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Continuous Random Variables Expected Values and Moments Statistics 110 Summer 2006 Copyright c 2006 by Mark E. Irwin
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Page 1: Continuous Random Variables Expected Values and Momentsmarkirwin.net/stat110/Lecture/Section22.pdf · that we want the standard deviation to scale by a factor of jbj. Since the variance

Continuous Random VariablesExpected Values and Moments

Statistics 110

Summer 2006

Copyright c©2006 by Mark E. Irwin

Page 2: Continuous Random Variables Expected Values and Momentsmarkirwin.net/stat110/Lecture/Section22.pdf · that we want the standard deviation to scale by a factor of jbj. Since the variance

Continuous Random Variables

When defining a distribution for a continuous RV, the PMF approach won’tquite work since summations only work for a finite or a countably infinitenumber of items. Instead they are based on the following

Definition: Let X be a continuous RV. The Probability Density Function(PDF) is a function f(x) on the range of X that satisfies the followingproperties:

0 5 10 15 20

0.00

0.04

0.08

0.12

X

f(x)

• f(x) ≥ 0

• f is piecewise continuous

• ∫∞−∞ f(x)dx = 1

Continuous Random Variables 1

Page 3: Continuous Random Variables Expected Values and Momentsmarkirwin.net/stat110/Lecture/Section22.pdf · that we want the standard deviation to scale by a factor of jbj. Since the variance

For any a < b, the probability that P [a < X < b] is the area under thedensity curve between a and b.

0 5 10 15 20

0.00

0.04

0.08

0.12

X

f(x)

a b

P [a < X < b] =∫ b

a

f(x)dx

Continuous Random Variables 2

Page 4: Continuous Random Variables Expected Values and Momentsmarkirwin.net/stat110/Lecture/Section22.pdf · that we want the standard deviation to scale by a factor of jbj. Since the variance

Note that f(a) is NOT the probability of observing X = a as

P [X = a] =∫ a

a

f(x)dx = 0

Thus the probability that a continuous RV takes on any particular value is0. (While this might seem counterintuitive, things do work properly.) Aconsequence of this is that

P [a < X < b] = P [a ≤ X < b] = P [a < X ≤ b] = P [a ≤ X ≤ b]

for continuous RVs. Note that this won’t hold for discrete RVs.

Continuous Random Variables 3

Page 5: Continuous Random Variables Expected Values and Momentsmarkirwin.net/stat110/Lecture/Section22.pdf · that we want the standard deviation to scale by a factor of jbj. Since the variance

Note that for small δ, if f is continuous at x

P

[x− δ

2≤ X ≤ x +

δ

2

]=

∫ x+δ2

x−δ2

f(u)du ≈ f(x)δ

X

f(x)

x −δ

2x +

δ

2x

So the probability of seeing an outcome in a small interval around x isproportional to f(x). So the PDF is giving information of how likely anobservation at x is.

Continuous Random Variables 4

Page 6: Continuous Random Variables Expected Values and Momentsmarkirwin.net/stat110/Lecture/Section22.pdf · that we want the standard deviation to scale by a factor of jbj. Since the variance

As with the PMF and the CDF for discrete RVs, there is a relationshipbetween the PDF, f(x), and the CDF, F (x), for continuous RVs

F (x) = P [X ≤ x] =∫ x

−∞f(u)du

f(x) = F ′(x)

assuming that f is continuous at x.

Based on this relationship, the probability for any reasonable event describinga RV can determined with the CDF as the probability of any interval satisfies

P [a < X ≤ b] = F (b)− F (a)

Note that this is slightly different than the formula given on page 47. Theabove holds for any RV (discrete, continuous, mixed). The form given onpage 47

P [a ≤ X ≤ b] = F (b)− F (a)only holds for continuous RVs.

Continuous Random Variables 5

Page 7: Continuous Random Variables Expected Values and Momentsmarkirwin.net/stat110/Lecture/Section22.pdf · that we want the standard deviation to scale by a factor of jbj. Since the variance

Example: Uniform RV on [0,1] (Denoted X ∼ U(0, 1))

What most people think of when we say pick a numberbetween 0 and 1. Any real number in the interval ispossible and equally likely, implying that any interval oflength h must have the same probability (which needsto be h). The PDF for X then must be

f(x) =

{1 0 ≤ x ≤ 10 x < 0 or x > 1

−1.0 −0.5 0.0 0.5 1.0 1.5 2.0

0.0

0.4

0.8

PDF of U(0,1)

x

f(x)

Continuous Random Variables 6

Page 8: Continuous Random Variables Expected Values and Momentsmarkirwin.net/stat110/Lecture/Section22.pdf · that we want the standard deviation to scale by a factor of jbj. Since the variance

The CDF for a U(0, 1) is

F (x) =

0 x < 0x 0 ≤ x ≤ 11 x > 1

−1.0 −0.5 0.0 0.5 1.0 1.5 2.0

0.0

0.2

0.4

0.6

0.8

1.0

CDF of U(0,1)

x

F(x

)

Continuous Random Variables 7

Page 9: Continuous Random Variables Expected Values and Momentsmarkirwin.net/stat110/Lecture/Section22.pdf · that we want the standard deviation to scale by a factor of jbj. Since the variance

One way to think of the CDF is that you give a value of the RV and it givesa probability associated with it (i.e. P [X ≤ x]). It can also be useful to gothe other way. Give a probability and figure out which value of the RV isassociated with it.

