CA2304583C

CA2304583C - X-ray absorbing material and variants

Info

Publication number: CA2304583C
Application number: CA002304583A
Authority: CA
Inventors: Vladimir Ivanovich Tkatchenko; Valeriy Anatolievich Ivanov; Valeriy Ivanovich Petchenkin; Stanislav Yurivich Sokolov; Igor Stepanovitch Nosov
Original assignee: Individual
Current assignee: Individual
Priority date: 1997-09-30
Filing date: 1998-09-24
Publication date: 2004-12-07
Anticipated expiration: 2018-09-24
Also published as: KR20010015675A; WO1999017303A1; PL339648A1; TR200000758T2; CN1147875C; HUP0003892A2; KR100450247B1; LV12509A; PL189266B1; CN1375105A; IL135041A; EP1020874B1; EA200000621A1; EA002078B1; DE69829767D1; AU9655098A; RO120513B1; DK1020874T3; LV12509B; IL135041A0

Abstract

The present invention relates to an X-ray absorbing material which can be used in medicine as well as in the production of special protection clothes, protection screens, housings, protection coatings and isolation materials. In a first embodiment, the material uses as a filler a poly-dispersed kneading-segregated mixture containing metallic particles having a size of between 10 -9 and 10 -3 m, wherein said particles are bonded to the surface of a textile base. The density of the material is defined by the relation q N = (0.01 - 0.20)q P where q N is the density of the X-ray absorbing material as a whole while q P is the density of the material used for the particles of the X-ray absorbing filler. In a second embodiment, this invention uses as a filler the above-mentioned mixture though the particles are surrounded by the volume of a matrix made of a compound that solidifies under atmospheric pressure. The total mass of the poly-dispersed and segregated mixture is defined by the relation M = (0.05 - 0.5)m where M is the total mass of the X-ray absorbing poly-dispersed and segregated filler, while m is the equivalent mass of the filler material which is equal by its protection properties to the mass M. In a third embodiment, this invention uses as a filler the above-mentioned mixture though the particles are bonded to an intermediate substrate consisting of a textile base and surrounded by the volume of a matrix.

Description

X-ItAY Af3SO1t13IN(: MA'fh~RIAI, (VAItIAN'I'S).
'I~he invention relates to X-ray contrasting and X-ray protection materials attd can be used in medicine, namely in roentgen equipment intended for diagnostics and inspection ill, specifically for monitoring over condition of endo-prosthetic appliances, internal surgical wields, post-surgical area in order to avoid leaving a surgical napkin, tampon or surgical inslruntents inside the body of a patient, for selection of exposure areas in the course oh radio-therapy, etc., as well as for production of protective uniform (aprons, smocks, waistcoats, caps, etc.), production of protection shields, partitions, protection coiling, isolation materials, ctc.
Previous level of engineering.
Known is an X-ray absorbing tnalerial, for example, under the Patent of Sweden N« 34936(i, J 960, providing for an artificial rayon threat( which contains barium sullale (l3<tSU~r) in the (orm of mechanical impurity (15 up to 65 % ol~ mass). I lowever, adding of the mentioned mechanical impurity to the textile base of material results in abrupt reduction of its durability.
Known are X-ray absorbing materials, executed, for example, in the lortn of tltreac(s which contain bismuth oxide, colloidal silver, iodine derivatives as X-ray contrasting impurities added to the polymeric composition (ref, to X-ray absorbing malertals descrtbcd, (itr example, in tltc Abstract of n. V. Vitulsky, Master of Science, ttatned O)btaittittg amt research of synthetic fibers with the X-ray contrasting and anti-germ preparations being added at the time of~ forming», Leningrad, 1971).
however, examining oh properties of a textile base containing such impurities has shown that due to violation of the fiber structure homogeneity, caused by negative in(lucncc of contrasting impurity particles, the worsening of the physical and mec)tanical properties of Iibcrs and threads made on the base of the mentioned impurities takes place.
~1 textile base containing such impurities lacks durability and this factor limits the Iic(d ol~ application thcreoh.
KIlowIl IS all X-ray absorbing material, for example, under the Certificate of nutltorship of Bulgaria N~ 36217, 1980, made in the form of a thread containing X-ray protection coating produced of heavy metals, plotted by means of falling out in corresponding calls solutes.
Unlike the tllatel'lalS tllelltlOlled above, this one has better physical and ntecltanical properties since the pluttillg of tllc coating by falling out of heavy metals froln solute does noU rcallly al7cct the mechanical properties of the initial material. Nevertheless, tl~c small width ol~ tllc coating causes lhc low creel X-ray contrasting and X-ray protection properties. Ivrtllcrnlurc, the weak adhesion of the X-ray absorbing coating towards initial material alter washing, cleaning and so on, causes abrupt reduction of X-ray contrasting and X-ray protective pr opcrties.
Known is an X-ray absorbing material under tile Ccrtilicatc of /lutllursllip N« 1826173 n611; 17/SG, 17/00, U.S.S.R., 1980, which, having the merits of a material made in the form of the tllrcad .containing the X-ray absorbing coating of heavy 'nlclals, is devoid mf its drawbacks due to the fact that the X-ray absorbing coating is made of ultra dispersible particles (UDl') with sizes of between 100' and lU-~ m and (laving such properly like abnormal weakening of radiation (according to «1'henomenon of abnormal reduction of X-ray radiation by ultra dispersible environmcnt», 1)Iploma N« 4 of the RIISSIaII
Nalur:ll Science /lcadcmy, priority dale - US/07/87). 'I~he metal-containing element (slze of between _- 10 '' and 10-' m) lincly ciispcrsiblc Illixture of this material is bonded to tllc surlacc of tllrt;ad i. c~. mo the textile base surface. 1-lowever, the use of finely dispersible mixture only in the range of ultra dispersible particles (between 10-~ and 10-' m), which arc chemically and physically Iissile and pyrophoric, is technologically problematic since it reduires special COIICIIlII)I1S Uf 111aI1t11:1Ct111'e, ll'allsp0l'tlllg, Storage alld leChIlOfUglcal appllCall0ll.
As a result of the recent discovery in the licld of physics of poly-dispersed environment named «7'he phenomenon of the permeating radiation quantum stream intensity abnormal alteration by mono- and multiple environment» (Diploma No. 57 of the Russian Natural Science Academy, priority date - 09/19/96; published 1998 by the Edition House of the Russian Natural Science Academy, RAEM, Moscow, Russia, in a collection entitled "Collection of Brief Descriptions. SCIENTIFIC DISCOVERIES For 1997", Ivanor, V.A., et al.) it was ascertained that the poly-dispersed environment, provided that the certain dispersibility of particles and segregation thereof by intcrlnixing is ensured, also reveals the capability of abnormally high reduction of X-radiation, which is conditioned by self=organization of poly-dispersed particles having a size elf between clot thousandth and hundreds of micrometers into energetically interconnected X-ray absorbing cnscanblcs. (Segregation of poly-dispersed mixture denotes irregular distribution of tllc puly-dispersed mixture particles caused by intermixing of the mixture, due to self organization of particles into the system of energetically interconnected ensembles ensuring the increasing of the photo-absorption cut). Meanwhile it is generally known that the use of poly-dispersed 2a mixtures consisting of particles having a size of between 109 up to 10-; in modern engineering does not require any specific limitations and is not (naught with any specific technological difficulties in manufacture, transportation, storage and use.

