Powharmonic series: Difference between revisions

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{{powharmonic series|12|expo=0.69314718056}}
{{powharmonic series|12|expo=0.69314718056}}


The harmonic series is technically a powharmonic series: the 1-powharmonic series. <span><math>p</math><span> closer to 1 give powharmonic series closer to the harmonic series, in case a series is desired which is close enough to the harmonic series to evoke it but has some finely alternately tuned characteristics.
The harmonic series is technically a powharmonic series, but it is the trivial case, with the exponent equal to 1. <span><math>p</math><span> closer to 1 give series closer to the harmonic series, in case a series is desired which is close enough to the harmonic series to evoke it but has some finely alternately tuned characteristics.


Multiplying the exponent of a powharmonic series by some constant c is equivalent to multiplying each of its pitches' cents by that constant c. For example, the 1.5-powharmonic series would be like stretching each octave of the harmonic series from 1200¢ to 1800¢. If you were to instead manipulate a harmonic series by adding or subtracting frequency, rather than exponentiating it, you instead get an [[AFS|AFS (arithmetic frequency sequence)]].
Multiplying the exponent of a powharmonic series by some constant c is equivalent to multiplying each of its pitches' cents by that constant c. For example, the 1.5-powharmonic series would be like stretching each octave of the harmonic series from 1200¢ to 1800¢. If you were to instead manipulate a harmonic series by adding or subtracting frequency, rather than exponentiating it, you instead get an [[AFS|AFS (arithmetic frequency sequence)]].
Line 17: Line 17:
Using a negative power for the exponent gives a similar, but inverted effect. <span><math>f(n) = n^{-1}</math></span> is simply the subharmonic series. Other negative powers give you the subharmonic equivalent of their (super) powharmonic counterpart. You could call these subpowharmonic series.
Using a negative power for the exponent gives a similar, but inverted effect. <span><math>f(n) = n^{-1}</math></span> is simply the subharmonic series. Other negative powers give you the subharmonic equivalent of their (super) powharmonic counterpart. You could call these subpowharmonic series.


== log-base-b-of-a-powharmonic series ==
== log-base-b-of-a-Powharmonic series ==
[[File:Log-base-3-of-2-powharmonic series.png|thumb|
[[File:Log-base-3-of-2-powharmonic series.png|thumb|
log-base-3-of-2-powharmonic series
log-base-3-of-2-powharmonic series
Line 23: Line 23:


=== Description ===
=== Description ===
When we choose a <span><math>p</math></span> of the form <span><math>\log_{b}a</math></span>, the resulting scale will include every integer power of <span><math>a</math></span>, and the count of steps between each power of <span><math>a</math></span> will increase by a factor of <span><math>b</math></span>.
When we choose a <span><math>p</math></span> of the form <span><math>\log_{b}a</math></span>, the resulting scale will include every integer power of <span><math>a</math></span>, and the count of steps between each power of <span><math>a</math></span> will increase by a factor of <span><math>b</math></span>.


Line 29: Line 28:


=== Pitches per period ===
=== Pitches per period ===
 
For example, the log-base-3-of-2-powharmonic series, where <span><math>p = log_{3}2</math></span>, will&mdash;like the harmonic series and by virtue of being "of 2"&mdash;include every octave (multiple of 2) of the fundamental. However, instead of the counts of pitches per octave increasing by a factor of 2:
For example, the log-base-3-of-2-powharmonic series, where <span><math>p = log_{3}2</math></span>, will — like the harmonic series — and by virtue of being "of 2" — include every octave (multiple of 2) of the fundamental. However, instead of the counts of pitches per octave increasing by a factor of 2:


<math>2, 4, 8, 16…
<math>2, 4, 8, 16…
</math>
</math>


they’ll — by virtue of being "base-3" — increase by a factor of 3:
they will&mdash;by virtue of being "base-3"&mdash;increase by a factor of 3:


<math>2, 6, 18, 54…
<math>2, 6, 18, 54…
Line 41: Line 39:


=== Equality explanation ===
=== Equality explanation ===
An equality involving exponents and logarithms helps us understand why:
An equality involving exponents and logarithms helps us understand why:


Line 56: Line 53:


=== Initial count ===
=== Initial count ===
The first period of the series, determined by <span><math>a</math></span>, will contain <span><math>b - 1</math></span> pitches. For example, the log-base-4-of-5-powharmonic series' first 5/1 interval will contain <span><math>4 - 1 = 3</math></span> pitches.
The first period of the series, determined by <span><math>a</math></span>, will contain <span><math>b - 1</math></span> pitches. For example, the log-base-4-of-5-powharmonic series' first 5/1 interval will contain <span><math>4 - 1 = 3</math></span> pitches.


