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CHAPTER V
FINITE DIFFERENCES. CENTRAL DIFFERENCES
+x(x2—1)(x2—4) A' f (— 2) + A' f ( 3)
5!    2
    
+x2(x2—1)(x2—4)A6f(—3)+         (1). 61

30    FINITE DIFFERENCES BESSEL'S :
.f(x)=f(0)2f (1)+(x--1)f(0)

+x(x-1) Alf(-1)+o2f(o)+(x- )x(x—1)o3f(—1)
2!    2    3!
+(x+1)x(x—1)(x—2) 0*f(—1)+ f(—2)
4!    2
(x—+)(x+1)x(x—1)(x—2)0, f(—2) +(x
5!
+(x+2)(x+1)x(x—1)(x—2)(x—3) Oef(—2)+Aef(—3)+...
6!    2
    (2).
GAUSS':
f(x)=f(0)+xAf(o)+(2-1)02 f(-1)+(x+13,(x-1)
+(c+l)x(x—1)(x— 2)A*f(—2) 4!
+(x+2)(x+l)x(x—1)(x—2) p5f(—2)+    (3).
5!
EVERETT'S :
(x2 , 1)o2f(0)+x(x9 - 5!(x2 -4)(-1)
+x(x2—1)(x2—4)(x2—9)0"f(—2)+... 7'
+yf(6)+y3!    1)A2f(-1)+y(y2—1)I(y9—4)p*f(-2)
+y(y2—1)(y2—4)(y2—9)psf(—3) +     (4)
71 [where y = 1—4

4. These formulas can be obtained in various ways from the ordinary formulas of advancing differences. Once, however, the scheme of differences entering into a formula is settled, the cocan readily be calculated by the method of Separation of Symbols. An example may be given of the demonstration of Gauss' formula by this method.

CENTRAL DIFFERENCES    31
Example 1.
To express f (x) in terms off (0), A f (0), 6,2 f (- 1), 03f (- 1), ....
Let    .f (x) = Ao.f (0)+A1Af (0) + A2Af(-1)+.... Then, since
Of (-1)=1+
A
'f(0); A3.f(-1)=1+3of(0); etc.,
(1+A)x=Ao+A1A+A21+20+A31+3L+...
A2r-1    Qtr
+A2M—1(1+0)r—'+A2'(1+0)'+.... Multiplying up by (1 + A)r-1, and equating coefficients of A2''-1,
A    (r+x-1)(r+x-2)...(x-r+1)
2r-1=    (2r-1)!
And, multiplying up by (1 + A)r, and equating coefficients of A2r, (r+x)(r+x-1)... (x-r+l)
Asr-1 + 112r =    2r!
Hence, by subtraction,
A2r-(r+x-1)(r+x-2)...(x-r) 2r!
Therefore f (x) = f (0) + xA f (0)
+x(xy_I 1) 02f(- 1)+(x+l)a (x-1)A3.f(-l)+....
The other formulas should be proved, in a similar way, as exercises by the student*.
5. The formulas of central differences, although in a different form, are intimately associated with those of advancing differences. For example, if an interpolated value is calculated by using the first three terms of Stirling's formula, it is obvious that the values
* See J.I. A. Vol. 50, pp. 28-33.

32    FINITE DIFFERENCES
of f(— 1), f (0) and f (l) are brought into the calculation. It is easy to show that the result is identical with that obtained by using the first three terms of the advancing difference formula starting with the term f(— 1).
It may be observed that the first two terms of Stirling's formula also involve three values of the function; the third term merely introduces the correction necessary to make the formula true to the order of differences (i.e. the second) implied by the use of three terms of the series. Thus, as the (2r)th and the (2r + 1)th terms of Stirling's formula both involve the use of (2r + 1) values of the function, there is ordinarily little advantage in using the extra (2r + 1)th term in any calculation.
Similarly in Bessel
's formula no material increase in precision is gained by using 2r terms rather than 2r — 1 terms.
Gauss' and Everett's formulas are each true to the order of differences involved and for general use they would appear to be the best of those propounded.

