A segment is removed from a semi circle what is the pdf of the remaining area?

The name of the pictureThe name of the pictureThe name of the pictureClash Royale CLAN TAG#URR8PPP











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Question:
Given the illustration below, the cdf of Z is
beginequation
Pr(Zleq z) = fractextexp(-lambda A_z)-textexp(-N/2)1-textexp(-N/2)
endequation



How could one Prove that



beginequation
f_z(Z) = frac2lambda sqrtR^2-z^21-textexp(-N/2) textexp[-lambda A_z]
endequation

for $0<zleq R$



where $A_z$ = $R^2 [cos^-1 (z/R)- (z/R)sqrt1-(z/R)^2]$



Challenge:
The first problem I have is understanding how $A_z$ was derived, then, how the numerator of the first equation of the pdf was gotten. The closest clue I have to $A_z$ is this question and this one, but here, the height of the segment here is unknown.



In case it might interest someone, $N = lambda pi R^2$ and $lambda$ represents the density of a two dimensional Poisson Point Process



pix







share|cite|improve this question

























    up vote
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    Question:
    Given the illustration below, the cdf of Z is
    beginequation
    Pr(Zleq z) = fractextexp(-lambda A_z)-textexp(-N/2)1-textexp(-N/2)
    endequation



    How could one Prove that



    beginequation
    f_z(Z) = frac2lambda sqrtR^2-z^21-textexp(-N/2) textexp[-lambda A_z]
    endequation

    for $0<zleq R$



    where $A_z$ = $R^2 [cos^-1 (z/R)- (z/R)sqrt1-(z/R)^2]$



    Challenge:
    The first problem I have is understanding how $A_z$ was derived, then, how the numerator of the first equation of the pdf was gotten. The closest clue I have to $A_z$ is this question and this one, but here, the height of the segment here is unknown.



    In case it might interest someone, $N = lambda pi R^2$ and $lambda$ represents the density of a two dimensional Poisson Point Process



    pix







    share|cite|improve this question























      up vote
      1
      down vote

      favorite
      1









      up vote
      1
      down vote

      favorite
      1






      1





      Question:
      Given the illustration below, the cdf of Z is
      beginequation
      Pr(Zleq z) = fractextexp(-lambda A_z)-textexp(-N/2)1-textexp(-N/2)
      endequation



      How could one Prove that



      beginequation
      f_z(Z) = frac2lambda sqrtR^2-z^21-textexp(-N/2) textexp[-lambda A_z]
      endequation

      for $0<zleq R$



      where $A_z$ = $R^2 [cos^-1 (z/R)- (z/R)sqrt1-(z/R)^2]$



      Challenge:
      The first problem I have is understanding how $A_z$ was derived, then, how the numerator of the first equation of the pdf was gotten. The closest clue I have to $A_z$ is this question and this one, but here, the height of the segment here is unknown.



      In case it might interest someone, $N = lambda pi R^2$ and $lambda$ represents the density of a two dimensional Poisson Point Process



      pix







      share|cite|improve this question













      Question:
      Given the illustration below, the cdf of Z is
      beginequation
      Pr(Zleq z) = fractextexp(-lambda A_z)-textexp(-N/2)1-textexp(-N/2)
      endequation



      How could one Prove that



      beginequation
      f_z(Z) = frac2lambda sqrtR^2-z^21-textexp(-N/2) textexp[-lambda A_z]
      endequation

      for $0<zleq R$



      where $A_z$ = $R^2 [cos^-1 (z/R)- (z/R)sqrt1-(z/R)^2]$



      Challenge:
      The first problem I have is understanding how $A_z$ was derived, then, how the numerator of the first equation of the pdf was gotten. The closest clue I have to $A_z$ is this question and this one, but here, the height of the segment here is unknown.