Lets assume that F is continuous and strictly increasing in some interval I(i.e. F = 0 to the left of I and F = 1 to the right of I) (note I mightbe unbounded). Under these assumptions the inverse function F−1 is welldefined (x = F−1(y) if F (x) = y).

Definition: The pth Quantile of the distribution F is defined to be thevalue xp such that

F (xp) = p or P [X ≤ xp] = p

Under the above assumptions xp = F−1(p).

Continuous Random Variables 8

Page 10: Continuous Random Variables Expected Values and Momentsmarkirwin.net/stat110/Lecture/Section22.pdf · that we want the standard deviation to scale by a factor of jbj. Since the variance

−4 −2 0 2 4

0.0

0.2

0.4

0.6

0.8

1.0

Quantiles

x

F(x

)

xp

p

Special cases of interest of the Median (p = 12) and the lower and upper

Quartiles (p = 14 and = 3

4)

Continuous Random Variables 9

Page 11: Continuous Random Variables Expected Values and Momentsmarkirwin.net/stat110/Lecture/Section22.pdf · that we want the standard deviation to scale by a factor of jbj. Since the variance

Note: Defining quantiles for discrete distributions is a bit tougher since theCDF doesn’t take all values between 0 and 1 (due to the jumps)

−1 0 1 2 3 4

0.0

0.2

0.4

0.6

0.8

1.0

CDF for number of heads in 3 flips

x (number of heads)

P[X

<=

x]

The definition above can be extended to solving the simultaneous equations

P [X ≤ xp] ≥ p and P [X < xp] ≤ p

Continuous Random Variables 10

Page 12: Continuous Random Variables Expected Values and Momentsmarkirwin.net/stat110/Lecture/Section22.pdf · that we want the standard deviation to scale by a factor of jbj. Since the variance

This can be though of as the place where the CDF jumps from below p toabove p

−1 0 1 2 3 4

0.0

0.4

0.8

CDF for number of heads in 3 flips

x (number of heads)

P[X

<=

x]

0.0 0.2 0.4 0.6 0.8 1.0

0.0

1.0

2.0

3.0

Quantile function for number of heads in 3 flips

p

x p

Continuous Random Variables 11

Page 13: Continuous Random Variables Expected Values and Momentsmarkirwin.net/stat110/Lecture/Section22.pdf · that we want the standard deviation to scale by a factor of jbj. Since the variance

Expected Values and Moments

Definition: The Expected Value of a continuous RV X (with PDF f(x))is

E[X] =∫ ∞

−∞xf(x)dx

assuming that∫∞−∞ |x|f(x)dx < ∞.

The expected value of a distribution is often referred to as the mean of thedistribution.

As with the discrete case, the absolute integrability is a technical point,which if ignored, can lead to paradoxes.

For an example of a continuous RV with infinite mean, see the Cauchydistribution (Example G, page 114)

Expected Values and Moments 12

Page 14: Continuous Random Variables Expected Values and Momentsmarkirwin.net/stat110/Lecture/Section22.pdf · that we want the standard deviation to scale by a factor of jbj. Since the variance

As with the discrete case, E[X] can be thought as a measure of center ofthe random variable.

For example, when X ∼ U(0, 1)

E[X] =∫ 1

0

xdx = 0.5

−1.0 −0.5 0.0 0.5 1.0 1.5 2.0

0.0

0.2

0.4

0.6

0.8

1.0

PDF of U(0,1)

x

f(x)

Expected Values and Moments 13

Page 15: Continuous Random Variables Expected Values and Momentsmarkirwin.net/stat110/Lecture/Section22.pdf · that we want the standard deviation to scale by a factor of jbj. Since the variance

Not surprisingly, expectations of functions of continuous RVs satisfy theexpected relationship

E[g(X)] =∫ ∞

−∞g(x)f(x)dx

For example, if X ∼ U(0, 1),

E[X2] =∫ 1

0

x2dx =13

This is often easier than figuring out the PDF of Y = g(X) and applyingthe definition as there is often some work to figure out the PDF of Y .(Which we will do later, it does have its uses)

As with discrete RVs, g(E[X]) 6= E[g(X)] in most cases. However, with alinear transformation Y = a + bX

E[a + bX] = a + bE[X]

Expected Values and Moments 14

Page 16: Continuous Random Variables Expected Values and Momentsmarkirwin.net/stat110/Lecture/Section22.pdf · that we want the standard deviation to scale by a factor of jbj. Since the variance

Spread of a RV

−2 −1 0 1 2

X

P[X

=x]

0.00

0.10

0.20

0.30

−2 −1 0 1 2

X

P[X

=x]