=== Equivalences ===
=== Equivalences ==
 
The harmonic series features counts of pitches of increasing powers of 2 in each next octave, but it also contains counts of pitches of increasing powers of 3 in each next tritave, and counts of pitches in increasing powers of 5 in each next 5/1 interval, and so forth. This is because the harmonic series is equivalent to the log-base-2-of-2-powharmonic series, the log-base-3-of-3-powharmonic series, the log-base-5-of-5-powharmonic series, and so forth (the log-base-b-of-b-powharmonic series). This because any <span><math>\log_{b}b = 1</math></span>.
The harmonic series features counts of pitches of increasing powers of 2 in each next octave, but it also contains counts of pitches of increasing powers of 3 in each next tritave, and counts of pitches in increasing powers of 5 in each next 5/1 interval, and so forth. This is because the harmonic series is equivalent to the log-base-2-of-2-powharmonic series, the log-base-3-of-3-powharmonic series, the log-base-5-of-5-powharmonic series, and so forth (the log-base-b-of-b-powharmonic series). This because any <span><math>\log_{b}b = 1</math></span>.


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[[File:Powharmonic space.png|378x378px]]
[[File:Powharmonic space.png|378x378px]]


== a-edharmonic series ==
== ''a''-Edharmonic series ==
 
=== Prerequisite: ln-of-a-powharmonic series ===
=== Prerequisite: ln-of-a-powharmonic series ===
[[File:Ln-of-2-powharmonic series.png|thumb|
[[File:Ln-of-2-powharmonic series.png|thumb|
ln-of-2-powharmonic series
ln-of-2-powharmonic series
Line 84: Line 77:


=== Description ===
=== Description ===
Perhaps even more interestingly, a ln-of-a-powharmonic series can be approximated by moving by steps of increasing equal divisions of <span><math>a</math></span>.
Perhaps even more interestingly, a ln-of-a-powharmonic series can be approximated by moving by steps of increasing equal divisions of <span><math>a</math></span>.


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=== Relation to ln-of-a-powharmonic series ===
=== Relation to ln-of-a-powharmonic series ===
The ratio between pitches of the ln-of-2-powharmonic series and the 2-edharmonic series approaches <span><math>2^γ ≈ 1.49196704047</math><span>, where <span><math>γ</math></span> is the [[wikipedia:Euler–Mascheroni_constant|Euler-Mascheroni constant]], <span><math>≈ 0.5772156649</math></span>, which represents the difference between the natural logarithm and the [[wikipedia:Harmonic_series_(mathematics)|mathematical harmonic series]] (as opposed to the musical harmonic series). This is because moving by steps of increasing equal divisions of <span><math>a</math></span> is equivalent to a series of pitches <span><math>2^{H(n)}</math></span> where <span><math>H(n)</math></span> is the <span><math>n^{th}</math></span> [[wikipedia:Harmonic_number|harmonic number]]:
The ratio between pitches of the ln-of-2-powharmonic series and the 2-edharmonic series approaches <span><math>2^γ ≈ 1.49196704047</math><span>, where <span><math>γ</math></span> is the [[wikipedia:Euler–Mascheroni_constant|Euler-Mascheroni constant]], <span><math>≈ 0.5772156649</math></span>, which represents the difference between the natural logarithm and the [[wikipedia:Harmonic_series_(mathematics)|mathematical harmonic series]] (as opposed to the musical harmonic series). This is because moving by steps of increasing equal divisions of <span><math>a</math></span> is equivalent to a series of pitches <span><math>2^{H(n)}</math></span> where <span><math>H(n)</math></span> is the <span><math>n^{th}</math></span> [[wikipedia:Harmonic_number|harmonic number]]:


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In other words, if we have gone by a step of 1ed2, we are at <span><math>2^1</math></span>. If we then go by a step of 2ed2, we have gone by <span><math>2^1 · 2^{\frac12} = 2^{\frac32}</math></span>. And a further step of 3ed2 gets us to <span><math>2^1 · 2^{\frac12} · 2^{\frac13} = 2^{\frac{11}{6}}</math></span>, etc.
In other words, if we have gone by a step of 1ed2, we are at <span><math>2^1</math></span>. If we then go by a step of 2ed2, we have gone by <span><math>2^1 · 2^{\frac12} = 2^{\frac32}</math></span>. And a further step of 3ed2 gets us to <span><math>2^1 · 2^{\frac12} · 2^{\frac13} = 2^{\frac{11}{6}}</math></span>, etc.


{| class="wikitable"
{| class="wikitable center-all"
|+
|+ Comparison of ln-of-2-Powharmonic with 2-Edharmonic series+
! rowspan="2" |pitch #
! rowspan="3" | Pitch #
! colspan="5" |ln-of-2-powharmonic series
! colspan="5" | ln-of-2-Powharmonic series
! colspan="5" |2-edharmonic series
! colspan="5" | 2-Edharmonic series
! rowspan="2" |ratio between frequency multipliers
! rowspan="3" | Ratio between frequency multipliers
|-
|-
|'''frequency multiplier (definition)'''
! colspan="2" | Frequency multiplier
|'''frequency multiplier (decimal)'''
! colspan="3" | Pitch
|'''pitch (¢)'''
! colspan="2" | Frequency multiplier
|'''pitch Δ (¢)'''
! colspan="3" | Pitch
|'''octave reduced pitch (¢)'''
|'''frequency multiplier (definition)'''
|'''frequency multiplier (decimal)'''
|'''pitch (¢)'''
|'''pitch Δ (¢)'''
|'''octave reduced pitch (¢)'''
|-
|-
|1
! Definition
|1<sup>ln(2)</sup> = 2<sup>ln(1)</sup>
! Decimal
|1
! Cents
|0.00
! Change (cents)
| -
! Octave-reduced (cents)
|0.00
! Definition
|2<sup>H(1)</sup> = 2<sup>1</sup>
! Decimal
|2
! Cents
|1200.00
! Change (cents)
| -
! Octave-reduced (cents)
|0.00
|2
|-
|-
|2
| 1
|2<sup>ln(2)</sup> = 2<sup>ln(2)</sup>
| 1<sup>ln(2)</sup> = 2<sup>ln(1)</sup>
|1.616806672
| 1
|831.78
| 0.00
|831.78
| &mdash;
|831.78
| 0.00
|2<sup>H(2)</sup> = 2<sup>3/2</sup>
| 2<sup>H(1)</sup> = 2<sup>1</sup>
|2.828427125
| 2
|1800.00
| 1200.00
|600.00
| &mdash;
|600.00
| 0.00
|1.749391052
| 2
|-
|-
|3
| 2
|3<sup>ln(2)</sup> = 2<sup>ln(3)</sup>
| 2<sup>ln(2)</sup> = 2<sup>ln(2)</sup>
|2.141486064
| 1.616806672
|1318.33
| 831.78
|486.56
| 831.78
|118.33
| 831.78
|2<sup>H(3)</sup> = 2<sup>11/6</sup>
| 2<sup>H(2)</sup> = 2<sup>3/2</sup>
|3.563594873
