Skip to main content

Quadratic and Cubic Methods

An approach for finding the minimum of [Graphics:Images/QuadraticSearchMod_gr_1.gif] in a given interval is to evaluate the function many times and search for a local minimum. To reduce the number of function evaluations it is important to have a good strategy for determining where [Graphics:Images/QuadraticSearchMod_gr_2.gif] is to be evaluated. Two efficient bracketing methods are the golden ratio and Fibonacci searches. To use either bracketing method for finding the minimum of [Graphics:Images/QuadraticSearchMod_gr_3.gif], a special condition must be met to ensure that there is a proper minimum in the given interval.

The function [Graphics:Images/QuadraticSearchMod_gr_4.gif] is unimodal on [Graphics:Images/QuadraticSearchMod_gr_5.gif], if there exists a unique number [Graphics:Images/QuadraticSearchMod_gr_6.gif] such that

[Graphics:Images/QuadraticSearchMod_gr_7.gif] is decreasing on [Graphics:Images/QuadraticSearchMod_gr_8.gif],
and
[Graphics:Images/QuadraticSearchMod_gr_9.gif] is increasing on [Graphics:Images/QuadraticSearchMod_gr_10.gif].

Minimization Using Derivatives

Suppose that
[Graphics:Images/QuadraticSearchMod_gr_11.gif] is unimodal over [Graphics:Images/QuadraticSearchMod_gr_12.gif] and has a unique minimum at [Graphics:Images/QuadraticSearchMod_gr_13.gif]. Also, assume that [Graphics:Images/QuadraticSearchMod_gr_14.gif] is defined at all points in [Graphics:Images/QuadraticSearchMod_gr_15.gif]. Let the starting value [Graphics:Images/QuadraticSearchMod_gr_16.gif] lie in [Graphics:Images/QuadraticSearchMod_gr_17.gif]. If [Graphics:Images/QuadraticSearchMod_gr_18.gif] , then the minimum point p lies to the right of [Graphics:Images/QuadraticSearchMod_gr_19.gif]. If [Graphics:Images/QuadraticSearchMod_gr_20.gif] , then the minimum point p lies to the left of [Graphics:Images/QuadraticSearchMod_gr_21.gif].


Our first task is to obtain three test values,

(1)
[Graphics:Images/QuadraticSearchMod_gr_22.gif],
so that
(2)
[Graphics:Images/QuadraticSearchMod_gr_23.gif].

Suppose that [Graphics:Images/QuadraticSearchMod_gr_24.gif]; then [Graphics:Images/QuadraticSearchMod_gr_25.gif] and the step size h should be chosen positive. It is an easy task to find a value of h so that the three points in (1) satisfy (2). Start with [Graphics:Images/QuadraticSearchMod_gr_26.gif] in formula (1) (provided that [Graphics:Images/QuadraticSearchMod_gr_27.gif]); if not, take [Graphics:Images/QuadraticSearchMod_gr_28.gif], and so on.

Case (i) If (2) is satisfied we are done.

Case (ii) If [Graphics:Images/QuadraticSearchMod_gr_29.gif], then [Graphics:Images/QuadraticSearchMod_gr_30.gif].
We need to check points that lie farther to the right. Double the step size and repeat the process.

Case (iii) If [Graphics:Images/QuadraticSearchMod_gr_31.gif], we have jumped over p and h is too large.
We need to check values closer to
[Graphics:Images/QuadraticSearchMod_gr_32.gif]. Reduce the step size by a factor of [Graphics:Images/QuadraticSearchMod_gr_33.gif] and repeat the process.

When
[Graphics:Images/QuadraticSearchMod_gr_34.gif], the step size h should be chosen negative and then cases similar to (i), (ii), and (iii) can be used.

Quadratic Approximation to Find p

Finally, we have three points (1) that satisfy (2). We will use quadratic interpolation to find
[Graphics:Images/QuadraticSearchMod_gr_35.gif], which is an approximation to p. The Lagrange polynomial based on the nodes in (1) is

(3)[Graphics:Images/QuadraticSearchMod_gr_36.gif],


where [Graphics:Images/QuadraticSearchMod_gr_37.gif].