Known is an X-ray absorbing material containing, for example, a rubber matrix with a fixed X-ray absorbing filler under the U. S. patent N~ 3239669, 1966.
According to the patent, the X-ray absorbing elements in the form of lead, bismuth, silver and tungsten can be used as a filler. The main drawback of the mentioned material is reduction of solidity of material in 2-3 times due to the negative influence of the absorbing particles of filler violating the uniform structure of the original polymeric mass.
Known are another X-ray absorbing materials containing a matrix with a fixed X-ray absorbing filler or, for example, in the form of golden tubes, under the U. S.
patent N
2153889, 1939 or in the form of wire made of silver-, bismuth-, tantalum-containing alloys, wherein the said wire and the matrix are fastened together by interweaving and forming a kind of a textile thread (U. S. patent Ns 3194239, 1965).
Materials containing a matrix with a fixed X-ray absorbing filler in the form of wire made of silver-, bismuth-, tantalum-containing alloys, wherein the said wire and the matrix are fastened together by interweaving and are forming a textile thread, are preferable in comparison with the materials under the U.S. patent Ns 2153889, if taking into account such property as solidity, but have lower plasticity, which is inadmissible in many cases.
Known are materials protecting from impact of X- and gamma-radiation containing heavy fillers, the most spread of which is, for example, lead (Article named «1'echnical headway in atomic engineering, Series «Isotopes in U. S. S. R», 1987, edition 1 (72), p. 85).
Iaue to the great difference in density between a filler (for example, lead) and a matrix (for example, concrete, polymers, etc.) the filler (lead) is being spread along the matrix volume irregularly which results in decrease of the X-ray absorbing properties of material as a whole.
Known is an X-ray absorbing material executed, for example, on the basis of the polysterol polymeric matrix and lead-containing organic filler, under the U.K.
patent N
1260342, G 21 F 1/10, 1972. The said material has the same drawback as the lead-containing fillers described in the article «Technical headway in atomic engineering, Series «Isotopes in U. S. S. R», 1987, edition 1 (72), p. 85, which consists in irregular distribution of heavy X-ray absorbing filler inside the matrix, the material of which has considerably lower density than the material of filler.
The closest to the offered invention is an X-ray absorbing material containing a matrix with the fixed X-ray absorbing metal-containing filler in the form of dispersed particles, under the Russian Federation patent Ns 2063074 G21 F 1/10 of 06/27/96 (prototype).
The drawback of the said material consists in the fact that adding of a lead-containing filler to a textile base results in reduction of density of the material due to the violation of the textile base uniform structure, that limits, in its turn, the possibility of use thereof for manufacture of various protective means. Material executed on the basis of a thread with a lead-containing filler can not be used as an X-ray contrasting material in medical radiology due to the lead's toxic properties. Furthermore, it is impossible to create effective compact protection from X- and gamma-radiation on the basis of such material as a thread (analogue thereof, for example, is described in the Russian Federation patent Ns 2063074) as in this case for purposes of using the said thread-material it is necessary to apply the special technology of dense multi-layer machine knitting for manufacture of multipurpose protective tissue. But thus, as the weakening of a narrow bundle of quantums by a stratum of a material having width = X
happens according to the exponential law, in compliance with the legitimacy described in the book "Methods of radiation granulometry and statistical simulation in research of structural properties of composite materials. " (V. A. Vorobiev, B. E. Golovanov, S. I.
Vorobieva, Moscow, Energoatomizdat, 1984), happens reduction of radiation intensity:
I=Io e-~" ( 1 ) Where I is the intensity of radiation passed through a stratum of material having width = X, Io is the intensity of initial radiation, ~t is the linear factor of radiation reduction (weakening) (tabular regulated value for each of X-ray absorbing materials).
The drawback of the prototype consists also in high percentage of a metal-containing filler in total amount of the X-ray absorbing material (66 - 89 %), that will cause increase of the mass of X-ray absorbing material as a whole, and on the other hand, the articles made out of such material are heavy and inconvenient in maintenance.
The irregular distribution of the heavy filler in the matrix volume is one more drawback of the mentioned prototype.
Disclosure of invention The main tasks in the course of development of X-ray absorbing (i. e. X-ray contrasting and X-ray protective) materials are:
- to eliminate toxicability of an X-ray contrasting material, - to reduce the mass and width of a protective material.