      In case it might interest someone, $N = lambda pi R^2$ and $lambda$ represents the density of a two dimensional Poisson Point Process



      pix









      share|cite|improve this question












      share|cite|improve this question




      share|cite|improve this question








      edited Jul 24 at 9:30
























      asked Jul 24 at 6:50









      Abdulhameed

      54111




      54111




















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          accepted










          I understand that you have already recognised that this problem can be solved by using the identity relating the PDF of a distribution to the CDF: $ f_Z(z) = F_Z'(z)$,
          which for your particular CDF is equivalent to:



          $$ f_Z(z) = frac-lambda A'(z) exp(-lambda A(z))1- exp(-N/2).$$



          So it remains to calculate $A(z)$, and then use this to derive $A'(z)$.




          Calculating A(z)



          In the following I refer to my diagram (unfortunately not as well produced as your graphic, but you should get the point).enter image description here



          Let $theta_z$ denote the angle made between $A hat O B$, using the standard trigonometric identify for the cosine we have that



          $$theta_z = cos^-1(z/R).$$



          Therefore the area of the circular wedge with angle $2theta_z$ (i.e. the wedge bounded by the lines $OB$ and $OC$) is



          beginalignedW_z &= pi R^2 times frac2theta_z2 pi \
          & = R^2 theta_z \
          & = R^2 cos^-1(z/R).
          endaligned



          We can now obtain $A(z)$ by subtracting from $W_z$ the area, $T_z$, of the triangle made out by the lines $OBCO$, which is equal to the area of the rectangle with side lengths equal to those of the line segments $OA$ and $AB$.



          Since $A$ has coordinates $(z,0)$ the line segment $OA$ has length $z$; we can calculate the coordinates of $B$ by relying on the formula $x^2 + y^2 = R^2$, which gives coordinates $(z, sqrtR^2 - z^2)$, and so the length of $AB$ is $sqrtR^2 - z^2$. Combining these we get



          $$T_z = z sqrtR^2 - z^2$$,



          and further more



          beginaligned
          A(z) &= W_z - T_z \
          & = R^2 cos^-1(z/R) - z sqrtR^2 - z^2 \
          & = R^2 left( cos^-1(z/R) - (z/R) sqrt1 - (z/R)^2 right),
          endaligned
          which is as you gave in the question statement.




          Calculating $A'(z)$



          This now follows from appealing to standard identities for derivatives. If we denote



          $$g(x) = cos^-1(x) - x sqrt1 - x^2,$$



          then we have $A(z) = R^2 g(z/R)$, and so using the chain rule:



          beginaligned
          A'(z) & = R^2 fracddz g(z/R) \
          & = R^2 g'(z/R) fracddz left(fraczRright) \
          & = R g'(z/R).
          endaligned
          So concentrating on $g(x)$ we differentiate this using the identity for the derivative of $cos^-1$, as well as the product rule to handle the second term to obtain:



          $$g'(x) = - frac1sqrt1-x^2 - frac1-2x^2sqrt1-x^2, $$
          where the first term above is contributed from $cos^-1$, and the second is from the product term. Rearranging this we have
          beginaligned
          g'(x) &= -2frac1 - x^2sqrt1-x^2 \
          & = -2 sqrt1 - x^2.
          endaligned
          And so we have



          beginaligned
          A'(z) &= Rg'(z/R) \
          & = -2R sqrt1 - (z/R)^2 \
          & = -2 sqrtR^2 - z^2.
          endaligned



          Substituting this into the original formula provided for $f_Z(z)$ gives the desired answer.






          share|cite|improve this answer























          • Thanks for this brilliant answer. Please could you add some detail on how $A'(z) = R g'(z/R).$ was gotten using the chain rule. I didn't get that part well even with my basic knowledge of the chain rule.
            – Abdulhameed
            Jul 25 at 0:09






          • 1




            I have added a few lines breaking down the chain rule calculation.
            – owen88
            Jul 25 at 14:50










          • Those lines are well appreciated and understood. Thank you very much
            – Abdulhameed
            Jul 26 at 3:49










          Your Answer




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          1 Answer
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          1 Answer
          1






          active

          oldest

          votes









          active

          oldest

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          active

          oldest

          votes








          up vote
          1
          down vote



          accepted










          I understand that you have already recognised that this problem can be solved by using the identity relating the PDF of a distribution to the CDF: $ f_Z(z) = F_Z'(z)$,
          which for your particular CDF is equivalent to:



          $$ f_Z(z) = frac-lambda A'(z) exp(-lambda A(z))1- exp(-N/2).$$



          So it remains to calculate $A(z)$, and then use this to derive $A'(z)$.




