \[t = \tan \frac{x}{4},\;\; \Rightarrow x = 4\arctan t,\;\; dx = \frac{{4dt}}{{1 + {t^2}}},\;\; \cos \frac{x}{2} = \frac{{1 - {t^2}}}{{1 + {t^2}}}.\], \[\int {\frac{{dx}}{{4 + 5\cos \frac{x}{2}}}} = \int {\frac{{\frac{{4dt}}{{1 + {t^2}}}}}{{4 + 5 \cdot \frac{{1 - {t^2}}}{{1 + {t^2}}}}}} = \int {\frac{{4dt}}{{4\left( {1 + {t^2}} \right) + 5\left( {1 - {t^2}} \right)}}} = 4\int {\frac{{dt}}{{4 + 4{t^2} + 5 - 5{t^2}}}} = 4\int {\frac{{dt}}{{{3^2} - {t^2}}}} = 4 \cdot \frac{1}{{2 \cdot 3}}\ln \left| {\frac{{3 + t}}{{3 - t}}} \right| + C = \frac{2}{3}\ln \left| {\frac{{3 + \tan \frac{x}{4}}}{{3 - \tan \frac{x}{4}}}} \right| + C.\], \[\int {\frac{{dx}}{{\sin x + \cos x}}} = \int {\frac{{\frac{{2dt}}{{1 + {t^2}}}}}{{\frac{{2t}}{{1 + {t^2}}} + \frac{{1 - {t^2}}}{{1 + {t^2}}}}}} = \int {\frac{{2dt}}{{2t + 1 - {t^2}}}} = 2\int {\frac{{dt}}{{1 - \left( {{t^2} - 2t} \right)}}} = 2\int {\frac{{dt}}{{1 - \left( {{t^2} - 2t + 1 - 1} \right)}}} = 2\int {\frac{{dt}}{{2 - {{\left( {t - 1} \right)}^2}}}} = 2\int {\frac{{d\left( {t - 1} \right)}}{{{{\left( {\sqrt 2 } \right)}^2} - {{\left( {t - 1} \right)}^2}}}} = 2 \cdot \frac{1}{{2\sqrt 2 }}\ln \left| {\frac{{\sqrt 2 + \left( {t - 1} \right)}}{{\sqrt 2 - \left( {t - 1} \right)}}} \right| + C = \frac{1}{{\sqrt 2 }}\ln \left| {\frac{{\sqrt 2 - 1 + \tan \frac{x}{2}}}{{\sqrt 2 + 1 - \tan \frac{x}{2}}}} \right| + C.\], \[t = \tan \frac{x}{2},\;\; \Rightarrow x = 2\arctan t,\;\; dx = \frac{{2dt}}{{1 + {t^2}}},\;\; \sin x = \frac{{2t}}{{1 + {t^2}}},\;\; \cos x = \frac{{1 - {t^2}}}{{1 + {t^2}}}.\], \[\int {\frac{{dx}}{{\sin x + \cos x + 1}}} = \int {\frac{{\frac{{2dt}}{{1 + {t^2}}}}}{{\frac{{2t}}{{1 + {t^2}}} + \frac{{1 - {t^2}}}{{1 + {t^2}}} + 1}}} = \int {\frac{{\frac{{2dt}}{{1 + {t^2}}}}}{{\frac{{2t + 1 - {t^2} + 1 + {t^2}}}{{1 + {t^2}}}}}} = \int {\frac{{2dt}}{{2t + 2}}} = \int {\frac{{dt}}{{t + 1}}} = \ln \left| {t + 1} \right| + C = \ln \left| {\tan \frac{x}{2} + 1} \right| + C.\], \[I = \int {\frac{{dx}}{{\sec x + 1}}} = \int {\frac{{dx}}{{\frac{1}{{\cos x}} + 1}}} = \int {\frac{{\cos xdx}}{{1 + \cos x}}} .\], \[I = \int {\frac{{\cos xdx}}{{1 + \cos x}}} = \int {\frac{{\frac{{1 - {t^2}}}{{1 + {t^2}}} \cdot \frac{{2dt}}{{1 + {t^2}}}}}{{1 + \frac{{1 - {t^2}}}{{1 + {t^2}}}}}} = 2\int {\frac{{\frac{{1 - {t^2}}}{{{{\left( {1 + {t^2}} \right)}^2}}}dt}}{{\frac{{1 + {t^2} + 1 - {t^2}}}{{1 + {t^2}}}}}} = \int {\frac{{1 - {t^2}}}{{1 + {t^2}}}dt} = - \int {\frac{{1 + {t^2} - 2}}{{1 + {t^2}}}dt} = - \int {1dt} + 2\int {\frac{{dt}}{{1 + {t^2}}}} = - t + 2\arctan t + C = - \tan \frac{x}{2} + 2\arctan \left( {\tan \frac{x}{2}} \right) + C = x - \tan \frac{x}{2} + C.\], Trigonometric and Hyperbolic Substitutions.

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