The derivative of [Graphics:Images/QuadraticSearchMod_gr_38.gif] is

(4)
[Graphics:Images/QuadraticSearchMod_gr_39.gif].

Solving [Graphics:Images/QuadraticSearchMod_gr_40.gif] in the form [Graphics:Images/QuadraticSearchMod_gr_41.gif] yields

(5)[Graphics:Images/QuadraticSearchMod_gr_42.gif].


Multiply each term in (5) by [Graphics:Images/QuadraticSearchMod_gr_43.gif] and collect terms involving [Graphics:Images/QuadraticSearchMod_gr_44.gif]:

[Graphics:Images/QuadraticSearchMod_gr_45.gif]

[Graphics:Images/QuadraticSearchMod_gr_46.gif]

[Graphics:Images/QuadraticSearchMod_gr_47.gif]

[Graphics:Images/QuadraticSearchMod_gr_48.gif]

This last quantity is easily solved for [Graphics:Images/QuadraticSearchMod_gr_49.gif]:

[Graphics:Images/QuadraticSearchMod_gr_50.gif].

The value [Graphics:Images/QuadraticSearchMod_gr_51.gif] is a better approximation to p than [Graphics:Images/QuadraticSearchMod_gr_52.gif]. Hence we can replace [Graphics:Images/QuadraticSearchMod_gr_53.gif] with [Graphics:Images/QuadraticSearchMod_gr_54.gif] and repeat the two processes outlined above to determine a new h and a new [Graphics:Images/QuadraticSearchMod_gr_55.gif]. Continue the iteration until the desired accuracy is achieved. In this algorithm the derivative of the objective function [Graphics:Images/QuadraticSearchMod_gr_56.gif] was used implicitly in (4) to locate the minimum of the interpolatory quadratic. The reader should note that the subroutine makes no explicit use of the derivative.

Cubic Approximation to Find p

We now consider an approach that utilizes functional evaluations of both [Graphics:Images/QuadraticSearchMod_gr_57.gif] and [Graphics:Images/QuadraticSearchMod_gr_58.gif]. An alternative approach that uses both functional and derivative evaluations explicitly is to find the minimum of a third-degree polynomial that interpolates the objective function [Graphics:Images/QuadraticSearchMod_gr_59.gif] at two points. Assume that [Graphics:Images/QuadraticSearchMod_gr_60.gif] is unimodal and differentiable on [Graphics:Images/QuadraticSearchMod_gr_61.gif], and has a unique minimum at [Graphics:Images/QuadraticSearchMod_gr_62.gif]. Let [Graphics:Images/QuadraticSearchMod_gr_63.gif]. Any good step size h can be used to start the iteration. The Mean Value Theorem could be used to obtain [Graphics:Images/QuadraticSearchMod_gr_64.gif] and if [Graphics:Images/QuadraticSearchMod_gr_65.gif] was just to the right of the minimum, then the slope [Graphics:Images/QuadraticSearchMod_gr_66.gif] might be twice [Graphics:Images/QuadraticSearchMod_gr_67.gif] which would mean that [Graphics:Images/QuadraticSearchMod_gr_68.gif] we do not know how much further to the right [Graphics:Images/QuadraticSearchMod_gr_69.gif] lies, so we can imagine that [Graphics:Images/QuadraticSearchMod_gr_70.gif] is close to [Graphics:Images/QuadraticSearchMod_gr_71.gif] and estimate h with the formula:

[Graphics:Images/QuadraticSearchMod_gr_72.gif].

Thus [Graphics:Images/QuadraticSearchMod_gr_73.gif]. The cubic approximating polynomial [Graphics:Images/QuadraticSearchMod_gr_74.gif] is expanded in a Taylor series about [Graphics:Images/QuadraticSearchMod_gr_75.gif] (which is the abscissa of the minimum). At the minimum we have [Graphics:Images/QuadraticSearchMod_gr_76.gif], and we write [Graphics:Images/QuadraticSearchMod_gr_77.gif] in the form:

(6)
[Graphics:Images/QuadraticSearchMod_gr_78.gif],
and
(7)[Graphics:Images/QuadraticSearchMod_gr_79.gif].

