Is there a change-of-variables solution for integrals from negative infinity to a constant?












3












$begingroup$


I found a fantastic and generalizable substitution technique for computing definite integrals that go to infinity from either negative infinity or a constant, regardless of the function (sorry for the external link):



http://ab-initio.mit.edu/wiki/index.php/Cubature#Infinite_intervals



But what's killing me is that I need the same sort of thing for a function going from negative infinity to a constant, and I can't convince myself that some obvious transformation of either of these two is correct. Doing u-substitution on any given integrand to take care of a (negative) infinite bound is simple enough, but a general transformation rule like one of the ones in the link - totally independent of the function itself - would be invaluable.



Edit 1 (Might be a Wild Goose Chase)



So the second formula up in that link, is:



$int_{-infty}^{infty}f(x)dx=int_{-1}^1 f(frac{t}{1-t^2})frac{1+t^2}{(1-t^2)^2}dt$



If $a$ represents our generic real-number constant, the above could certainly be broken up as:



$int_{-infty}^{infty}f(x)dx=int_{-1}^a f(frac{t}{1-t^2})frac{1+t^2}{(1-t^2)^2}dt+int_{a}^1 f(frac{t}{1-t^2})frac{1+t^2}{(1-t^2)^2}dt$



Which tempts me to jump to the conclusion that the first term on the RHS can be used as our general negative-infinity-to-constant formula:



$int_{-infty}^{a}f(x)dx=int_{-1}^a f(frac{t}{1-t^2})frac{1+t^2}{(1-t^2)^2}dt$



In order for this to be true, however, the second RHS term would have to complement it by being a valid formula to integrate from any constant up to infinity, IE:



$int_{a}^{infty}f(x)dx=int_{a}^1 f(frac{t}{1-t^2})frac{1+t^2}{(1-t^2)^2}dt$



...but the first formula given at the above link is also supposed to be such a formula, solving for that exact LHS term! So the two would have to be equivalent - IE:



$int_{a}^{infty}f(x)dx=int_{a}^1 f(frac{t}{1-t^2})frac{1+t^2}{(1-t^2)^2}dt=int_{0}^1 f(a+frac{t}{1-t})frac{1}{(1-t)^2}dt$



And here I'm stuck, because I can't figure out whether or not that's plausible for all convergent $f(x)$. I have a bad feeling about that whole approach because it relies on the assumption that dividing up a finite space at a given point is the same as dividing up an equivalent infinite space at the exact same point, proportionally.










share|cite|improve this question











$endgroup$

















    3












    $begingroup$


    I found a fantastic and generalizable substitution technique for computing definite integrals that go to infinity from either negative infinity or a constant, regardless of the function (sorry for the external link):



    http://ab-initio.mit.edu/wiki/index.php/Cubature#Infinite_intervals



    But what's killing me is that I need the same sort of thing for a function going from negative infinity to a constant, and I can't convince myself that some obvious transformation of either of these two is correct. Doing u-substitution on any given integrand to take care of a (negative) infinite bound is simple enough, but a general transformation rule like one of the ones in the link - totally independent of the function itself - would be invaluable.



    Edit 1 (Might be a Wild Goose Chase)



    So the second formula up in that link, is:



    $int_{-infty}^{infty}f(x)dx=int_{-1}^1 f(frac{t}{1-t^2})frac{1+t^2}{(1-t^2)^2}dt$



    If $a$ represents our generic real-number constant, the above could certainly be broken up as:



    $int_{-infty}^{infty}f(x)dx=int_{-1}^a f(frac{t}{1-t^2})frac{1+t^2}{(1-t^2)^2}dt+int_{a}^1 f(frac{t}{1-t^2})frac{1+t^2}{(1-t^2)^2}dt$



    Which tempts me to jump to the conclusion that the first term on the RHS can be used as our general negative-infinity-to-constant formula:



    $int_{-infty}^{a}f(x)dx=int_{-1}^a f(frac{t}{1-t^2})frac{1+t^2}{(1-t^2)^2}dt$



    In order for this to be true, however, the second RHS term would have to complement it by being a valid formula to integrate from any constant up to infinity, IE:



    $int_{a}^{infty}f(x)dx=int_{a}^1 f(frac{t}{1-t^2})frac{1+t^2}{(1-t^2)^2}dt$



    ...but the first formula given at the above link is also supposed to be such a formula, solving for that exact LHS term! So the two would have to be equivalent - IE:



    $int_{a}^{infty}f(x)dx=int_{a}^1 f(frac{t}{1-t^2})frac{1+t^2}{(1-t^2)^2}dt=int_{0}^1 f(a+frac{t}{1-t})frac{1}{(1-t)^2}dt$



    And here I'm stuck, because I can't figure out whether or not that's plausible for all convergent $f(x)$. I have a bad feeling about that whole approach because it relies on the assumption that dividing up a finite space at a given point is the same as dividing up an equivalent infinite space at the exact same point, proportionally.