          Calculating A(z)



          In the following I refer to my diagram (unfortunately not as well produced as your graphic, but you should get the point).enter image description here



          Let $theta_z$ denote the angle made between $A hat O B$, using the standard trigonometric identify for the cosine we have that



          $$theta_z = cos^-1(z/R).$$



          Therefore the area of the circular wedge with angle $2theta_z$ (i.e. the wedge bounded by the lines $OB$ and $OC$) is



          beginalignedW_z &= pi R^2 times frac2theta_z2 pi \
          & = R^2 theta_z \
          & = R^2 cos^-1(z/R).
          endaligned



          We can now obtain $A(z)$ by subtracting from $W_z$ the area, $T_z$, of the triangle made out by the lines $OBCO$, which is equal to the area of the rectangle with side lengths equal to those of the line segments $OA$ and $AB$.



          Since $A$ has coordinates $(z,0)$ the line segment $OA$ has length $z$; we can calculate the coordinates of $B$ by relying on the formula $x^2 + y^2 = R^2$, which gives coordinates $(z, sqrtR^2 - z^2)$, and so the length of $AB$ is $sqrtR^2 - z^2$. Combining these we get



          $$T_z = z sqrtR^2 - z^2$$,



          and further more



          beginaligned
          A(z) &= W_z - T_z \
          & = R^2 cos^-1(z/R) - z sqrtR^2 - z^2 \
          & = R^2 left( cos^-1(z/R) - (z/R) sqrt1 - (z/R)^2 right),
          endaligned
          which is as you gave in the question statement.




          Calculating $A'(z)$



          This now follows from appealing to standard identities for derivatives. If we denote



          $$g(x) = cos^-1(x) - x sqrt1 - x^2,$$



          then we have $A(z) = R^2 g(z/R)$, and so using the chain rule:



          beginaligned
          A'(z) & = R^2 fracddz g(z/R) \
          & = R^2 g'(z/R) fracddz left(fraczRright) \
          & = R g'(z/R).
          endaligned
          So concentrating on $g(x)$ we differentiate this using the identity for the derivative of $cos^-1$, as well as the product rule to handle the second term to obtain:



          $$g'(x) = - frac1sqrt1-x^2 - frac1-2x^2sqrt1-x^2, $$
          where the first term above is contributed from $cos^-1$, and the second is from the product term. Rearranging this we have
          beginaligned
          g'(x) &= -2frac1 - x^2sqrt1-x^2 \
          & = -2 sqrt1 - x^2.
          endaligned
          And so we have



          beginaligned
          A'(z) &= Rg'(z/R) \
          & = -2R sqrt1 - (z/R)^2 \
          & = -2 sqrtR^2 - z^2.
          endaligned



          Substituting this into the original formula provided for $f_Z(z)$ gives the desired answer.






          share|cite|improve this answer























          • Thanks for this brilliant answer. Please could you add some detail on how $A'(z) = R g'(z/R).$ was gotten using the chain rule. I didn't get that part well even with my basic knowledge of the chain rule.
            – Abdulhameed
            Jul 25 at 0:09






          • 1




            I have added a few lines breaking down the chain rule calculation.
            – owen88
            Jul 25 at 14:50










          • Those lines are well appreciated and understood. Thank you very much
            – Abdulhameed
            Jul 26 at 3:49














          up vote
          1
          down vote



          accepted










          I understand that you have already recognised that this problem can be solved by using the identity relating the PDF of a distribution to the CDF: $ f_Z(z) = F_Z'(z)$,
          which for your particular CDF is equivalent to:



          $$ f_Z(z) = frac-lambda A'(z) exp(-lambda A(z))1- exp(-N/2).$$



          So it remains to calculate $A(z)$, and then use this to derive $A'(z)$.