The introduction of [Graphics:Images/QuadraticSearchMod_gr_80.gif] in the denominators of (6) and (7) will make further calculations less tiresome. It is required that [Graphics:Images/QuadraticSearchMod_gr_81.gif], [Graphics:Images/QuadraticSearchMod_gr_82.gif], [Graphics:Images/QuadraticSearchMod_gr_83.gif], and [Graphics:Images/QuadraticSearchMod_gr_84.gif]. To find [Graphics:Images/QuadraticSearchMod_gr_85.gif] we define:

(8)
[Graphics:Images/QuadraticSearchMod_gr_86.gif],

and we must go through several intermediate calculations before we end up with [Graphics:Images/QuadraticSearchMod_gr_87.gif].

Use use (6) to obtain

[Graphics:Images/QuadraticSearchMod_gr_88.gif]

Then use (8) to get

[Graphics:Images/QuadraticSearchMod_gr_89.gif]

Then substitute [Graphics:Images/QuadraticSearchMod_gr_90.gif] and we have

(9)
[Graphics:Images/QuadraticSearchMod_gr_91.gif]

Use use (7) to obtain

[Graphics:Images/QuadraticSearchMod_gr_92.gif]

[Graphics:Images/QuadraticSearchMod_gr_93.gif]

Then use (8) to get

[Graphics:Images/QuadraticSearchMod_gr_94.gif]

Then substitute [Graphics:Images/QuadraticSearchMod_gr_95.gif] and we have

(10) [Graphics:Images/QuadraticSearchMod_gr_96.gif]

Finally, use (7) and write

[Graphics:Images/QuadraticSearchMod_gr_97.gif]

Then use (8) to get

(11) [Graphics:Images/QuadraticSearchMod_gr_98.gif]

Now we will use the three nonlinear equations (9), 10), (11) listed below in (12). The order of determining the variables will be [Graphics:Images/QuadraticSearchMod_gr_99.gif] (the variable [Graphics:Images/QuadraticSearchMod_gr_100.gif] will be eliminated).

[Graphics:Images/QuadraticSearchMod_gr_101.gif]
(12) [Graphics:Images/QuadraticSearchMod_gr_102.gif]
[Graphics:Images/QuadraticSearchMod_gr_103.gif]

First, we will find [Graphics:Images/QuadraticSearchMod_gr_104.gif] which is accomplished by combining the equation in (12) as follows:

[Graphics:Images/QuadraticSearchMod_gr_105.gif]

Straightforward simplification yields [Graphics:Images/QuadraticSearchMod_gr_106.gif], therefore [Graphics:Images/QuadraticSearchMod_gr_107.gif] is given by

(13) [Graphics:Images/QuadraticSearchMod_gr_108.gif].

Second, we will eliminate [Graphics:Images/QuadraticSearchMod_gr_109.gif] by combining the equation in (12) as follows, multiply the first equation by [Graphics:Images/QuadraticSearchMod_gr_110.gif] and add it to the third equation

[Graphics:Images/QuadraticSearchMod_gr_111.gif]
[Graphics:Images/QuadraticSearchMod_gr_112.gif]

[Graphics:Images/QuadraticSearchMod_gr_113.gif]

which can be rearranged in the form

[Graphics:Images/QuadraticSearchMod_gr_114.gif]

Now the quadratic equation can be used to solve for [Graphics:Images/QuadraticSearchMod_gr_115.gif]

[Graphics:Images/QuadraticSearchMod_gr_116.gif]

It will take a bit of effort to simplify this equation into its computationally preferred form.