Elimination of toxicability is achieved through the application of non-toxic fillers (tungsten, for example). And creation of compact protection with the protective material width reduced together with saving of X-ray absorbing properties (i. e. X-ray and gamma-radiation reduction degree) leads to increasing of the material protective layer mass caused by use of "heavy"
fillers, i. e. filler of high density. Vice versa, when the X-ray absorbing properties are saved, reduction of protective material density causes the necessity of increasing of its width.
Let's illustrate this position on an example of an X-ray absorbing material in the form of a protective tissue (radiologist' protective apron, for example) which ensures protection characterized by the reduction factor K=100. It is possible to deduce from Formula ( 1 ) as follows:
K=Io/I= e~X =100, Whence it follows x=1nK/p=4,6/p (2) As an example, let's compare properties of tissues made of threads containing the known fillers in the form of non-segregated dispersed particles of lead (Pb) and tungsten (W). The size of the compared tissues was set as 10 x 10 cm. The rest initial data for comparison are shown in Table 1.
Table 1.
Initial data for comparison.
Material used for the Linear factor radiationParticles material particles of of density, filler reduction p g/sm3 (weakening), ~, cm~>

Pb 40,3 11,34 W 50,1 18,7 '~) ttemarlc: radiation source is an X-ray emittW g (roentgen) tube, energy -60 keV.
It is possible to deduce from Formula (2), using the data of Table 1, the values of width X for tissues made of threads with a filler made of:

G
I'b (X= 0,1 1 c;m) and of W (X= 0,09 cm).
accordingly the mass ul'such protection tissues with vululne of IU x 10 x X
will constitute:
for I'b - 124,74 .g, f or Vv~ - I 68,3 g.
)f the IlIaSS of a protection tissue on the fb basis is taken for 1, then (by equal Iroteclive properties and equal sizes) the ratio of masses of tissues made un the base of threads containing 1'b :rnd Vv - will be 1:1,35.
'Thus, it 1S 1111p05S1bIC l0 017ta111 SII11111ta11COlIS 1'cdttctloll Of the protective nrllerial width and 111aSS tlSlng the prototype and known similar technologies.
ncc~rding to the present invention the set tasks are solved by Illeillls 111eI1tIUllt;d in the distinctive part of independent claims of the invention formula.
In a first embodiment of an X-ray absorbing material comprising a matrix with lixed X-ray absorbing metal-containing filler, the said material uses as a tiller the segregated by intcrmiriil~, poly-dispersed mixture containing metallic particles having a sioc of hctw~cen 1 ()-'' and 10-x. while the textile base serves as a matrix. ~\s this takes place, the particles are bonded to the surface of said textile base and the density of X-ray absorbing material as a whole, at X-ray absorbing properties of the material being equal to those of the material used lur tllc particles of the X-ray absorbing filler, is defined by the relation:
p ..._ (U,01 - U,2U)lln, where: p ", - density of X-ray absorbing material as a whole, while ~,, is the dcnsiy of the material used for the particles of the X-r111' nhscorhing filler.
According to one aspect of the present invention, there is provided an X-ray absorbing material comprising a matrix with a fixed X-ray absorbing metal-containing filler in the form of dispersed particles, wherein the filler is a poly-dispersed mixture containing metallic particles having a size of between 10-9 and 10-3 m, wherein the particles have been segregated by intermixing, wherein a textile base serves as a matrix;