0.00

0.10

0.20

0.30

x -1 0 1

p(x) 13

13

13

x -2 -1 0 1 2

p(x) 19

29

39

29

19

Expected Values and Moments 15

Page 17: Continuous Random Variables Expected Values and Momentsmarkirwin.net/stat110/Lecture/Section22.pdf · that we want the standard deviation to scale by a factor of jbj. Since the variance

−2 −1 0 1 2

0.0

0.1

0.2

0.3

0.4

0.5

x

f(x)

−2 −1 0 1 2

0.0

0.1

0.2

0.3

0.4

0.5

x

f(x)

f(x) =

{0.5 −1 ≤ x ≤ 10 Otherwise

f(x) =

0.5 + x4 −2 ≤ x ≤ 0

0.5− x4 0 ≤ x ≤ 2

0 Otherwise

All these distributions have E[X] = 0 but the right hand side in each casehas a bigger spread. A common measure of spread is the Standard Deviation

Expected Values and Moments 16

Page 18: Continuous Random Variables Expected Values and Momentsmarkirwin.net/stat110/Lecture/Section22.pdf · that we want the standard deviation to scale by a factor of jbj. Since the variance

Definition: Let µ = E[X], then the Variance of the random variable X is

Var(X) = E[(X − µ)2]

provided the expectation exists.

The Standard Deviation of X is

SD(X) =√

Var(X)

For a discrete RV,Var(X) =

i

(xi − µ)2p(xi)

For a continuous RV

Var(X) =∫ ∞

−∞(x− µ)2f(x)dx

Expected Values and Moments 17

Page 19: Continuous Random Variables Expected Values and Momentsmarkirwin.net/stat110/Lecture/Section22.pdf · that we want the standard deviation to scale by a factor of jbj. Since the variance

The variance measures the expected squared difference of an observationfrom the mean. While the interpretation of the standard deviation isn’tquite easy, it can be thought of a measure of the typical spread of a RV.

It can be shown that, assuming that the variance exists,

Var(X) = E[X2]− (E[X])2

This form is often useful for calculation purposes.

Notation: The variance is often denoted by σ2 and the standard deviationby σ.

Expected Values and Moments 18

Page 20: Continuous Random Variables Expected Values and Momentsmarkirwin.net/stat110/Lecture/Section22.pdf · that we want the standard deviation to scale by a factor of jbj. Since the variance

For the examples

−2 −1 0 1 2

X

P[X

=x]

0.00

0.10

0.20

0.30

x −1 0 1

p(x) 13

13

13

Var(X) = (−1− 0)213

+ (0− 0)213

+ (1− 0)213

=23

SD(X) =

√23

= 0.8165

Expected Values and Moments 19

Page 21: Continuous Random Variables Expected Values and Momentsmarkirwin.net/stat110/Lecture/Section22.pdf · that we want the standard deviation to scale by a factor of jbj. Since the variance

−2 −1 0 1 2

X

P[X

=x]

0.00

0.10

0.20

0.30 x −2 −1 0 1 2

p(x) 19

29

39

29

19

Var(X) = (−2− 0)219

+ (−1− 0)229

+ (0− 0)239

+ (1− 0)229

+ (2− 0)219

=109

SD(X) =

√109

= 1.0541

Expected Values and Moments 20

Page 22: Continuous Random Variables Expected Values and Momentsmarkirwin.net/stat110/Lecture/Section22.pdf · that we want the standard deviation to scale by a factor of jbj. Since the variance

−2 −1 0 1 2

0.0

0.1

0.2

0.3

0.4

0.5

x

f(x)

f(x) =

{0.5 −1 ≤ x ≤ 10 Otherwise

Var(X) =∫ 1

−1

(x− 0)212dx =

13

SD(X) =

√13

= 0.5774

Expected Values and Moments 21

Page 23: Continuous Random Variables Expected Values and Momentsmarkirwin.net/stat110/Lecture/Section22.pdf · that we want the standard deviation to scale by a factor of jbj. Since the variance

−2 −1 0 1 2

0.0

0.1

0.2

0.3

0.4

0.5

x

f(x)

f(x) =

0.5 + x4 −2 ≤ x ≤ 0

0.5− x4 0 ≤ x ≤ 2

0 Otherwise

Var(X) = 2∫ 2

0

(x− 0)2(0.5− x

4)dx =

43

SD(X) =

√43

= 1.1547

Expected Values and Moments 22

Page 24: Continuous Random Variables Expected Values and Momentsmarkirwin.net/stat110/Lecture/Section22.pdf · that we want the standard deviation to scale by a factor of jbj. Since the variance

What is the effect of a linear transformation (Y = a + bX) on the varianceand standard deviation?

Var(a + bX) = b2Var(X) SD(a + bX) = |b|SD(X)

These two results are to be expected. For example, if two possible X valuesdiffer by d = |x1−x2|, the corresponding Y values differ by |b|d, suggestingthat we want the standard deviation to scale by a factor of |b|. Since thevariance measures squared spread, it needs to scale by a factor of b2.

The factor a not having an effect also makes sense. Adding a to a randomvariable shifts the location of its distribution, but doesn’t changes thedistance between corresponding pairs of points.

Expected Values and Moments 23


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