Let $C in mathbbR^n$ be a Jordan mensurable set of measure zero. Show that $int_A chi_C = 0$, for every closed rectangle $A supset C$.

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Let $C in mathbbR^n$ be a Jordan mensurable set of measure zero. Show that $int_A chi_C = 0$, for every closed rectangle $A supset C$.



A subset $A$ of $mathbbR^n$ has measure 0 if for every $epsilon > 0$ there is a cover $U_1, U_2,... $ of A by closed rectangles such that $sum_i=1^inftyv(U_i) < epsilon.$



A bounded set C is called Jordan-measurable if for every closed rectangle A such that $C subset A$ we have that $chi_C: A to mathbbR$ (given by $chi_C(x) = 1$ if $x in C$, and $chi_C(x) = 0$ if $x in A-C$) is integrable. In this case $v(C) = int_A chi_C$




The only thing I know is that by hypothesis we have that $int_A chi_C = v(C)$. I am really bad in analysis.



Any help would be great.







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    Let $C in mathbbR^n$ be a Jordan mensurable set of measure zero. Show that $int_A chi_C = 0$, for every closed rectangle $A supset C$.



    A subset $A$ of $mathbbR^n$ has measure 0 if for every $epsilon > 0$ there is a cover $U_1, U_2,... $ of A by closed rectangles such that $sum_i=1^inftyv(U_i) < epsilon.$



    A bounded set C is called Jordan-measurable if for every closed rectangle A such that $C subset A$ we have that $chi_C: A to mathbbR$ (given by $chi_C(x) = 1$ if $x in C$, and $chi_C(x) = 0$ if $x in A-C$) is integrable. In this case $v(C) = int_A chi_C$




    The only thing I know is that by hypothesis we have that $int_A chi_C = v(C)$. I am really bad in analysis.



    Any help would be great.







    share|cite|improve this question























      up vote
      0
      down vote

      favorite









      up vote
      0
      down vote

      favorite











      Let $C in mathbbR^n$ be a Jordan mensurable set of measure zero. Show that $int_A chi_C = 0$, for every closed rectangle $A supset C$.



      A subset $A$ of $mathbbR^n$ has measure 0 if for every $epsilon > 0$ there is a cover $U_1, U_2,... $ of A by closed rectangles such that $sum_i=1^inftyv(U_i) < epsilon.$



      A bounded set C is called Jordan-measurable if for every closed rectangle A such that $C subset A$ we have that $chi_C: A to mathbbR$ (given by $chi_C(x) = 1$ if $x in C$, and $chi_C(x) = 0$ if $x in A-C$) is integrable. In this case $v(C) = int_A chi_C$




      The only thing I know is that by hypothesis we have that $int_A chi_C = v(C)$. I am really bad in analysis.



      Any help would be great.







      share|cite|improve this question













      Let $C in mathbbR^n$ be a Jordan mensurable set of measure zero. Show that $int_A chi_C = 0$, for every closed rectangle $A supset C$.



      A subset $A$ of $mathbbR^n$ has measure 0 if for every $epsilon > 0$ there is a cover $U_1, U_2,... $ of A by closed rectangles such that $sum_i=1^inftyv(U_i) < epsilon.$



      A bounded set C is called Jordan-measurable if for every closed rectangle A such that $C subset A$ we have that $chi_C: A to mathbbR$ (given by $chi_C(x) = 1$ if $x in C$, and $chi_C(x) = 0$ if $x in A-C$) is integrable. In this case $v(C) = int_A chi_C$




      The only thing I know is that by hypothesis we have that $int_A chi_C = v(C)$. I am really bad in analysis.



      Any help would be great.









      share|cite|improve this question












      share|cite|improve this question




      share|cite|improve this question








      edited Jul 15 at 2:48
























      asked Jul 15 at 2:23









      P.G

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          We can write A as $Ccup (A - C)$ and we can express the integral as $int_A chi_C = int_C chi_C + int_A-Cchi_C$.



          By the definition of $chi_C$, we have that $chi_C=0$ on $A-C$, so the second integral of the sum is zero. Then $int_A chi_C = int_C chi_C = v(C)$. Which is zero because C has measure zero (or alternatively we can show by the definition that $v(C)$ is less than $epsilon$ for every $epsilon > 0$






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            active

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            up vote
            2
            down vote



            accepted










            We can write A as $Ccup (A - C)$ and we can express the integral as $int_A chi_C = int_C chi_C + int_A-Cchi_C$.



            By the definition of $chi_C$, we have that $chi_C=0$ on $A-C$, so the second integral of the sum is zero. Then $int_A chi_C = int_C chi_C = v(C)$. Which is zero because C has measure zero (or alternatively we can show by the definition that $v(C)$ is less than $epsilon$ for every $epsilon > 0$






            share|cite|improve this answer

























              up vote
              2
              down vote



              accepted










              We can write A as $Ccup (A - C)$ and we can express the integral as $int_A chi_C = int_C chi_C + int_A-Cchi_C$.



              By the definition of $chi_C$, we have that $chi_C=0$ on $A-C$, so the second integral of the sum is zero. Then $int_A chi_C = int_C chi_C = v(C)$. Which is zero because C has measure zero (or alternatively we can show by the definition that $v(C)$ is less than $epsilon$ for every $epsilon > 0$






              share|cite|improve this answer























                up vote
                2
                down vote



                accepted







                up vote
                2
                down vote



                accepted






                We can write A as $Ccup (A - C)$ and we can express the integral as $int_A chi_C = int_C chi_C + int_A-Cchi_C$.



                By the definition of $chi_C$, we have that $chi_C=0$ on $A-C$, so the second integral of the sum is zero. Then $int_A chi_C = int_C chi_C = v(C)$. Which is zero because C has measure zero (or alternatively we can show by the definition that $v(C)$ is less than $epsilon$ for every $epsilon > 0$






                share|cite|improve this answer













                We can write A as $Ccup (A - C)$ and we can express the integral as $int_A chi_C = int_C chi_C + int_A-Cchi_C$.



                By the definition of $chi_C$, we have that $chi_C=0$ on $A-C$, so the second integral of the sum is zero. Then $int_A chi_C = int_C chi_C = v(C)$. Which is zero because C has measure zero (or alternatively we can show by the definition that $v(C)$ is less than $epsilon$ for every $epsilon > 0$







                share|cite|improve this answer













                share|cite|improve this answer



                share|cite|improve this answer











                answered Jul 15 at 4:21









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