| 2.828427125
|2200.00
| 1800.00
|400.00
| 600.00
|1000.00
| 600.00
|1.664075677
| 1.749391052
|-
|-
|4
| 3
|4<sup>ln(2)</sup> = 2<sup>ln(4)</sup>
| 3<sup>ln(2)</sup> = 2<sup>ln(3)</sup>
|2.614063815
| 2.141486064
|1663.55
| 1318.33
|345.22
| 486.56
|463.55
| 118.33
|2<sup>H(4)</sup> = 2<sup>25/12</sup>
| 2<sup>H(3)</sup> = 2<sup>11/6</sup>
|4.237852377
| 3.563594873
|2500.00
| 2200.00
|300.00
| 400.00
|100.00
| 1000.00
|1.621174033
| 1.664075677
|-
|-
|5
| 4
|5<sup>ln(2)</sup> = 2<sup>ln(5)</sup>
| 4<sup>ln(2)</sup> = 2<sup>ln(4)</sup>
|3.05132936
| 2.614063815
|1931.33
| 1663.55
|267.77
| 345.22
|731.33
| 463.55
|2<sup>H(5)</sup> = 2<sup>137/60</sup>
| 2<sup>H(4)</sup> = 2<sup>25/12</sup>
|4.868014055
| 4.237852377
|2740.00
| 2500.00
|240.00
| 300.00
|340.00
| 100.00
|1.595374829
| 1.621174033
|-
|-
|6
| 5
|6<sup>ln(2)</sup> = 2<sup>ln(6)</sup>
| 5<sup>ln(2)</sup> = 2<sup>ln(5)</sup>
|3.462368957
| 3.05132936
|2150.11
| 1931.33
|218.79
| 267.77
|950.11
| 731.33
|2<sup>H(6)</sup> = 2<sup>49/20</sup>
| 2<sup>H(5)</sup> = 2<sup>137/60</sup>
|5.464161027
| 4.868014055
|2940.00
| 2740.00
|200.00
| 240.00
|540.00
| 340.00
|1.578156775
| 1.595374829
|-
|-
|7
| 6
|7<sup>ln(2)</sup> = 2<sup>ln(7)</sup>
| 6<sup>ln(2)</sup> = 2<sup>ln(6)</sup>
|3.852807616
| 3.462368957
|2335.09
| 2150.11
|184.98
| 218.79
|1135.09
| 950.11
|2<sup>H(7)</sup> = 2<sup>363/140</sup>
| 2<sup>H(6)</sup> = 2<sup>49/20</sup>
|6.032922891
| 5.464161027
|3111.43
| 2940.00
|171.43
| 200.00
|711.43
| 540.00
|1.56585106
| 1.578156775
|-
|-
|8
| 7
|8<sup>ln(2)</sup> = 2<sup>ln(8)</sup>
| 7<sup>ln(2)</sup> = 2<sup>ln(7)</sup>
|4.226435818
| 3.852807616
|2495.33
| 2335.09
|160.24
| 184.98
|95.33
| 1135.09
|2<sup>H(8)</sup> = 2<sup>761/280</sup>
| 2<sup>H(7)</sup> = 2<sup>363/140</sup>
|6.578949063
| 6.032922891
|3261.43
| 3111.43
|150.00
| 171.43
|861.43
| 711.43
|1.556618708
| 1.56585106
|-
|-
|9
| 8
|9<sup>ln(2)</sup> = 2<sup>ln(9)</sup>
| 8<sup>ln(2)</sup> = 2<sup>ln(8)</sup>
|4.585962562
| 4.226435818
|2636.67
| 2495.33
|141.34
| 160.24
|236.67
| 95.33
|2<sup>H(9)</sup> = 2<sup>7129/2520</sup>
| 2<sup>H(8)</sup> = 2<sup>761/280</sup>
|7.105658007
| 6.578949063
|3394.76
| 3261.43
|133.33
| 150.00
|994.76
| 861.43
|1.549436549
| 1.556618708
|-
|-
|10
| 9
|10<sup>ln(2)</sup> = 2<sup>ln(10)</sup>
| 9<sup>ln(2)</sup> = 2<sup>ln(9)</sup>
|4.933409668
| 4.585962562
|2763.10
| 2636.67
