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The article "Microwave Observations of Daily Antarctic Sea-Ice Edge Expansion and Contribution Rates" (IEEE Geosci. and Remote Sensing Letters,\({\rm{2006: 54 - 58}}\)) states that "The distribution of the daily sea-ice advance/retreat from each sensor is similar and is approximately double exponential." The proposed double exponential distribution has density function \({\rm{f(x) = }}{\rm{.5\lambda }}{{\rm{e}}^{{\rm{ - \lambda lel }}}}\)for\( - \yen < x < \yen \). The standard deviation is given as\({\rm{40}}{\rm{.9\;km}}\).

a. What is the value of the parameter\({\rm{\lambda }}\)?

b. What is the probability that the extent of daily sea ice change is within \({\rm{1}}\) standard deviation of the mean value?

Short Answer

Expert verified

(a) The value of the parameter \({\rm{\lambda }}\)is \({\rm{0}}{\rm{.0348}}\).

(b) The probability is \({\rm{0}}{\rm{.3784}}\).

Step by step solution

01

Definition

Probability simply refers to the likelihood of something occurring. We may talk about the probabilities of particular outcomes—how likely they are—when we're unclear about the result of an event. Statistics is the study of occurrences guided by probability.

02

Calculating the value of the parameter \({\rm{\lambda }}\)

pdf of \({\rm{X}}\) is given, which can also be written as:

Now we first calculate standard deviation of given \({\rm{r}}{\rm{.v}}{\rm{.}}\)

Expected value of \({\rm{f(x)}}\) is given as:

\(\begin{aligned}E(x) &= \int_{{\rm{ - \yen }}}^{\rm{\yen }} {\rm{x}} {\rm{ \times f(x) \times dx}}\\& = \int_{{\rm{ - \yen }}}^{\rm{0}} {{\rm{(0}}{\rm{.5x)}}} \left( {{\rm{\lambda \times }}{{\rm{e}}^{{\rm{\lambda x}}}}} \right){\rm{ \times dx + }}\int_{\rm{0}}^{\rm{\yen }} {{\rm{(0}}{\rm{.5x)}}} \left( {{\rm{\lambda \times }}{{\rm{e}}^{{\rm{ - \lambda x}}}}} \right){\rm{ \times dx}}\end{aligned}\)

If we replace \({\rm{x}}\) by \({\rm{ - t}}\)in the first integral then it is equal to negative of second one. Hence

\({\rm{E(x) = 0}}\)

\(\begin{aligned}{\rm{E}}\left( {{{\rm{x}}^{\rm{2}}}} \right) &= \int_{{\rm{ - \yen }}}^{\rm{\yen }} {{{\rm{x}}^{\rm{2}}}} {\rm{ \times f(x) \times dx}}\\ &= \int_{{\rm{ - \yen }}}^{\rm{0}} {\left( {{\rm{0}}{\rm{.5}}{{\rm{x}}^{\rm{2}}}} \right)} \left( {{\rm{\lambda \times }}{{\rm{e}}^{{\rm{\lambda x}}}}} \right){\rm{ \times dx + }}\int_{\rm{0}}^{\rm{\yen }} {\left( {{\rm{0}}{\rm{.5}}{{\rm{x}}^{\rm{2}}}} \right)} \left( {{\rm{\lambda \times }}{{\rm{e}}^{{\rm{ - \lambda x}}}}} \right){\rm{ \times dx}}\end{aligned}\)

03

Calculating the value of the parameter \({\rm{\lambda }}\)

If we replace \({\rm{x}}\) by \({\rm{ - t}}\) in the first integral then it is equal to second integral. Hence