          Calculating A(z)



          In the following I refer to my diagram (unfortunately not as well produced as your graphic, but you should get the point).enter image description here



          Let $theta_z$ denote the angle made between $A hat O B$, using the standard trigonometric identify for the cosine we have that



          $$theta_z = cos^-1(z/R).$$



          Therefore the area of the circular wedge with angle $2theta_z$ (i.e. the wedge bounded by the lines $OB$ and $OC$) is



          beginalignedW_z &= pi R^2 times frac2theta_z2 pi \
          & = R^2 theta_z \
          & = R^2 cos^-1(z/R).
          endaligned



          We can now obtain $A(z)$ by subtracting from $W_z$ the area, $T_z$, of the triangle made out by the lines $OBCO$, which is equal to the area of the rectangle with side lengths equal to those of the line segments $OA$ and $AB$.



          Since $A$ has coordinates $(z,0)$ the line segment $OA$ has length $z$; we can calculate the coordinates of $B$ by relying on the formula $x^2 + y^2 = R^2$, which gives coordinates $(z, sqrtR^2 - z^2)$, and so the length of $AB$ is $sqrtR^2 - z^2$. Combining these we get



          $$T_z = z sqrtR^2 - z^2$$,



          and further more



          beginaligned
          A(z) &= W_z - T_z \
          & = R^2 cos^-1(z/R) - z sqrtR^2 - z^2 \
          & = R^2 left( cos^-1(z/R) - (z/R) sqrt1 - (z/R)^2 right),
          endaligned
          which is as you gave in the question statement.




          Calculating $A'(z)$



          This now follows from appealing to standard identities for derivatives. If we denote



          $$g(x) = cos^-1(x) - x sqrt1 - x^2,$$



          then we have $A(z) = R^2 g(z/R)$, and so using the chain rule:



          beginaligned
          A'(z) & = R^2 fracddz g(z/R) \
          & = R^2 g'(z/R) fracddz left(fraczRright) \
          & = R g'(z/R).
          endaligned
          So concentrating on $g(x)$ we differentiate this using the identity for the derivative of $cos^-1$, as well as the product rule to handle the second term to obtain:



          $$g'(x) = - frac1sqrt1-x^2 - frac1-2x^2sqrt1-x^2, $$
          where the first term above is contributed from $cos^-1$, and the second is from the product term. Rearranging this we have
          beginaligned
          g'(x) &= -2frac1 - x^2sqrt1-x^2 \
          & = -2 sqrt1 - x^2.
          endaligned
          And so we have



          beginaligned
          A'(z) &= Rg'(z/R) \
          & = -2R sqrt1 - (z/R)^2 \
          & = -2 sqrtR^2 - z^2.
          endaligned



          Substituting this into the original formula provided for $f_Z(z)$ gives the desired answer.






          share|cite|improve this answer























          • Thanks for this brilliant answer. Please could you add some detail on how $A'(z) = R g'(z/R).$ was gotten using the chain rule. I didn't get that part well even with my basic knowledge of the chain rule.
            – Abdulhameed
            Jul 25 at 0:09






          • 1




            I have added a few lines breaking down the chain rule calculation.
            – owen88
            Jul 25 at 14:50










          • Those lines are well appreciated and understood. Thank you very much
            – Abdulhameed
            Jul 26 at 3:49












          up vote
          1
          down vote



          accepted







          up vote
          1
          down vote



          accepted






          I understand that you have already recognised that this problem can be solved by using the identity relating the PDF of a distribution to the CDF: $ f_Z(z) = F_Z'(z)$,
          which for your particular CDF is equivalent to:



          $$ f_Z(z) = frac-lambda A'(z) exp(-lambda A(z))1- exp(-N/2).$$



          So it remains to calculate $A(z)$, and then use this to derive $A'(z)$.