    share|cite|improve this question











    $endgroup$















      3












      3








      3


      1



      $begingroup$


      I found a fantastic and generalizable substitution technique for computing definite integrals that go to infinity from either negative infinity or a constant, regardless of the function (sorry for the external link):



      http://ab-initio.mit.edu/wiki/index.php/Cubature#Infinite_intervals



      But what's killing me is that I need the same sort of thing for a function going from negative infinity to a constant, and I can't convince myself that some obvious transformation of either of these two is correct. Doing u-substitution on any given integrand to take care of a (negative) infinite bound is simple enough, but a general transformation rule like one of the ones in the link - totally independent of the function itself - would be invaluable.



      Edit 1 (Might be a Wild Goose Chase)



      So the second formula up in that link, is:



      $int_{-infty}^{infty}f(x)dx=int_{-1}^1 f(frac{t}{1-t^2})frac{1+t^2}{(1-t^2)^2}dt$



      If $a$ represents our generic real-number constant, the above could certainly be broken up as:



      $int_{-infty}^{infty}f(x)dx=int_{-1}^a f(frac{t}{1-t^2})frac{1+t^2}{(1-t^2)^2}dt+int_{a}^1 f(frac{t}{1-t^2})frac{1+t^2}{(1-t^2)^2}dt$



      Which tempts me to jump to the conclusion that the first term on the RHS can be used as our general negative-infinity-to-constant formula:



      $int_{-infty}^{a}f(x)dx=int_{-1}^a f(frac{t}{1-t^2})frac{1+t^2}{(1-t^2)^2}dt$



      In order for this to be true, however, the second RHS term would have to complement it by being a valid formula to integrate from any constant up to infinity, IE:



      $int_{a}^{infty}f(x)dx=int_{a}^1 f(frac{t}{1-t^2})frac{1+t^2}{(1-t^2)^2}dt$



      ...but the first formula given at the above link is also supposed to be such a formula, solving for that exact LHS term! So the two would have to be equivalent - IE:



      $int_{a}^{infty}f(x)dx=int_{a}^1 f(frac{t}{1-t^2})frac{1+t^2}{(1-t^2)^2}dt=int_{0}^1 f(a+frac{t}{1-t})frac{1}{(1-t)^2}dt$



      And here I'm stuck, because I can't figure out whether or not that's plausible for all convergent $f(x)$. I have a bad feeling about that whole approach because it relies on the assumption that dividing up a finite space at a given point is the same as dividing up an equivalent infinite space at the exact same point, proportionally.










      share|cite|improve this question











      $endgroup$




      I found a fantastic and generalizable substitution technique for computing definite integrals that go to infinity from either negative infinity or a constant, regardless of the function (sorry for the external link):



      http://ab-initio.mit.edu/wiki/index.php/Cubature#Infinite_intervals



      But what's killing me is that I need the same sort of thing for a function going from negative infinity to a constant, and I can't convince myself that some obvious transformation of either of these two is correct. Doing u-substitution on any given integrand to take care of a (negative) infinite bound is simple enough, but a general transformation rule like one of the ones in the link - totally independent of the function itself - would be invaluable.



      Edit 1 (Might be a Wild Goose Chase)



      So the second formula up in that link, is:



      $int_{-infty}^{infty}f(x)dx=int_{-1}^1 f(frac{t}{1-t^2})frac{1+t^2}{(1-t^2)^2}dt$



      If $a$ represents our generic real-number constant, the above could certainly be broken up as:



      $int_{-infty}^{infty}f(x)dx=int_{-1}^a f(frac{t}{1-t^2})frac{1+t^2}{(1-t^2)^2}dt+int_{a}^1 f(frac{t}{1-t^2})frac{1+t^2}{(1-t^2)^2}dt$



      Which tempts me to jump to the conclusion that the first term on the RHS can be used as our general negative-infinity-to-constant formula:



      $int_{-infty}^{a}f(x)dx=int_{-1}^a f(frac{t}{1-t^2})frac{1+t^2}{(1-t^2)^2}dt$



      In order for this to be true, however, the second RHS term would have to complement it by being a valid formula to integrate from any constant up to infinity, IE:



      $int_{a}^{infty}f(x)dx=int_{a}^1 f(frac{t}{1-t^2})frac{1+t^2}{(1-t^2)^2}dt$



      ...but the first formula given at the above link is also supposed to be such a formula, solving for that exact LHS term! So the two would have to be equivalent - IE:



      $int_{a}^{infty}f(x)dx=int_{a}^1 f(frac{t}{1-t^2})frac{1+t^2}{(1-t^2)^2}dt=int_{0}^1 f(a+frac{t}{1-t})frac{1}{(1-t)^2}dt$