and wherein the particles are bonded to a surface of said textile base, and the density of X-ray absorbing material as a whole, pm is within the range of 0.01 pP to 0.20pp, wherein X-ray absorbing properties of the X-ray absorbing material as a whole are equal to those of the filler; wherein pm is the density of X-ray absorbing material as a whole, and pp is the density of the material used for the particles of the X-ray absorbing filler.
In a second cmbodilnent of an X-ray absorbing material comprising a matrix with lived X-ray absorbing.,lnetal-containing filler in the forth of dispersed larlicles, the said tnatcrial lISCS aS a filler the segregated by intermixing poly-dispersed mixture containing metallic particles having a size of between 10-9 and 103 m, wherein the said metallic particles are surrounded by the volume of a matrix executed of at least one component solidifying under atmospllcric pressure or ol~ (I1C COIIIpOSltl011 011 the base of said colnponcnt. /~s this takes place 111c total mass of SCt,I'C~:ltctl p<lly-(IISpCI'CC(l mixllnw C'.()IISISIing of X-ray absurhing (rlrliclcs ul~
miller, is dc(ined by the relation:
M = (0,05 - 0,5) m, where M is the total mass of segregated poly-dispersed Illlxttll'e COIISISIIIIg of X-ray absorbing particles of miller, \Nhlle 111 IS the cduivalcnt IllasS Of the X-ray-absorbing filler material equal by its hrotcclive properties to 111e mass M.
According to another aspect of the present invention, there is provided an X-ray absorbing material comprising a matrix with a fixed X-ray absorbing metal-containing filler in the form of dispersed particles, wherein the filler is a poly-dispersed mixture containing metallic particles having a size of between 10-9 and 10-3 metres, wherein the particles have been segregated by intermixing, wherein the particles are surrounded by a volume of a matrix comprising at least one compound that solidifies under atmospheric pressure, and the total mass of the segregated poly-dispersed mixture consisting of particles of X-ray absorbing filler, M, is in the range of O.OSm to O.SOm, wherein M is the total mass of the segregated poly-disperse mixture consisting of the X-ray-absorbing filler particles, and m is the equivalent mass of the X-ray-absorbing filler material equal by its protective properties to the mass, M.