[Graphics:Images/QuadraticSearchMod_gr_117.gif]

[Graphics:Images/QuadraticSearchMod_gr_118.gif]

[Graphics:Images/QuadraticSearchMod_gr_119.gif]
Hence,

(14) [Graphics:Images/QuadraticSearchMod_gr_120.gif]

Therefore, the value of [Graphics:Images/QuadraticSearchMod_gr_121.gif] is found by substituting the calculated value of [Graphics:Images/QuadraticSearchMod_gr_122.gif] in (14) into the formula [Graphics:Images/QuadraticSearchMod_gr_123.gif]. To continue the iteration process, let [Graphics:Images/QuadraticSearchMod_gr_124.gif] and replace [Graphics:Images/QuadraticSearchMod_gr_125.gif] and [Graphics:Images/QuadraticSearchMod_gr_126.gif] with [Graphics:Images/QuadraticSearchMod_gr_127.gif] and [Graphics:Images/QuadraticSearchMod_gr_128.gif], respectively, in formulas (12), (13), and (14). The algorithm outlined above is not a bracketing method. Thus determining stopping criteria becomes more problematic. One technique would be to require that [Graphics:Images/QuadraticSearchMod_gr_129.gif], since [Graphics:Images/QuadraticSearchMod_gr_130.gif].

Comments

Popular Posts

Runge-Kutta-Fehlberg Method

One way to guarantee accuracy in the solution of an I.V.P. is to solve the problem twice using step sizes h and and compare answers at the mesh points corresponding to the larger step size. But this requires a significant amount of computation for the smaller step size and must be repeated if it is determined that the agreement is not good enough. The Runge-Kutta-Fehlberg method (denoted RKF45) is one way to try to resolve this problem. It has a procedure to determine if the proper step size h is being used. At each step, two different approximations for the solution are made and compared. If the two answers are in close agreement, the approximation is accepted. If the two answers do not agree to a specified accuracy, the step size is reduced. If the answers agree to more significant digits than required, the step size is increased. Each Runge-Kutta-Fehlberg step requires the use of the following six values: Then an approximation to the solution of the I.V.P.

Van Der Pol System

The van der Pol equation is an ordinary differential equation that can be derived from the Rayleigh differential equation by differentiating and setting . It is an equation describing self-sustaining oscillations in which energy is fed into small oscillations and removed from large oscillations. This equation arises in the study of circuits containing vacuum tubes and is given by If , the equation reduces to the equation of simple harmonic motion The van der Pol equation is , where is a constant. When the equation reduces to , and has the familiar solution . Usually the term in equation (1) should be regarded as friction or resistance, and this is the case when the coefficient is positive. However, if the coefficient is negative then we have the case of "negative resistance." In the age of "vacuum tube" radios, the " tetrode vacuum tube " (cathode, grid, plate), was used for a power amplifie

Powell's Method

The essence of Powell's method is to add two steps to the process described in the preceding paragraph. The vector represents, in some sense, the average direction moved over the n intermediate steps in an iteration. Thus the point is determined to be the point at which the minimum of the function f occurs along the vector . As before, f is a function of one variable along this vector and the minimization could be accomplished with an application of the golden ratio or Fibonacci searches. Finally, since the vector was such a good direction, it replaces one of the direction vectors for the next iteration. The iteration is then repeated using the new set of direction vectors to generate a sequence of points . In one step of the iteration instead of a zig-zag path the iteration follows a "dog-leg" path. The process is outlined below. Let be an initial guess at the location of the minimum of the function . Let for be the

Fibonacci Method

An approach for finding the minimum of in a given interval is to evaluate the function many times and search for a local minimum. To reduce the number of function evaluations it is important to have a good strategy for determining where is to be evaluated. Two efficient bracketing methods are the golden ratio and Fibonacci searches. To use either bracketing method for finding the minimum of , a special condition must be met to ensure that there is a proper minimum in the given interval. The function is unimodal on , if there exists a unique number such that is decreasing on , and is increasing on . In the golden ratio search two function evaluations are made at the first iteration and then only one function evaluation is made for each subsequent iteration. The value of remains constant on each subinterval and the search is terminated at the subinterval, provided that or where are the predefined tolerances. The Fibo