|126.43
| 141.34
|363.10
| 236.67
|2<sup>H(10)</sup>
| 2<sup>H(9)</sup> = 2<sup>7129/2520</sup>
|7.615655686
| 7.105658007
|3514.76
| 3394.76
|120.00
| 133.33
|1114.76
| 994.76
|1.543690105
| 1.549436549
|-
|-
|11
| 10
|11<sup>ln(2)</sup> = 2<sup>ln(11)</sup>
| 10<sup>ln(2)</sup> = 2<sup>ln(10)</sup>
|5.270337212
| 4.933409668
|2877.47
| 2763.10
|114.37
| 126.43
|477.47
| 363.10
|2<sup>H(11)</sup>
| 2<sup>H(10)</sup>
|8.110986229
| 7.615655686
|3623.85
| 3514.76
|109.09
| 120.00
|23.85
| 1114.76
|1.538988096
| 1.543690105
|-
|-
|12
| 11
|12<sup>ln(2)</sup> = 2<sup>ln(12)</sup>
| 11<sup>ln(2)</sup> = 2<sup>ln(11)</sup>
|5.597981231
| 5.270337212
|2981.89
| 2877.47
|104.41
| 114.37
|581.89
| 477.47
|2<sup>H(12)</sup>
| 2<sup>H(11)</sup>
|8.593290568
| 8.110986229
|3723.85
| 3623.85
|100.00
| 109.09
|123.85
| 23.85
|1.535069557
| 1.538988096
|-
|-
|13
| 12
|13<sup>ln(2)</sup> = 2<sup>ln(13)</sup>
| 12<sup>ln(2)</sup> = 2<sup>ln(12)</sup>
|5.917342318
| 5.597981231
|3077.94
| 2981.89
|96.05
| 104.41
|677.94
| 581.89
|2<sup>H(13)</sup>
| 2<sup>H(12)</sup>
|9.063911377
| 8.593290568
|3816.16
| 3723.85
|92.31
| 100.00
|216.16
| 123.85
|1.531753765
| 1.535069557
|-
|-
|14
| 13
|14<sup>ln(2)</sup> = 2<sup>ln(14)</sup>
| 13<sup>ln(2)</sup> = 2<sup>ln(13)</sup>
|6.22924506
| 5.917342318
|3166.87
| 3077.94
|88.93
| 96.05
|766.87
| 677.94
|2<sup>H(14)</sup>
| 2<sup>H(13)</sup>
|9.523965051
| 9.063911377
|3901.87
| 3816.16
|85.71
| 92.31
|301.87
| 216.16
|1.528911603
| 1.531753765
|-
|-
|15
| 14
|15<sup>ln(2)</sup> = 2<sup>ln(15)</sup>
| 14<sup>ln(2)</sup> = 2<sup>ln(14)</sup>
|6.5343793
| 6.22924506
|3249.66
| 3166.87
|82.79
| 88.93
|849.66
| 766.87
|2<sup>H(15)</sup>
| 2<sup>H(14)</sup>
|9.974392624
| 9.523965051
|3981.87
| 3901.87
|80.00
| 85.71
|381.87
| 301.87
|1.526448369
| 1.528911603
|-
|-
|16
| 15
|16<sup>ln(2)</sup> = 2<sup>ln(16)</sup>
| 15<sup>ln(2)</sup> = 2<sup>ln(15)</sup>
|6.833329631
| 6.5343793
|3327.11
| 3249.66
|77.45
| 82.79
|927.11
| 849.66
|2<sup>H(16)</sup>
| 2<sup>H(15)</sup>
|10.41599671
| 9.974392624
|4056.87
| 3981.87
|75.00
| 80.00
|456.87
| 381.87
|1.524293028 ... -> 2<sup>γ</sup> = 1.49196704047
| 1.526448369
|-
| 16
| 16<sup>ln(2)</sup> = 2<sup>ln(16)</sup>
| 6.833329631
| 3327.11
| 77.45
| 927.11
| 2<sup>H(16)</sup>
| 10.41599671
| 4056.87
| 75.00
| 456.87
| 1.524293028 ... &rarr; 2<sup>&gamma;</sup> = 1.49196704047
|}
|}