          Calculating A(z)



          In the following I refer to my diagram (unfortunately not as well produced as your graphic, but you should get the point).enter image description here



          Let $theta_z$ denote the angle made between $A hat O B$, using the standard trigonometric identify for the cosine we have that



          $$theta_z = cos^-1(z/R).$$



          Therefore the area of the circular wedge with angle $2theta_z$ (i.e. the wedge bounded by the lines $OB$ and $OC$) is



          beginalignedW_z &= pi R^2 times frac2theta_z2 pi \
          & = R^2 theta_z \
          & = R^2 cos^-1(z/R).
          endaligned



          We can now obtain $A(z)$ by subtracting from $W_z$ the area, $T_z$, of the triangle made out by the lines $OBCO$, which is equal to the area of the rectangle with side lengths equal to those of the line segments $OA$ and $AB$.



          Since $A$ has coordinates $(z,0)$ the line segment $OA$ has length $z$; we can calculate the coordinates of $B$ by relying on the formula $x^2 + y^2 = R^2$, which gives coordinates $(z, sqrtR^2 - z^2)$, and so the length of $AB$ is $sqrtR^2 - z^2$. Combining these we get



          $$T_z = z sqrtR^2 - z^2$$,



          and further more



          beginaligned
          A(z) &= W_z - T_z \
          & = R^2 cos^-1(z/R) - z sqrtR^2 - z^2 \
          & = R^2 left( cos^-1(z/R) - (z/R) sqrt1 - (z/R)^2 right),
          endaligned
          which is as you gave in the question statement.




          Calculating $A'(z)$



          This now follows from appealing to standard identities for derivatives. If we denote



          $$g(x) = cos^-1(x) - x sqrt1 - x^2,$$



          then we have $A(z) = R^2 g(z/R)$, and so using the chain rule:



          beginaligned
          A'(z) & = R^2 fracddz g(z/R) \
          & = R^2 g'(z/R) fracddz left(fraczRright) \
          & = R g'(z/R).
          endaligned
          So concentrating on $g(x)$ we differentiate this using the identity for the derivative of $cos^-1$, as well as the product rule to handle the second term to obtain:



          $$g'(x) = - frac1sqrt1-x^2 - frac1-2x^2sqrt1-x^2, $$
          where the first term above is contributed from $cos^-1$, and the second is from the product term. Rearranging this we have
          beginaligned
          g'(x) &= -2frac1 - x^2sqrt1-x^2 \
          & = -2 sqrt1 - x^2.
          endaligned
          And so we have



          beginaligned
          A'(z) &= Rg'(z/R) \
          & = -2R sqrt1 - (z/R)^2 \
          & = -2 sqrtR^2 - z^2.
          endaligned



          Substituting this into the original formula provided for $f_Z(z)$ gives the desired answer.






          share|cite|improve this answer















          I understand that you have already recognised that this problem can be solved by using the identity relating the PDF of a distribution to the CDF: $ f_Z(z) = F_Z'(z)$,
          which for your particular CDF is equivalent to:



          $$ f_Z(z) = frac-lambda A'(z) exp(-lambda A(z))1- exp(-N/2).$$



          So it remains to calculate $A(z)$, and then use this to derive $A'(z)$.




          Calculating A(z)



          In the following I refer to my diagram (unfortunately not as well produced as your graphic, but you should get the point).enter image description here



          Let $theta_z$ denote the angle made between $A hat O B$, using the standard trigonometric identify for the cosine we have that



          $$theta_z = cos^-1(z/R).$$



          Therefore the area of the circular wedge with angle $2theta_z$ (i.e. the wedge bounded by the lines $OB$ and $OC$) is



          beginalignedW_z &= pi R^2 times frac2theta_z2 pi \
          & = R^2 theta_z \
          & = R^2 cos^-1(z/R).
          endaligned



          We can now obtain $A(z)$ by subtracting from $W_z$ the area, $T_z$, of the triangle made out by the lines $OBCO$, which is equal to the area of the rectangle with side lengths equal to those of the line segments $OA$ and $AB$.