CENTRAL DIFFERENCES    33
years, and we will take 5 years as the unit. Thus we get the following scheme :
No. of
years
x f f.))
Q
e2 Q3  
A5
0
-3 1.
27628
'07633 •02110 •00580 '00165
5
-2 1.27628
•35261
•09743 '02690 '00745 '00206
10
-1 1.62889
•45004
'12433 •03435 •00951  
15
0 2.07893
'57437
•15868 •04386    
20
1 2.65330
.73305
•20254      
25
2
:3:38635
•93559        
30
3 4.32194          

As the unit of time is 5 years, the required value is repreby f (•4).
Central Differences. We will use Gauss' formula, i.e.
f (x) = f (0) + xhf (0)
+x(x—1)(—1)+(x+1)x(x—1)as)(—1)+.... 21    3!

The successive terms, with the corresponding values of f (•4), are
f (0) =    2.07893, 1st approx. = 2.07893
•4f(0) =    •22975, 2nd    „    =
2.30868
•4x—.6A2 f(—1)= — •01492,3rd    =
2.29376
1.4 x •4 x — •6 03    1    00192, 4th 2.29184
6    f(    )    =
1 4 x 4 x — 6 x _ 1 6    4 f (    2 ) ,    •00017 5th    =
2.29201
24    '
 
2.4x1.4x•4x— 6x—1.6A5 f(—2)=    •00002, 6th    =
2.29203
120  

It is clear that no further terms would affect the calculated value. The true value is 2.29202.
H. T. B. I.    3

34    FINITE DIFFERENCES
Advancing Differences.


1st approximation    f(0)    = 2.07893,


2nd approximation    f (0) +    f (0)    = 2.30868,
3rd approximation
    f(—1)+1'4Of(—1)+142      4O'f(—1) =2.29376,
4th approximation
f(—1)+1.46,f(—1)+142 4O2f(—1)
+ 1.4 x•4x—•6 As 6      O f(—1)=229184,
5th approximation
    f(—2)+ 2.4A.f(—2)+242    14f(—2)
2.4xP4x•4 3
+—    f(—2)


2.4x1.4x•4x—•6 +    24    &f(_ 2) = 2 .29200,
6th approximation
6
(5th approximation) +24 x 14 x 4 x    x -16 120    A°f (—2)=2.29202.
It will be observed that in proceeding to the 3rd and 5th approximations using advancing differences every term in the formula has to be recalculated, whereas, in the application of the central difference formula, terms already calculated hold good whatever be the degree of approximation.
It should be noted, however, that both formulas give mathethe same results, the difference of a unit in the final figure being due to the use of only five places of decimals throughout.
8. As regards other practical points, it may be observed that the numerical coefficients in the central difference formulas are smaller than those in the advancing difference formulas (see Example 2).
Other advantages arise in special cases. Thus Bessel's formula

CENTRAL DIFFERENCES    35
can conveniently be applied for the bisection of an interval, since the alternate terms vanish, giving
f(I)=f(0)+f(1)02f(—1)+6.2f(0)
2    8    2
+ 3 A4f(-2)+04.f(—1)+... (5). 128    2
Everett's formula gives the same value.
3—2

36    FINITE DIFFERENCES
The coefficients of the several terms in Everett's formula are
•2
- •032
•006336
.4
- •056
010752
•6
- •064
011648
.8
- •048
•008064

The work may be arranged in tabular form:
r _-_.          
    $
2    2
Sum of first
Sum of Inter
x
a f (1)
_
x (x    1)
D2 f (0)
_    _
x (x    1) (x    4)
~4f (-1)
three terms
second P
p
result
    31 5!      
       