Line 357: Line 353:
In the case of the (2-)edharmonic series, doing so brings it closer in similarity to the (musical) harmonic series; the first step is exactly an octave, the second step a fifth (701.96¢ vs 600.00¢), the third step a fourth (498.04¢ vs 400.00¢), the fourth step a third, (386.31¢ vs 300¢), etc. This similarity could be useful when using the entire series as a scale rather than drawing scales from it. We therefore propose referring to this variation as the "emulatory edharmonic series", because it emulates the harmonic series.
In the case of the (2-)edharmonic series, doing so brings it closer in similarity to the (musical) harmonic series; the first step is exactly an octave, the second step a fifth (701.96¢ vs 600.00¢), the third step a fourth (498.04¢ vs 400.00¢), the fourth step a third, (386.31¢ vs 300¢), etc. This similarity could be useful when using the entire series as a scale rather than drawing scales from it. We therefore propose referring to this variation as the "emulatory edharmonic series", because it emulates the harmonic series.


{| class="wikitable"
{| class="wikitable center-all"
|+
|+ Comparison of harmonic series and emulatory edharmonic series
! rowspan="2" |pitch #
! rowspan="3" | Pitch #
! colspan="4" |harmonic series
! colspan="4" | Harmonic series
! colspan="5" |emulatory edharmonic series
! colspan="5" | Emulatory edharmonic series
|-
! Frequency multiplier
! colspan="3" | Pitch
! colspan="2" | Frequency multiplier
! colspan="3" | Pitch
|-
|-
|'''frequency multiplier (decimal)'''
! Decimal
|'''pitch (¢)'''
! Cents
|'''pitch Δ (¢)'''
! Change (cents)
|'''octave reduced pitch (¢)'''
! Octave-reduced (cents)
|'''frequency multiplier (definition)'''
! Definition
|'''frequency multiplier (decimal)'''
! Decimal
|'''pitch (¢)'''
! Cents
|'''pitch Δ (¢)'''
! Change (cents)
|'''octave reduced pitch (¢)'''
! Octave-reduced (cents)
|-
|-
|1
| 1
|1.000000
| 1.000000
|0
| 0
| -
| &mdash;
|0
| 0
|2<sup>H(0)</sup> = 2<sup>0</sup>
| 2<sup>H(0)</sup> = 2<sup>0</sup>
|1.000000000
| 1.000000000
|0
| 0
| -
| &mdash;
|0
| 0
|-
|-
|2
| 2
|2.000000
| 2.000000
|1200
| 1200
|1200
| 1200
|0
| 0
|2<sup>H(1)</sup> = 2<sup>1</sup>
| 2<sup>H(1)</sup> = 2<sup>1</sup>
|2.000000000
| 2.000000000
|1200.00
| 1200.00
|1200.00
| 1200.00
|0.00
| 0.00
|-
|-
|3
| 3
|3.000000
| 3.000000
|1901.955001
| 1901.955001
|701.955001
| 701.955001
|701.955001
| 701.955001
|2<sup>H(2)</sup> = 2<sup>3/2</sup>
| 2<sup>H(2)</sup> = 2<sup>3/2</sup>
|2.828427125
| 2.828427125
|1800.00
| 1800.00
|600.00
| 600.00
|600.00
| 600.00
|-
|-
|4
| 4
|4.000000
| 4.000000
|2400
| 2400
|498.044999
| 498.044999
|0
| 0
|2<sup>H(3)</sup> = 2<sup>11/6</sup>
| 2<sup>H(3)</sup> = 2<sup>11/6</sup>
|3.563594873
| 3.563594873
|2200.00
| 2200.00
|400.00
| 400.00
|1000.00
| 1000.00
|-
|-
|5
| 5
|5.000000
| 5.000000
|2786.313714
| 2786.313714
|386.313714
| 386.313714
|386.313714