\(\begin{aligned} &= 2\int_{\text{0}}^{\text{¥}} {\left( {{\text{0}}{\text{.5}}{{\text{x}}^{\text{2}}}} \right)} \left( {{\text{λ x }}{{\text{e}}^{{\text{ - λ x}}}}} \right){\text{ x dx}} \\ &= \int_{\text{0}}^{\text{¥}} {{{\text{x}}^{\text{2}}}} \left( {{\text{λ x }}{{\text{e}}^{{\text{ - λ x}}}}} \right){\text{ x dx}} \\ &= \left[ {\left( {{{\text{x}}^{\text{2}}}} \right)\left( {{\text{ - }}{{\text{e}}^{{\text{ - λ x}}}}} \right)} \right]_{\text{0}}^{\text{¥}}{\text{ - }}\int_{\text{0}}^{\text{¥}} {{\text{(2x)}}} \left( {{\text{ - }}{{\text{e}}^{{\text{ - λ x}}}}} \right) \\ &= 0 + 2\left( {\int_{\text{0}}^{\text{¥}} {{{\text{e}}^{{\text{ - λx}}}}} } \right) \\& = 2\left[ {{\text{x}}\left( {{\text{ - }}{{\text{e}}^{{\text{ -λ x}}}}} \right)} \right]_{\text{0}}^{\text{¥}}{\text{ - 2}}\int_{\text{0}}^{\text{¥}} {\left( {{\text{ - }}{{\text{e}}^{{\text{ - λ x}}}}} \right)} \\ & = 0 - 2{\left[ {{\text{0 - }}\frac{{\text{1}}}{{\text{λ }}}} \right]^{{\text{(use partial fraction) }}}} \\ {\text{E}}\left( {{{\text{x}}^{\text{2}}}} \right) &= \frac{{\text{2}}}{{\text{λ}}} \\ \end{aligned} \)

(Use partial fraction again)

Hence the standard deviation can be given as:

\(\begin{aligned}\sigma &= \sqrt {{\rm{E}}\left( {{{\rm{x}}^{\rm{2}}}} \right){\rm{ - (E(X)}}{{\rm{)}}^{\rm{2}}}} \\&= \sqrt {\frac{{\rm{2}}}{{\rm{\lambda }}}{\rm{ - 0}}} {\rm{\sigma }}\\&= \frac{{\sqrt {\rm{2}} }}{{\rm{\lambda }}}\end{aligned}\)

The standard deviation is given to us as\({\rm{40}}{\rm{.9\;km}}\). Hence

\(\begin{aligned}\frac{{\sqrt {\rm{2}} }}{{\rm{\lambda }}} &= 40{\rm{.9\lambda }}\\&= \frac{{\sqrt {\rm{2}} }}{{{\rm{40}}{\rm{.9}}}}{\rm{\lambda }}\\ &= 0 {\rm{.0348}}\end{aligned}\)

04

Calculating the probability

(b)

The probability that the extent of daily sea-ice change is within\({\rm{1}}\)standard deviation of the mean value is given as\({\rm{P(X£ 40}}{\rm{.9)}}\). Hence

\(\begin{aligned}{\text{P(X£40}}\text.9) &= \int_{\text{0}}^{{\text{40}}{\text{.9}}} {\text{f}} {\text{(x) × dx}} \\ \ &= \int_{\text{0}}^{{\text{40}}{\text{.9}}} {\text{0}} {\text{.5 λ× }}{{\text{e}}^{{\text{ - λ x}}}}{\text{ × dx}} \\ &= 0{\text{.5 λ}}\left[ {\frac{{{\text{ - }}{{\text{e}}^{{\text{ - λ x}}}}}}{{\text{ λ}}}} \right]_{\text{0}}^{{\text{40}}{\text{.9}}} \\ &= - 0{\text{.5}}\left[ {{{\text{e}}^{{\text{ - λ (40}}{\text{.9)}}}}{\text{ - 1}}} \right] \\ & = 0{\text{.5}}\left[ {{\text{1 - }}{{\text{e}}^{{\text{ - (0}}{\text{.0348)(40}}{\text{.9)}}}}} \right]{\text{P(X£40}}{\text{.9)}} \\ &= 0{\text{.3784}} \\ \end{aligned} \)

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\({\rm{f(x) = \{ }}\begin{array}{*{20}{c}}{{\rm{.09375(4 - }}{{\rm{x}}^2})}&{{\rm{ - 2}} \le {\rm{x}} \le {\rm{2}}}\\{\rm{0}}&{{\rm{otherwise}}}\end{array}\)

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