7a I» a third embodiment of an X-ray absorbing material comprising a matrix with fixed X-ray absorbing metal-containing !flier in the form of dispersed particles, the said »latcrial uses as a filler the segregated by intermixing poly-dispersed mi;cture, containing metal particles having a size of between 10-') up to 10~~ m, wherein the said particles arc bonded to an intermediate substrate which is surrounded by the volume ol~ matrix executed cll~ at Ic.ast one compound solidilyi»g under atmospheric pl'CSSLII-C OI- of the co»Ipositiu»
on .tlle base of said compound. A textile Vase serves as an intermediate substrate. A mineral fiber can be used .lS i111 IIltC1-IIICdIaIC SIIbStI-aIC.
According to a further aspect of the present invention, there is provided an X-ray absorbing material comprising a matrix with a fixed X-ray absorbing metal-containing filler in the form of dispersed particles, wherein the filler is a poly-dispersed mixture containing metallic particles having a size of between 10-9 and 10-3 m, wherein the particles have been segregated by intermixing, and wherein the particles are bonded to an intermediate substrate surrounded by a volume of a matrix comprising at least one compound that solidifies under atmospheric pressure.
~lllc attributes scl forth above relate to a range of inventions i»tcrc;u»»cctcd by tllc COI71»1011 atllllOr'S COIICCpl1011. As this takes place, the said range of inventions consists ul-ubjccts of one type and appliance, ensuring the same teclulical result.
»alllclv: exclusion ul~
tuxicability of an X-ray contrasting material and reduction of mass and width of a protective material which is the necessary requirement for an invention represented by variants.
Inventions re~liz~lion v:~ri~nls.
In a first c»lbudime»t of X-ray absorbing material lhc execution ul-a tiller in the lily»1 of segregated by intermixing poly-dispersed mixture comprising metallic:
partICICS having a size of between 10~y up to 10-3 m ensures the manifestation of a dualitativcly new cl~lecl by used X-ray absorbing filler - increasing of cut of interaction between the X-ray and gamma-ray emission and substance. Due to the mentioned effect the increasing oh specific properties ul~
X-ray absorption with the offered material is achieved.
~I-he use of poly-dispersed 1111X1111-CS a5 a filler is widely applied in X-ray absorbing materials described, fur example, in the IW ssia» federation patents N~~
2063~7~1 and Ne 2029399, whereof the non-segregated particles having a size of between 10-6 up to 10-3 m are used. However, in the said materials the above mentioned attribute is used in purpose of more regular distribution of X-ray absorbing filler along the surface of a matrix or inside thereof.
In the X-ray absorbing metal-containing material defined herein the segregated by intermixing poly-dispersed mixture ensures not only the more regular distribution of X-ray absorbing filler along the surface of a matrix or inside thereof but also provides for manifestation of a qualitatively new effect - increasing of cut of interaction between the X-ray and gamma-ray emission and substance.
The finely dispersible mixture of metal-containing element (sizes between 106 and 10~~
m) used in the known analogous material under the U.S.S.R. Certificate of Authorship N
1826173 is bonded to the textile base surface. Unlike the said analogous material, under the offered invention the poly-dispersed mixture made of particles having sizes of wide range: 10-9 up to 10-3, is used. As this takes place, the particles having sizes of the above mentioned range are included into the common mixture. Consequently, working on such mixture in common, natural conditions does not reveal any technological obstacles, i. e.
the said mixture does not demonstrate physical and chemical activity. In particular it does not manifest pyrophoric properties.
Under the offered invention the use of the segregated by intermixing poly-dispersed mixture comprising particles having sizes in the range of 109 up to 10-3 m provides for a qualitatively new effect, if compared with the said analogous material under the U.S.S.R.
Certificate of Authorship Ns 1826173. This effect consists in obtaining the same abnormal X-ray absorbing properties.
Side by side with this, the dispersed particles of the analogous material (acc. to the U.S.S.R. Certificate of Authorship Ns 1826173) are bonded to the thread surface, i.e. to the surface of a textile base. However, under the offered invention not only a thread but also separate filaments thereof can be used as a textile base, i. e. the notion «textile base» grasps a thread as well as separate filaments. According to the present invention in the case of separate filaments coating by an X-ray-absorbing filler (and, what is more, in the form of segregated by intermixing poly-dispersed mixture with self organization of poly-dispersed particles into the energetically interconnected power-consuming ensembles), and provided that the filaments would twist into a thread, the said thread shall have the specific X-ray absorbing properties of a qualitatively new, higher level, in comparison with the analogous material under the U.S.S.R. Certificate of Authorship Ns 1826173.
So, using a textile base as a matrix with the X-ray absorbing metal-containing segregated particles of filler being bonded to surface thereof ensures a qualitatively new effect (differing from the prototype) which finds expression in higher X-ray absorbing properties of material characterized by extremely heightened specific properties of X-ray absorption.
Under the U.S.S.R Certificate of Authorship Ns 1826173 an X-ray absorbing coating of the thread-matrix surface is provided. As for the X-ray absorbing material offered herein, a textile base not only in the form of thread as a whole can be used as a matrix; but also a textile base in the form of separate filaments which the thread consists of (as mentioned above). A
thread twisted out of separate filaments coated by an X-ray absorbing filler has much higher X-ray absorbing properties than a thread where only the open surface thereof is coated with an X-ray absorbing filler (unlike the offered material, where the surface of each filament included into the thread is coated by an X-ray absorbing filler). Moreover, the surface of each filament is covered by dispersed particles segregated by intermixing. As a result the said dispersed particles are self organised into the energetically interconnected X-ray absorbing ensembles, and this, in its turn, ensures the extreme heightening of X-ray absorbing specific characteristics.
Realization of an X-ray absorbing material as a whole, at same X-ray absorbing properties of this material and the filler material, wherein the density of filler is defined by the relation:
p n,= (0,01 - 0,20)pp, where p m is density of X-ray absorbing material as a whole, while pp is the density of the material used for the particles of the X-ray absorbing filler, creates a qualitatively new effect (if compared with the material of the prototype), namely the simultaneous reduction of width and density of a protective material.
The simultaneous reduction of width and density of a protective material woven, for example, of an X-ray absorbing thread, ensures overcoming of the main contradiction arising while creating effective compact protection against X- and gamma-radiation.
According to the offered invention, densities of the protective materials in the form of a thread and tissues derived therefrom, depending on the set technical conditions, can constitute between 0,01 (upper limit) and 0,2 (lower limit) of the X-ray absorbing filler particles material density. If the mass of X-ray absorbing material (in the present case, a protective tissue executed on the base of a thread, according to the invention) is taken for 1, then at protective properties and sizes of compared protective tissues being equal to those of the tissue on the basis of the offered thread, for conditions set forth in Table 1, the correlation by mass will be as defined in Table 2 below.
Table 2 Comparative correlation of tissues by masses at equal protection properties (with regard to the data set forth in 'Table 1 ) Relative limitsTissue made Tissue made Tissue made of of of of oscillation offered materialthreads with threads with of a a correlation filler in the filler in the form form between density of non-segregatedof non-segregated of tissue made particles of particles of of the Pb W

