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Homework #2 Problem #17


  1. We see at right that the sum and the integral differ by the triangular shaped notches near the curve. Let us estimate the area of the difference of the jth column, D, as

    Dj =  integral jj-1 exp(- alpha 2x2) dx - exp(- alpha 2x2)

    That integral is the error function which has no closed form solution except for  Integral(0 to infinity) which, in fact, we're to evaluate in the 2nd part of this problem!

    So we are going to take literally the suggestion that the Dj are triangular and use a triangular area to estimate the difference. Since the base of each column (and triangle) is just one, the triangular area is equal to ½ the height of the triangle, or

    Dj = ½ [ exp(- alpha 2(j-1)2) - exp(- alpha 2j2) ]

    Expanding (j-1)2 gives (j2-2j+1) as additive terms in an the exponential, but we know that ex±y=exe±y, we can factor out exp(- alpha 2j2) leaving

    Dj = ½ exp(- alpha 2j2) * [ exp(+2 alpha 2j- alpha 2) - 1 ]

    Noting that for vanishingly small argument e epsilon  arrow right 1, we can make the term in [...] vanish in the limit that  alpha 2 arrow right 0.

    So it's near-zero values of  alpha that do the trick!

  2. That dxdy elemental area in polar coordinates becomes dr, the small extension of a radial arm, times rd Theta , the small arc length through which d Theta sweeps the arm. And since x and y are always in the first quadrant (it's  Integral(0 to infinity) after all), that means that  Theta ranges from 0 to  pi /2 only. The radius takes on all positive values; negative radii are meaningless.

    Since x and y are independent (as are r and  Theta ), we can take them in and out of one another's integrals at will. So

    I =  Integral(0 to infinity) exp(- alpha 2x2)dx =  Integral(0 to infinity) exp(- alpha 2y2)dy

    then

    I 2 =  Integral(0 to infinity)  Integral(0 to infinity) exp[- alpha 2(x2+y2)] dx dy

    I 2 =  Integral(0 to infinity)  integral 0 pi /2 exp[- alpha 2r2] rdr d Theta

    And if we notice that the derivative of that exponential with respect to r is just

    -2r alpha 2 exp[- alpha 2r2],

    then the integrand becomes nothing more than

    r exp(- alpha 2r2) = -(1/2 alpha 2) d [exp(- alpha 2r2)] / dr

    And the advantage for us is that the integral of a derivative is the derivative's function evaluated at the endpoints!

     Integral(0 to infinity) r exp(- alpha 2r2) dr = - (1/2 alpha 2) [exp(- alpha 2r2) | 0 infinity = - (1/2 alpha 2) (0-1) = + (1/2 alpha 2)

    The other integral is trivial:


    it is  integral 0 pi /2 d Theta =  pi /2

    making the double integral

    I 2 = (1/2 alpha 2)( pi /2) =  pi /4 alpha 2

    or

    I = ( pi )½/2 alpha

    as advertized.

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Chris Parr University of Texas at Dallas Programs in Chemistry, Room Berkner 3.506 P.O. Box 830688 M/S BE2.6 (for snailmail) Richardson, TX 75083-0688
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Last modified 8 October 1996