Breakage and entropy Fractal distribution in nature Questions arisen - - PowerPoint PPT Presentation

breakage and entropy
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Breakage and entropy Fractal distribution in nature Questions arisen - - PowerPoint PPT Presentation

Breakage and entropy Fractal distribution in nature Questions arisen from literature Why fractal distribution is so frequent? It is true that fractal dimension is always less than 3? Is there an ultimate distribution? Why fractal


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SLIDE 1

Breakage and entropy

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SLIDE 2

Fractal distribution in nature

Questions arisen from literature

  • Why fractal distribution is so frequent?
  • It is true that fractal dimension is always less than 3?
  • Is there an ultimate distribution?
  • Why fractal distribution with a fractal dimension of around

2.5–2.6 seems to be steady-state or stable?

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SLIDE 3

Entropy notions

  • classical entropy of thermodynamics (Sc) (Clausius

(1865))

  • statistical formulation of the classical entropy of

thermodynamics (Sf),

  • statistical entropy (Ss)
  • entropy of information theory (SI)
  • grading entropy
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SLIDE 4

Entropy principle

The directional properties of natural or spontaneous processes (‘entropy principle’):

  • In the classical sense, the second law of thermodynamics

states: “In any closed system the entropy remains constant or increases during the ongoing processes “ (Breuer, 1993).

  • It is true that grading entropy can be related to the entropy

principle?

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SLIDE 5
  • Basic assumption: Largest fraction does not

disappear

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SLIDE 6

Hard grains

Sand samples:

  • One fraction sand
  • Concave fractal
  • Convex fractal
  • Silica, carbonate
  • Each sample was subjected to a series of crushing treatments

using a special reinforced crushing pot, made at the Geotechnical Department with the dimensions: diameter: 50 mm, height: 70 mm, wall thickness: 3mm.

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SLIDE 7

Oedometer pot

  • képek
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SLIDE 8

The continuous grading curve path in the non- normalised diagram

0.0 2.0 4.0 6.0 8.0

Base entropy, S [-]

0.0 0.4 0.8 1.2 1.6 2.0 2.4 2.8

Entropy increment, S [-]

N=7 N=5 N=3 N=4 N=6 N=2 0.3

0.2 0.1

0.0 2.0 4.0 6.0 8.0

Base entropy, S [-]

0.0 0.4 0.8 1.2 1.6 2.0 2.4 2.8

Entropy increment, S [-]

N=7 N=5 N=3 N=4 N=6 N=2

0.4 0.6

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SLIDE 9

The discontinuous grading curve path in the normalised diagram

0.00 0.20 0.40 0.60 0.80 1.00 A [-] 0.00 0.40 0.80 1.20 1.60 B [-]

continuous breakage path from dolomitic and silica sand data theoretical jump

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SLIDE 10

Initially one fraction soil

0.6 0.8 1.0

Relative base entropy, A (-)

0.0 0.4 0.8 1.2

Entropy increment, B [-]

maximal entropy point for 6 fractions 7 fractions A=2/3 n=45 n=1 n=0 n=105, n=125, n=85 n=65

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SLIDE 11
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SLIDE 12

0.0 0.2 0.4 0.6 0.8 1.0

A [-]

0.0 0.4 0.8 1.2

B [-]

Initial (N=2) N=3 discontinuity jumps (smaller fractions added) (larger fractions added) (both smaller and larger fractions added) N=4 N=3 4

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SLIDE 13

Comments on the normalized entropy path

  • Why fractal distribution is so frequent?
  • If N is constant, the path goes towards the maximum B

line, where all grading curves have finite fractal distribution.

  • On the A>0.5 side of the maximum B line, the

fractal dimension n varies between 3 and - infinity.

  • On the A<0.5 side of the maximum normalized

entropy increment line, the fractal dimension n varies between 3 and plus infinity.

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SLIDE 14

Normalized grading entropy diagram stability rule and fractal dimension

0.6 0.8 1.0

Relative base entropy, A [-]

0.0 0.4 0.8 1.2

Entropy increment, B [-]

II.

a b c d e f

I.

2 3 4 5 6 7

III.

1

1: maximum entropy increment point where the fractal dimension is n=3 independently of N. 2, 3, 4…7 : maximum entropy points for N = 2, 3, 4…7, the fractal dimension is n=2 since dependent on N except in point 1. I, II, III: Grain structure stability domains for N=7 I: piping, II: stable, III: stable with suffosion.

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SLIDE 15

Some conclusions – hard grains

  • The base entropy So decreases, the entropy increment ΔS

strictly monotonically increases. The breakage speed is different for silica and carbonate sand, the path is similar. It is true that grading entropy can be related to the entropy principle?

  • It follows from the measured data that the entropy principle

is valid for the ΔS entropy coordinate.

  • (The base entropy So decrease can be explained by the

decrease of the mean grain diameter during breakage.)

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SLIDE 16
  • Why fractal distribution with n<3 is so frequent? If a

smaller fraction appear, the normalized entropy path has a discontinuity, increasing the A value and decreasing B value.

  • As a result, the normalised entropy path is drifted into the

right side of the diagram n <3, A>0.5. That is why the structurally stable grading curves (A>2/3 ) occur more frequently than the structurally unstable ones.

  • This can be used in rock testing.
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SLIDE 17
  • Is there an ultimate state?
  • Applying the entropy principle to the non-normalized

grading entropy B, a theoretical ultimate state is resulted, the symmetry point of the maximum line, with fractal dimension n =3.

  • This can be reached by tests with topology change
  • nly (applied here) on condition that N stops to

increase and large grains remain.

  • Further research is suggested on this and on soft

rocks where the largest fraction does not remain.