offered material and density of the material used for the particles of the X-ray absorbing filler Upper limit 1 198 267 (0,01 ) Lower limit 1 9,9 13,35 (0,2) So, the offered X-ray absorbing material (tissue) would have mass lesser in 9,9 up to 267 times (at the other physical and chemical parameters being equal), if compared with the protection tissues on the basis of threads with a filler in the form of non-segregated particles of Pb and W. The mentioned factor ensures a qualitatively new effect.
Consequently, if compared with the prototype, the offered X-ray absorbing material, demonstrating the absolute absence of toxicability, ensures high solidity equal to the solidity of the X-ray absorbing textile base plotted. Furthermore, it ensures the abnormally high X-ray absorbing properties at low density.
In a second embodiment of X-ray absorbing material the use of segregated by intermixing poly-dispersed mixture comprising metallic particles having a size of between 10-y up to 10-3 m (as set forth above) ensures the manifestation of a qualitatively new effect by the used X-ray absorbing filler - increasing of cut of interaction between the X-ray and gamma-ray emission and substance.
The poly-dispersed mixture containing metallic particles having a size of between 10-y up to 10-3 m, being placed inside a matrix volume, wherein the matrix is made of at least one component solidifying under atmospheric pressure or of a composition on the basis of said component, excluded is violation of energetic X-ray absorbing ensembles formed by intermixing and made of the X-ray absorbing element particles segregated poly-dispersed mixture. Meanwhile, this promotes the self organization of said energetic X-ray absorbing ensembles.
An inorganic glue, such as the Na silicate and K silicate water solute or water suspension of compositions containing oxides of alkaline metals and earth metals, as well as compositions on the base of such glue, can be used as a matrix.
The natural polymers, such as collagen, albumin, casein, gum, wood pitch, starch, dextrin, latex, natural caoutchouc, gutta-percha, zero, soy casein, as well as compositions on the base of such polymers, can also be used as a matrix.
The synthetic polymers, such as polyakrylates, polyamides, polyethylenes, polyethers, polyurethanes, synthetic rubber, phenolformaldehyde resins, carbomid resins, calibration epoxy and compositions based on such polymers, can be used as a matrix.
Element-organic polymers, such as silicon-organic polymers, boron-organic polymers, metal-organic polymers and compositions based on such polymers, can also be used as a matrix.
Plastics filled with gas, such as foam plastic and expanded plastic, can be used as a matrix.
Vegetable oils or drying oils can be used as a matrix.
Solutes of film-generating substances, such as oily, alkyd, ether-cellulose lacquers, can be used as a matrix.
Polymers water dispersions, such as emulsion colors, can be used as a matrix.
Concrete, gyps and so on can be used as a matrix.
According to the invention defined herein using the matrix made of solidifying compound, unlike the material-prototype under the Russian Federation patent N~ 2063074, takes place under atmospheric pressure, i.e. under natural conditions and not under pressure of 150 mPa like according to the prototype. According to the invention defined herein the mixture is not underwent pressure like the protection rubbers as described in the Russian Federation patents NsN~ 2077745, 2066491, 2069904 which are underwent vulcanization under pressure after preparation of the mixture. Consequently, it helps to avoid destroying of energetic X-ray absorbing ensembles formed in the course of intermixing of X-ray absorbing element particles segregated poly-dispersed mixture. The same distinction of the invention defined herein from the analogous material under the U.S.S.R. Certificate of Authorship N~ 834772 takes place, since according to the mentioned Certificate an X-ray absorbing material is obtained under pressure of 150-200 kg/cm2.
In an analogous material under the U.S. patent Ns 3194239 the pressed pills of previously crumbled up iron-manganese concretions (IMC) are used as an X-ray absorbing filler, which is different from the invention defined herein. Effect of pressure on the tiller of an analogous material under the Russian Federation patent Ns 2029399 also results in impossibility of energetical ensembles self organizing (however it takes place in the offered invention). Thus, application as a matrix of at least one compound solidifying under atmospheric pressure or of compositions on its base in the offered invention has essential differences from the material - prototype as defined in the Russian Federation patent Ns 2063074 7. and from the analogous materials under the Russian Federation patents NON
2029399, 2077745, 2066491, 2069904 in part of respective functional properties.
Realization of a condition, at which the common mass of the segregated poly-dispersed mixture consisting of the X-ray absorbing filler particles material is defined by the relation M = (0,05 - 0,5) m, where M is a the total mass of segregated poly-dispersed mixture consisting of X-ray absorbing particles of filler;
while m is equivalent mass of the X-ray absorbing filler material which is equal by its protective properties to the mass M, - will allow (according to the second variant of X-ray absorbing material) to reduce a mass of known X-ray absorbing fillers in protection materials in 2 up to 20 times, depending on particular technical conditions and at saving an X-ray and gamma-ray radiation reduction factor.
Reduction of mass and width of protection material can be regarded as the main objective while constructing protection from roentgen- and gamma-radiation.
However creation of the compact protection having a diminished thickness of layer leads to increase of a protective layer mass because of usage of the known heavy fillers. And, vice versa, saving of a roentgen - and the gamma - radiation reduction factor at lowering the density of a material entails necessity of increasing width of protection. And this is the main inconsistency arising while creating effective compact protection from roentgen - and gamma-radiation, as the simultaneous reduction of width and mass of X-ray absorbing material practically cannot be achieved with the known fillers applied 1-or protection. This inconsistency requires some compromise approach as to the choice of protection width and mass with allowance for a cost of such protection.
Let's illustrate this problem on an example of the most common material applied in purpose of protection against gamma-radiation, such as concrete. Density of different sorts of usual Portland concrete, containing cement as a connecting substance and the silicon shingle, gravel, quartz sand and similar mineral fillers, constitutes 2,0 - 2,4 g /
cm3. A linear gamma-radiation reduction factor constitutes 0,11 - 0,13 cm-~ (for energies of 1-2 MeV). The protection made of concrete having such density is quite cumbrous and should have considerable width. The concrete containing cement as a connecting substance, sand as a filler and galena as an X-ray absorbing filler in the ratio 1: 2: 4 has the density of 4,27 g/cm3, and the linear reduction factor thereof constitutes 0,26 cm-~ (for energies 1,25 MeV). The concrete containing cement as a connecting substance, sand as a filler and lead as an X-ray absorbing filler in the ratio 1: 2: 4 has density of 5,9 g/cm3, and the linear reduction factor thereof constitutes 0,38 cni ~ (for energies 1,25 MeV). 'the protection made of concrete with a filler in the form of lead (leaden fraction) or galena is more compact, but such protection is too much more expensive than usual concretes.
Such X-ray absorbing filler as the baryta BaS04 allows to solve a problem of choosing width and mass of protection with allowance for its cost. Though the appropriate solution can be found only on the palliative level. The barytes concrete containing as fillers sand and gravel, and the baryta as an X-ray absorbing filler, has density of 3,0 - 3,6 g/cm3, and the linear reduction factor thereof constitutes 0,15 - 0,17 cm-~ (for energies 1,25 MeV). However, the barytes concrete protection total mass for set gamma - quantums energy value remains considerable, which causes serious difficulties while creating protection, especially protection of transport facilities.
The above-stated inconsistency could be overcome, when the iron-manganese concretions are used as an X-ray-absorbing filler, for example, as defined in the patent of Russian Federation N~ 2029399. But even in this case it is impossible to reduce a total mass of a protective material more than by 20 - 45 %, if compared with the known materials.
However according to the offered invention the correlation of a total mass of segregated poly-dispersed mixture consisting of an X-ray absorbing material particles with the formula set forth above allows to reduce a mass of the included into protective materials known X-ray absorbing fillers in 2 up to 20 times, depending on particular technical conditions and at saving an X-ray and gamma-ray radiation reduction factor .