(2) + (3) + (4)
tethree
rms
(5) + (6)
(1)
(2) (3)
(4)
(5) (6) (7)
•2
200.2 -    2.6 0.0 197.6    
•4
400.4 - 4.7 0.1 395.8    
•6
600.6 - 5.4 0.1 595.3    
•8
800.8 - 4.0 0.0 796.8    
•2
244.8 - 4.0 0.2 241.0 796.8 1037.8
•4
489.6 -    7.0 0.4 483.0 595.3 1078.3
•6
7344
- 8.0 0.4
726-8
395.8 1122.6
•8
979.2 - 6.0 0.3 973.5 197.6 1171.1
•2
314.4 - 6.5 0.2
3081
973.5 1281.6
•4
628.8 -11.4 0.3 617.7 726.8 1344.5
•6
943.2 -13.0 0.3 930.5 483.0
1.413.5
•8
1257.6 - 9.7 0.2 1248.1 241-0 1489.1

Columns (2), (3) and (4), which represent the first three terms of the formula, are obtained by ordinary multiplication. Column (5) gives the sum of these terms. From what has been said above, it is clear that column (6), which represents the second set of three terms of the formula to fourth central differences, is obtained by writing down, in reverse order, the values of column (5) applicable to the previous group of terms. The addition of columns (5) and (6) then gives the desired result.
The given values of f (x) have been taken from the tabulated values of the probability of dying in a given year of age according to the HM mortality table, multiplied by 105.
The tabular values for the interpolated terms are 1038, 1081, 1122, 1172, 1281, 1345, 1415, 1490. The small differences between these values and the interpolated values are due to the fact that the HM table was constructed by means of a mathematical formula which is only approximately represented by Everett's formula.

CENTRAL DIFFERENCES    37
38    FINITE DIFFERENCES

Example 4. See Example 2. Seven terms are given, the formula will therefore be
    f(•4)     = ,f(—3) _ f(—2)    f(—1)
•4(•16—1)(•16—4)(•16—9) 720 x 3.4 120 x 2.4+48 x 1.4
f    (o) +f(1)    f(2)    f(3)
36x•448x—•6 120x—1.6+720x— 2.6'
or f (•4) = — •0046592 f (— 3) + .0396032 f (— 2) — •169728,f (— 1)
+ 792064, f (0) + •396032 f (1) — •0594048 f (2) + .0060928f(3)
=
+ •05055
— •00466
  1.64665
•27647
  1.05079
•20117
 
•02633
 
  + 2.77432
— •48230
=
2.29202 as before.

Note, as a check, that the algebraic sum of the coefficients of the terms on the right-hand side of the above equation is unity.
13. For the sake of completeness it is necessary to refer to a system of notation in connection with central differences which was introduced by W. S. B. Woolhouse and is still in use to some extent. This system of notation is compared with that used in the previous chapters in the following scheme :
Ordinary Notation Woolhouse's Notation
f(—2)     f(—2)      
(—2)
      a_2    
f(—1)0 ~2.f(—2)   .f(—1)   b_1  
(—1)
  Daf(—2)   a_1   c_i
f(0) A2f (—1)
&f(—2)
f(0) (ao) bo (co)    do
Of (0)   oaf(—1)   al   c1
f(1) ,,2f(0)   f(1)   bl  
Af(1)            
f (2)     f (2)      

where A f (— 2), 62 f (— 2), etc. are denoted by a_2, b_„ etc. and ao = i (a—i + a+1), co = 2 (c_1 + c+1).
Under this notation Stirling's formula to fourth differences is x2    x (x2 1)    x2 (x2 1)
f(x)=f(o)+xao+bo+    ,, --co+    4,    do
=f(0)+(ao—3°,)x+(2i—:i)x'+°ixs+fix' ...(11).

CENTRAL DIFFERENCES    39
Similarly Gauss' formula can be written
    
x(x—1)    (x+1)x(x—1)
f (x) = f (0) + xa, +    2!      bo '    3!
    ci
+(x+1)x(x-1)(x-2)d    (12).
4,1

14. Another system of notation, which is extensively used, is that due to W. F. Sheppard. Two operators 8 and /h are used, such that
    
8f(I) =f(0) —.f (— 1),    µ.f (1) = [.f (0) +f(1)],
sf(2)=.f(1)—f(o),    wsf(0)=[sf(I)+sf(—i)7,
etc.    etc.
This notation, although somewhat complicated, gives the usual central difference formulas in very convenient forms.