Error propagation of a variable for an integral

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  • Thread starter Arman777
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  • #1
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I have an integral that depends on two parameters ##a\pm\delta a## and ##b\pm \delta b##. I am doing this integral numerically and no python function can calculate the integral with uncertainties.

So I have calculated the integral for each min, max values of a and b.
As a result I have obtained 4 values, such that;

$$(a + \delta a, b + \delta b) = 13827.450210 \pm 0.000015~~(1)$$
$$(a + \delta a, b - \delta b) = 13827.354688 \pm 0.000015~~(2)$$
$$(a - \delta a, b + \delta b) = 13912.521548 \pm 0.000010~~(3)$$
$$(a - \delta a, b - \delta b) = 13912.425467 \pm 0.000010~~(4)$$

So it is clear that ##(2)## gives the min and ##(3)## gives the max. Let us show the result of the integral as ##c \pm \delta c##. So my problem is what is ##c## and ##\delta c## here?

The integral is something like this

$$I(a,b,x) =C\int_0^b \frac{dx}{\sqrt{a(1+x)^3 + \eta(1+x)^4 + (\gamma^2 - a - \eta)}}$$

where ##\eta## and ##\gamma## are constant.

Note: You guys can also generalize it by taking ##\eta \pm \delta \eta## but it is not necessary for now.

I have to take derivatives or integrals numerically. There's no known analytical solution for the integral.

##\eta = 4.177 \times 10^{-5}##, ##a = 0.1430 \pm 0.0011##, ##b = 1089.92 \pm 0.25##, ##\gamma = 0.6736 \pm 0.0054##, ##C = 2997.92458##
 
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Answers and Replies

  • #2
pasmith
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Generally, if your intergal is [itex]I(a,b) = \int_{x_0}^{x_1} F(a,b,x)\,dx[/itex], then uncertainties in [itex]a[/itex] and [itex]b[/itex] would lead to [tex]I(a,b)
\pm\frac{\partial I}{\partial a}\delta a \pm \frac{\partial I}{\partial b}\delta b[/tex] with the partial derivatives evaluated at [itex]a[/itex] and [itex]b[/itex]. You can evaluate these derivatives by differentiating under the integral:
[tex]
\frac{\partial I}{\partial a} = \int_{x_0}^{x_1} \frac{\partial F}{\partial a}(a, b, x)\,dx[/tex] etc.
 
  • #3
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The integral is something like this

$$I(a,b,x) =\int_0^b \frac{dx}{\sqrt{a(1+x)^3 + \eta(1+x)^4 + (\gamma^2 - a - \eta)}}$$

where ##\eta## and ##\gamma## are constant.
 
  • #4
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Assuming a and b are uncorrelated: Calculate the integral at (a,b+delta_b), (a,b-delta_b) and analogous for delta_a. Then use the deviations as approximation for ##\frac{\partial I}{\partial b}\delta b## and add both uncertainties in quadrature.
 
  • #5
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Assuming a and b are uncorrelated: Calculate the integral at (a,b+delta_b), (a,b-delta_b) and analogous for delta_a. Then use the deviations as approximation for ##\frac{\partial I}{\partial b}\delta b## and add both uncertainties in quadrature.
I did not quite understand it..Can you maybe put it in a more mathematical way
 
  • #6
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Code:
  from numpy import sqrt
    from scipy import integrate
    import uncertainties as u
    from uncertainties.umath import *

    #Important Parameters
    C = 2997.92458  # speed of light in [km/s]
    eta = 4.177 * 10**(-5)
    a = u.ufloat(0.1430, 0.0011)
    b = u.ufloat(1089.92, 0.25)
    gama = u.ufloat(0.6736, 0.0054)

    @u.wrap
    def D_zrec_finder(gama, a, b):
        def D_zrec(z):
            return C / sqrt(a * (1+z)**3 + eta * (1+z)**4 + (gama**2 - a - eta))
        result, error = integrate.quad(D_zrec, 0, b)
        return result


    print((D_zrec_finder(gama, a, b)).n)
    print((D_zrec_finder(gama, a, b)).s)

This works
 
  • #7
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I did not quite understand it..Can you maybe put it in a more mathematical way
$$\frac{\partial I}{\partial b}\delta b \approx \frac 1 2 (I(a,b+\delta b)-I(a,b-\delta b))$$
$$\frac{\partial I}{\partial a}\delta a \approx \frac 1 2 (I(a+\delta a,b)-I(a-\delta a,b))$$

As b is your integration border you can simplify this one: ##\frac{\partial I}{\partial b}## is simply the function value at x=b.
 

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