The technical outcome of the second variant of the invention is obtaining of an X-ray absorbing material with low percentage of a metal-containing X-ray absorbing filler. This effect provides for reduction of width and mass of an X-ray absorbing material as a whole without aggravation of X-ray absorbing properties.
In a third embodiment of an X-ray absorbing material the use of the segregated by intermixing poly-dispersed mixture comprising metallic particles having a size of between 10-9 up to 10-3 m, as a filler, (as was described above) provides for manifestation of qualitatively new effect of the used X-ray absorbing filler, namely, increasing cut of interaction between the X-ray and gamma-ray emission and substance.
The bonding of segregated poly-dispersed mixture consisting of the X-ray absorbing substrate particles to the intermediate substrate promotes obtaining an X-ray absorbing material with even distribution of the heavy X-ray absorbing metal-containing filler inside the matrix having considerably smaller density, than the material of filler.
Allocation of the poly-dispersed mixture comprising metallic particles having a size of between to-' and lo-' m inside the volume of matrix executed of at least one compound solidifying under atmospheric pressure or of the composition on the base of said compound, eliminates (as was described above) violation of the formed at intermixing energetic X-ray absorbing ensembles consisting of the X-ray absorbing element particles poly-dispersed mixture and also promotes self organizing of energetic X-ray absorbing ensembles.
A textile base and a mineral fiber can be used as an intermediate substrate under the third variant of invention.
The above description of X-ray absorbing material variants confirms the possibility of the invention realization, since the resources known on date of creation of the invention are used.
Besides, it is shown that the totality of tags describing an essence of the invention, is sufficient for solution of the set task.
Industrial applicability.
The above stated variants of the invention can be illustrated on the following examples.
Example 1. A filler in the form of segregated by intermixing poly-dispersed mixture made of tungsten particles, is bonded to the matrix surface executed in the form of a twisted lavsan thread. For this purpose a thread is to be put for a period of 10 minutes into the pseudo-liquefied (boiling) (under effect of heavy air stream) stratum of poly-dispersed mixture of the IS
following faction structure: 20 microns -1 S °/"; 45 microns - 8U %;
SUU microns - about 5 "/";
1000 IlllCl'OI7S - 0,01 %.
In these conditions segregation of particles happens due to said particles sell=organizing ilttu inlerdcpc;ltdeltt lower X-ray absorbing enscnlhles. Meanwhile such parliclcs .Ire allr,lclrcl to the thread, therefore they are "welded" on its surface. -fhe treated thus thread gains 1)1'Upel'tICS providing abnurntal rcducliun ohX-radiation.
Data of experiment:
Uiametcr of a thread - U,3 mm;
Length of a thread - 320U mm;
Weight of a thread bclitre plulling mechanical impurity (i-om tungsten - 0,1 10 g;
Weight of a thread after plotting mechanical impurity from tungsten - U, I 60 g;
Solidity of a thread before plotting mechanical impurity li-om tungsten - 47 l l, the s<Imc alter plotting mechanical impurity from tungsten - 47 11.
As this has taken place the mass density of ensembles of tungsten particles on the tltrcad surface hilS C(117Stlluted (),()()17 g/c1t12, size of the thread - U,22 cm3, and density tltereul-as a whole: p = 0.7 g/cm;.
~lf~ler treating the obtained sample of thread with the stream of cluantums with energy ctl' GO kcV and fixing of outcomes on a roentgen film, the densitumetry. in compariwm with tlm standard leaden plates of dil7ercnt vvidllt (stepped wcakcncr of 0.05 mm Pb up to 0.5 mm Pb with step 0,05 mm 1'b) lags been executed. In outcome it is asce:rtaincd that Iltc X-ray absorption of a thread is eduivalent to a leaden plate having width of U,l 111111 ur U,U75 ntm W
accordingly, that testifies about abnormally high X-ray absorbing properties ofa thread.
Ivrlhermorc, according to the formula of the invention p ,»_ (0,01 - 0,20)pl,, w~hcrc p ~» is dcnsily of X-ray absorbing ntatcrial (in our cast - a tlu-cad) as a whole.
while ph - density of X-ray absorbing f filler material (in our case; -tLlllgslell) ;
we have: p ~~~ / p ~= 0,7/19,3=U,U3G.
The obtained value of the ratio p ~" / p h keeps within the range (U,U1- U,2j according to thr formula of the invention.
example Z. The segregated poly-dispersed particles of tungsten having a size of between t0"