          Since $A$ has coordinates $(z,0)$ the line segment $OA$ has length $z$; we can calculate the coordinates of $B$ by relying on the formula $x^2 + y^2 = R^2$, which gives coordinates $(z, sqrtR^2 - z^2)$, and so the length of $AB$ is $sqrtR^2 - z^2$. Combining these we get



          $$T_z = z sqrtR^2 - z^2$$,



          and further more



          beginaligned
          A(z) &= W_z - T_z \
          & = R^2 cos^-1(z/R) - z sqrtR^2 - z^2 \
          & = R^2 left( cos^-1(z/R) - (z/R) sqrt1 - (z/R)^2 right),
          endaligned
          which is as you gave in the question statement.




          Calculating $A'(z)$



          This now follows from appealing to standard identities for derivatives. If we denote



          $$g(x) = cos^-1(x) - x sqrt1 - x^2,$$



          then we have $A(z) = R^2 g(z/R)$, and so using the chain rule:



          beginaligned
          A'(z) & = R^2 fracddz g(z/R) \
          & = R^2 g'(z/R) fracddz left(fraczRright) \
          & = R g'(z/R).
          endaligned
          So concentrating on $g(x)$ we differentiate this using the identity for the derivative of $cos^-1$, as well as the product rule to handle the second term to obtain:



          $$g'(x) = - frac1sqrt1-x^2 - frac1-2x^2sqrt1-x^2, $$
          where the first term above is contributed from $cos^-1$, and the second is from the product term. Rearranging this we have
          beginaligned
          g'(x) &= -2frac1 - x^2sqrt1-x^2 \
          & = -2 sqrt1 - x^2.
          endaligned
          And so we have



          beginaligned
          A'(z) &= Rg'(z/R) \
          & = -2R sqrt1 - (z/R)^2 \
          & = -2 sqrtR^2 - z^2.
          endaligned



          Substituting this into the original formula provided for $f_Z(z)$ gives the desired answer.







          share|cite|improve this answer















          share|cite|improve this answer



          share|cite|improve this answer








          edited Jul 25 at 14:50


























          answered Jul 24 at 18:27









          owen88

          3,2731021




          3,2731021











          • Thanks for this brilliant answer. Please could you add some detail on how $A'(z) = R g'(z/R).$ was gotten using the chain rule. I didn't get that part well even with my basic knowledge of the chain rule.
            – Abdulhameed
            Jul 25 at 0:09






          • 1




            I have added a few lines breaking down the chain rule calculation.
            – owen88
            Jul 25 at 14:50










          • Those lines are well appreciated and understood. Thank you very much
            – Abdulhameed
            Jul 26 at 3:49
















          • Thanks for this brilliant answer. Please could you add some detail on how $A'(z) = R g'(z/R).$ was gotten using the chain rule. I didn't get that part well even with my basic knowledge of the chain rule.
            – Abdulhameed
            Jul 25 at 0:09






          • 1




            I have added a few lines breaking down the chain rule calculation.
            – owen88
            Jul 25 at 14:50










          • Those lines are well appreciated and understood. Thank you very much
            – Abdulhameed
            Jul 26 at 3:49















          Thanks for this brilliant answer. Please could you add some detail on how $A'(z) = R g'(z/R).$ was gotten using the chain rule. I didn't get that part well even with my basic knowledge of the chain rule.
          – Abdulhameed
          Jul 25 at 0:09




          Thanks for this brilliant answer. Please could you add some detail on how $A'(z) = R g'(z/R).$ was gotten using the chain rule. I didn't get that part well even with my basic knowledge of the chain rule.
          – Abdulhameed
          Jul 25 at 0:09




          1




          1




          I have added a few lines breaking down the chain rule calculation.
          – owen88
          Jul 25 at 14:50




          I have added a few lines breaking down the chain rule calculation.
          – owen88
          Jul 25 at 14:50












          Those lines are well appreciated and understood. Thank you very much
          – Abdulhameed
          Jul 26 at 3:49




          Those lines are well appreciated and understood. Thank you very much
          – Abdulhameed
          Jul 26 at 3:49












           

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