      And here I'm stuck, because I can't figure out whether or not that's plausible for all convergent $f(x)$. I have a bad feeling about that whole approach because it relies on the assumption that dividing up a finite space at a given point is the same as dividing up an equivalent infinite space at the exact same point, proportionally.







      integration infinity substitution






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      edited Aug 4 '15 at 20:16







      DHW

















      asked Aug 4 '15 at 18:44









      DHWDHW

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          $begingroup$

          From the wikipedia page for integration by substitution, you need a differentiable function $varphi$ with integrable derivative. If $f$ is continuous, then



          $$ int_{varphi(a)}^{varphi(b)} f(x) dx = int_a^b f(varphi(x)) varphi'(x) dx$$



          As long as $varphi(a) = -infty$ and $varphi(b) = c$, it should work.
          Some functions you can use are:



          $$ varphi(x) = c + 1 - frac{1}{x} $$
          $$ int_{-infty}^{c} f(x) dx = int_0^1 fleft(c + 1 - frac{1}{x} right) frac{1}{x^2} dx$$
          $$ varphi(x) = c + log(x) $$
          $$ int_{-infty}^{c} f(x) dx = int_0^1 f(c + log(x)) frac{1}{x} dx$$






          share|cite|improve this answer









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            $begingroup$

            From the wikipedia page for integration by substitution, you need a differentiable function $varphi$ with integrable derivative. If $f$ is continuous, then



            $$ int_{varphi(a)}^{varphi(b)} f(x) dx = int_a^b f(varphi(x)) varphi'(x) dx$$



            As long as $varphi(a) = -infty$ and $varphi(b) = c$, it should work.
            Some functions you can use are:



            $$ varphi(x) = c + 1 - frac{1}{x} $$
            $$ int_{-infty}^{c} f(x) dx = int_0^1 fleft(c + 1 - frac{1}{x} right) frac{1}{x^2} dx$$
            $$ varphi(x) = c + log(x) $$
            $$ int_{-infty}^{c} f(x) dx = int_0^1 f(c + log(x)) frac{1}{x} dx$$






            share|cite|improve this answer









            $endgroup$


















              0












              $begingroup$

              From the wikipedia page for integration by substitution, you need a differentiable function $varphi$ with integrable derivative. If $f$ is continuous, then



              $$ int_{varphi(a)}^{varphi(b)} f(x) dx = int_a^b f(varphi(x)) varphi'(x) dx$$



              As long as $varphi(a) = -infty$ and $varphi(b) = c$, it should work.
              Some functions you can use are:



              $$ varphi(x) = c + 1 - frac{1}{x} $$
              $$ int_{-infty}^{c} f(x) dx = int_0^1 fleft(c + 1 - frac{1}{x} right) frac{1}{x^2} dx$$
              $$ varphi(x) = c + log(x) $$
              $$ int_{-infty}^{c} f(x) dx = int_0^1 f(c + log(x)) frac{1}{x} dx$$






              share|cite|improve this answer









              $endgroup$
















                0












                0








                0





                $begingroup$

                From the wikipedia page for integration by substitution, you need a differentiable function $varphi$ with integrable derivative. If $f$ is continuous, then



                $$ int_{varphi(a)}^{varphi(b)} f(x) dx = int_a^b f(varphi(x)) varphi'(x) dx$$



                As long as $varphi(a) = -infty$ and $varphi(b) = c$, it should work.
                Some functions you can use are:



                $$ varphi(x) = c + 1 - frac{1}{x} $$
                $$ int_{-infty}^{c} f(x) dx = int_0^1 fleft(c + 1 - frac{1}{x} right) frac{1}{x^2} dx$$
                $$ varphi(x) = c + log(x) $$
                $$ int_{-infty}^{c} f(x) dx = int_0^1 f(c + log(x)) frac{1}{x} dx$$






                share|cite|improve this answer









                $endgroup$



                From the wikipedia page for integration by substitution, you need a differentiable function $varphi$ with integrable derivative. If $f$ is continuous, then



                $$ int_{varphi(a)}^{varphi(b)} f(x) dx = int_a^b f(varphi(x)) varphi'(x) dx$$



                As long as $varphi(a) = -infty$ and $varphi(b) = c$, it should work.
                Some functions you can use are:



                $$ varphi(x) = c + 1 - frac{1}{x} $$
                $$ int_{-infty}^{c} f(x) dx = int_0^1 fleft(c + 1 - frac{1}{x} right) frac{1}{x^2} dx$$
                $$ varphi(x) = c + log(x) $$
                $$ int_{-infty}^{c} f(x) dx = int_0^1 f(c + log(x)) frac{1}{x} dx$$







                share|cite|improve this answer












                share|cite|improve this answer



                share|cite|improve this answer










                answered Dec 13 '18 at 3:39









                slek120slek120

                101




                101






























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