| 386.313714
|2<sup>H(4)</sup> = 2<sup>25/12</sup>
| 2<sup>H(4)</sup> = 2<sup>25/12</sup>
|4.237852377
| 4.237852377
|2500.00
| 2500.00
|300.00
| 300.00
|100.00
| 100.00
|-
|-
|6
| 6
|6.000000
| 6.000000
|3101.955001
| 3101.955001
|315.6412870
| 315.6412870
|701.955001
| 701.955001
|2<sup>H(5)</sup> = 2<sup>137/60</sup>
| 2<sup>H(5)</sup> = 2<sup>137/60</sup>
|4.868014055
| 4.868014055
|2740.00
| 2740.00
|240.00
| 240.00
|340.00
| 340.00
|-
|-
|7
| 7
|7.000000
| 7.000000
|3368.825906
| 3368.825906
|266.8709056
| 266.8709056
|968.825906
| 968.825906
|2<sup>H(6)</sup> = 2<sup>49/20</sup>
| 2<sup>H(6)</sup> = 2<sup>49/20</sup>
|5.464161027
| 5.464161027
|2940.00
| 2940.00
|200.00
| 200.00
|540.00
| 540.00
|-
|-
|8
| 8
|8.000000
| 8.000000
|3600
| 3600
|231.1740935
| 231.1740935
|0
| 0
|2<sup>H(7)</sup> = 2<sup>363/140</sup>
| 2<sup>H(7)</sup> = 2<sup>363/140</sup>
|6.032922891
| 6.032922891
|3111.43
| 3111.43
|171.43
| 171.43
|711.43
| 711.43
|-
|-
|9
| 9
|9.000000
| 9.000000
|3803.910002
| 3803.910002
|203.9100017
| 203.9100017
|203.910002
| 203.910002
|2<sup>H(8)</sup> = 2<sup>761/280</sup>
| 2<sup>H(8)</sup> = 2<sup>761/280</sup>
|6.578949063
| 6.578949063
|3261.43
| 3261.43
|150.00
| 150.00
|861.43
| 861.43
|-
|-
|10
| 10
|10.000000
| 10.000000
|3986.313714
| 3986.313714
|182.4037121
| 182.4037121
|386.313714
| 386.313714
|2<sup>H(9)</sup> = 2<sup>7129/2520</sup>
| 2<sup>H(9)</sup> = 2<sup>7129/2520</sup>
|7.105658007
| 7.105658007
|3394.76
| 3394.76
|133.33
| 133.33
|994.76
| 994.76
|-
|-
|11
| 11
|11.000000
| 11.000000
|4151.317942
| 4151.317942
|165.0042285
| 165.0042285
|551.317942
| 551.317942
|2<sup>H(10)</sup>
| 2<sup>H(10)</sup>
|7.615655686
| 7.615655686
|3514.76
| 3514.76
|120.00
| 120.00
|1114.76
| 1114.76
|-
|-
|12
| 12
|12.000000
| 12.000000
|4301.955001
| 4301.955001
|150.6370585
| 150.6370585
|701.955001
| 701.955001
|2<sup>H(11)</sup>
| 2<sup>H(11)</sup>
|8.110986229
| 8.110986229
|3623.85
| 3623.85
|109.09
| 109.09
|23.85
| 23.85
|-
|-
|13
| 13
|13.000000
| 13.000000
|4440.527662
| 4440.527662
|138.5726609
| 138.5726609
|840.527662
| 840.527662
|2<sup>H(12)</sup>
| 2<sup>H(12)</sup>
|8.593290568
| 8.593290568
|3723.85
| 3723.85
|100.00
| 100.00
|123.85
| 123.85
|-
|-
|14
| 14
|14.000000
| 14.000000
|4568.825906
| 4568.825906
|128.2982447
| 128.2982447
|968.825906
| 968.825906
|2<sup>H(13)</sup>
| 2<sup>H(13)</sup>
|9.063911377
| 9.063911377
|3816.16
| 3816.16
|92.31
| 92.31
|216.16
| 216.16
|-
|-
|15
| 15
|15.000000
| 15.000000
|4688.268715
| 4688.268715
|119.4428083
| 119.4428083
|1088.268715
| 1088.268715
|2<sup>H(14)</sup>
| 2<sup>H(14)</sup>
|9.523965051
| 9.523965051
|3901.87
| 3901.87
|85.71
| 85.71
|301.87
| 301.87
|-
|-
|16
| 16
|16.000000
| 16.000000
|4800
| 4800
|111.7312853
| 111.7312853
|0
| 0
|2<sup>H(15)</sup>
| 2<sup>H(15)</sup>
|9.974392624
| 9.974392624
|3981.87
| 3981.87
|80.00
| 80.00
|381.87
| 381.87
|}
|}