Authors

  • Tojiev Rasuljon
    Doctor Of Technical Sciences, Professor, Fergana Polytechnic Institute, Fer-Gana, Republic Of Uzbekistan
  • Abdurakhmon Sulaymanov
    Doctoral Student, Fergana Polytechnic Institute, Republic Of Uzbekistan, Fergana
  • Gulmiraxon Madaminova
    Assistant, Fergana Polytechnic Institute, Republic Of Uzbekistan, Fergana
  • S.U. Agzamov
    Assistant, Fergana Polytechnic Institute, Republic Of Uzbekistan, Fergana

DOI:

https://doi.org/10.71337/inlibrary.uz.ijasr.130837

Keywords:

Technology grinding clinker powder slurry surfaces

Abstract

The article is written about the fact that a lot of electricity is consumed in the process of grinding materials in cement production technology, and to ensure the efficiency of material grinding by studying the reasons where it is spent.

 


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Volume 02 Issue 11-2022

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International Journal of Advance Scientific Research
(ISSN

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VOLUME

02

I

SSUE

11

Pages:

25-34

SJIF

I

MPACT

FACTOR

(2021:

5.478

)

(2022:

5.636

)

METADATA

IF

7.356



















































A

BSTRACT

The article is written about the fact that a lot of electricity is consumed in the process of grinding materials
in cement production technology, and to ensure the efficiency of material grinding by studying the reasons
where it is spent.

K

EYWORDS

Technology, grinding, clinker, powder, slurry, surfaces, forging, friction, molecule, deformation crystal, soft,
elastic, plastic.

I

NTRODUCTION

Journal

Website:

http://sciencebring.co
m/index.php/ijasr

Copyright:

Original

content from this work
may be used under the
terms of the creative
commons

attributes

4.0 licence.

Research Article

GRINDING OF MATERIALS: MAIN CHARACTERISTICS


Submission Date:

November 05, 2022,

Accepted Date:

November 10, 2022,

Published Date:

November 18, 2022

Crossref doi:

https://doi.org/10.37547/ijasr-02-11-05


Tojiev Rasuljon

Doctor Of Technical Sciences, Professor, Fergana Polytechnic Institute, Fer-Gana, Republic Of Uzbekistan

Abdurakhmon Sulaymanov

Doctoral Student, Fergana Polytechnic Institute, Republic Of Uzbekistan, Fergana

Gulmiraxon Madaminova

Assistant, Fergana Polytechnic Institute, Republic Of Uzbekistan, Fergana

S.U. Agzamov

Assistant, Fergana Polytechnic Institute, Republic Of Uzbekistan, Fergana


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VOLUME

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Pages:

25-34

SJIF

I

MPACT

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(2021:

5.478

)

(2022:

5.636

)

METADATA

IF

7.356















































The process of grinding materials is very
complicated and depends on the following
factors: physical and mechanical properties of the
material, its shape, size and granularity, the
number of defects in the material, its strength,
hardness or softness, and the construction and
types of other grinding machines [1-7].

In order to correctly interpret this situation, it is
necessary to study the physical state of the
grinding process. For example. The grinding

process due to any deformation can be explained
as follows. The external force causes the
accumulation of elastic deformation stresses in
the div [8-15].

T

HE MAIN PART

If we compare the above-mentioned hypotheses
and compare the grinding with the work done,
and put the pieces of grinding on the Hooke
diagram, we get the following [14-21].

Figure 1. The relationship between the unit energy consumption E and the final size of the

material being crushed D.

As can be seen from the diagram, the energy
consumption is 0.4kW to get 1t rubble 5-40mm;

Grinding 1t of sand is 2kW with a unit surface
area of 1800cm2/g; 1t of cement (from clinker) is

Е

,

кВт

/

Т

10

5

10

4

10

3

10

2

10

1

0.1

0.0001 0.01 10 100 1000

Д

,

мм


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SJIF

I

MPACT

FACTOR

(2021:

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)

(2022:

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)

METADATA

IF

7.356















































2800-3000 cm2/g and 7 kW of energy is
consumed. In fact, it takes 35-45 kW of energy to
produce 1 ton of cement from clinker, which is
very energy intensive. This shows that such
calculations Rittinger, Kirpichev-Kick and Bond
hypotheses do not accurately represent this
process. But it correctly expresses the quality
characteristics of grinding processes [22-28].

According to Griffiths, the difference between the
theoretical and actual strength of solid bodies
occurs due to the formation of small cracks in
them, resulting in strong concentrated stress. The
basic idea used by Griffiths is that under the
influence of the recommended tensile stress at

the tips of small cracks, a local overstress σ is

calculated in all sections of the sample, which is

many times more than the average stress σ.

If the stress is too high, dangerous cracks will

reach the theoretical strength σК, in which the

crack will grow violently and break the specimen
into pieces. The recommended average voltage at
this time should correspond to the peak voltage

σК. When the ultimate stress is less than the

theoretical strength, the crack does not grow and
the material does not crush. The coefficient of
stress concentration in microcracks is equal to

β=σ*/σ. It depends on

the direction, size and

shape of the micro-cracks according to the
direction of elongation. Therefore, tensile
strength is not considered to be related to the
material constant. Different samples differ in the
size of critical microcracks [29-33].

In justifying the formula for the calculation of
concentration stresses, Griffiths based on the
following cases:

a) thermal failure of brittle material does not
depend on temperature;

b) if an increase in the free plane energy is
observed to increase tension micro-cracks in the
sample, the growth of micro-cracks may occur.

c) the length of microcracks is much shorter than
the cross-section of the sample, and the cross-
sectional stress in the crack practically
corresponds to the average stress calculated at
the nominal strength.


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VOLUME

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Pages:

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SJIF

I

MPACT

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(2021:

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)

(2022:

5.636

)

METADATA

IF

7.356















































Figure 2. The diagram of stress concentration at the crack tip.

Based on this situation, Griffiths defined the intensity as follows:

0

2

к

E l

=

where: a-energy of free formation of a tense div; E-voltage module; 1

0

-angle microcracks initial depth.

According to modern views, Griffiths theory has a

number of shortcomings. The main ones are:

1) The calculation of concentration stresses does not

depend in principle on the equality of the tension energy

change and the change of the energy of free formation,

in which, according to the law of conservation of energy,

it is necessary to take into account the mechanical loss of

the crushing energy of a brittle div;

2) Griffiths's theory does not take into account the

dependence on temporal stability;

3) Molecular structure is not taken into account.

In justification of the final state, we consider the

molecular model of microcracks and the mechanism of

their growth in a brittle solid. At the boundary of the

integral transition to free formation, a discontinuity

occurs between atoms. Atoms up to 1...5 are located in

the volume of the div, and up to 6...10 are in free


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VOLUME

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SJIF

I

MPACT

FACTOR

(2021:

5.478

)

(2022:

5.636

)

METADATA

IF

7.356















































formation. Due to thermal motion and fluctuation, the

atoms at the tip of the cracks periodically generate

sufficient kinetic energy or try to restore the bond

between them. This process is observed when the

potential overcomes the E and E1 barriers. The kinetic

energy of particles is the activity energy of breaking

processes or restoring chemical bonds. E-

Е

1

differences

have a potential generation energy, which can be

considered as a function of the distance between

particles in the direction of elongation [34-41].

0

х

=

and

0

х

 =

. The charge equal to should

correspond to the balance of the distance between the

intermediate atoms on the surface of the layer in the

non-given div. The maximum of the potential curve

indicates the influence of the nearby layer of atoms on

the bond breaking process. The presence of particles in

the x zone in the loaded material

х

is higher than in the

zone [42-46]. After unloading, the crack coalesces to the

defect. In a loaded material, the tensile stress prevents

the bonds from breaking and restoring them, which in

turn means that in the unloaded state, the bonds are

short and require a large kinetic energy to break. At high

strain, the bond discontinuities are large and lead to the

growth of microcracks.

σ=σ

0

is assumed to be safe in case

of potential failure and the equality of restored

connections.


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)

(2022:

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)

METADATA

IF

7.356















































Figure 3. molecular model of α

-microcracks;

β

-potential energy change.

The external force causes the accumulation of
elastic deformation forces inside the div (piece).
The concentrated stress formed as a result of a
defect somewhere in the piece increases without
reaching the strength limit, and part of it is spent
on the newly formed surface, this energy is useful
energy and grinds the piece. And the rest are
distributed in the case of elastic deformation to
compress the piece, in the case of thermal energy
and in the case of other energies.

Thus, according to modern views, there are two
types of crushing mechanism. In the first stage,
the cracks are provided by thermofluctuation,
and in the second stage, the tensile properties of
the solid div are determined by the growth of
the cracks, and the energy reserve is stored in it.

R

EFERENCES


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)

(2022:

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Tojiev, R., Alizafarov, B., & Muydinov, A. (2022). Theoretical analysis of increasing conveyor tape endurance. Innovative Technologica: Methodical Research Journal, 3(06), 167-171.

Тожиев, Р. Ж., Миршарипов, Р. Х., & Ражабова, Н. Р. (2022). Гидродинамические Режимы в Процессе Сушки Минеральных Удобрений. Central asian journal of theoretical & applied sciences, 3(5), 352-357.

Tojiev, R. J., & Isomidinov, A. S. (2022). Application of the principle of gas dynamics to agricultural technologies: monograph. Publishing house «European Scientific Platform», 72-72.

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