up to 10'3m are bonded to a matrix in the form of a textile material (the thick woolen cloth for overcoat) having width of 0,4 cm. Segregation and bonding of the tungsten particles to a textile matrix is realized by means of precipitation from hydrosol in conditions of continuous intermixing during the last I S minutes. 'then a sample is to be exsiccated at a room temperature within one day. The subsequent X-ray testing (at quantums energy of 60 keV) has shown that the X-ray protection properties of the obtained sample correspond to the same properties of a leaden slice having width 0,015 cm. This level of protection testifies about abnormally high reduction of X-ray emission stream, since the indicated level of protection at usage of usual non-segregated filler particles material requires bonding to a matrix of 100 of tungsten by mass (instead of 53 %, as in our case). Indeed, according to the invention and in connection with the considered example the mass of X-ray absorbing filler has constituted 0,116 g, i.e. 53 % of a total mass of a sample, wherein width of a sample made of textile material (the thick woolen cloth for overcoat) has been equal to 0,4 cm, the size of sample has been 1 x 1 cmz and mass thereof has been 0,216 g. As this has taken place, the density of X-ray absorbing material as a whole has constituted:
p m = 0,216 / I x 1 x0,4 = 0.54 g/cm3, and the mass of tungsten of non-segregated particles being equivalent by X-ray-absorbing properties constitutes:
0,015 x 0,75 x 19,3 = 0,217 g, i. e. 100 % of the mass of a textile material sample.
It is obvious therefrom that the relation p r" / p p = 0,54 / 19,3 = 0,0279 corresponds to a declared range.
Example 3. An X-ray absorbing filler in the form of the poly-dispersed particles of tungsten having a size of between 10-9 and ~ 0-3 m, amount = 12 % of mass, is introduced into a matrix in the form of hinge rubber of a brand < Ap - 24» having the following structure:
C - 84,73 %; 1-I
- 9,12 %; 5 -1,63 %; N - 0,58 %; Zn - 2,27 %; Oz - 1,69 % and a size - 100 cm3. Tungsten particles included into the structure of crude rubber are underwent segregation by intermixing in a mixer during 8 hours. As a result, the self organizing of particles into the system of power-consuming ensembles is achieved.
After that the crude rubber filled with the X-ray absorbing filler has been underwent vulcanization without effect of pressure. The subsequent X-ray testing (at energy of quantums - 60 keV) has shown that the X-ray protection properties of the obtained sample of rubber having width 3 mm correspond to the same properties of a leaden slice having width of 0,11 mm. This level of protection testifies about abnormally high reduction of X-ray emission stream, since the indicated level of protection at usage of non-segregated filler particles material requires adding to the matrix of 0,16 g of tungsten, i.e. 34 % by mass (instead of 12 %, as in our case).
Thus, for a considered example (width of a rubber sample -& = 0,3 cm; density -p =
1,56 g/cm3; a mass of rubber sample having a size 1 x 1 cm constitutes 0,468 g; the filler poly-dispersed particles material total mass, i.e. 12 % of rubber sample mass M=0,056 g) an equivalent mass of X-ray absorbing filler being equal by protective properties to the mass M, is equal m = 0,16 g (34 % of the rubber sample total mass).
It is obvious therefrom that the relation M/m = 0,056 / 0,16 = 0,35 corresponds to the range defined in the formula of invention (0,05 - 0,5), that diminishes the waste of filler, reduces a mass of a protection material as a whole and diminishes the production costs thereof.
Example 4. A filler in the form of super-thin basalt fiber TK-4, on which the segregated by intermixing (in a spherical porcelain attritor) poly-dispersed mixture made of tungsten particles having a size of between 10-9 and 10-' was fixed, is introduced inside a matrix in the form of epoxy priming of a brand «AP-0010» (Russian Federation Official Standard Ns 28379-89). A relation of a basalt fiber mass to a mass of tungsten constitutes 1:3. 1'he epoxy priming has been carefully intermixed by a palette-knife with a prepared basalt fiber, thus the relation of a mass of priming to a mass of a fiber has constituted 9:1. After intermixing and obtaining of a homogeneous mass the priming has been spread over a surface of cardboard plates as an even stratum and after solidifying within one day has been tested. 'the X-ray testing of samples (at energy of quantums - 60 keV) has shown that at a depth of priming layer equal to 2,06 mm, the protective properties thereof are equal to 0,08 null Pb, that testifies about abnormally high reduction of X-ray emission stream, since the indicated level of protection at usage of non-segregated weighing material particles requires adding to the epoxy matrix 38 % of tungsten by mass (instead of 7,5 %, as in our case).
In a considered example (& = 2,06 mm; p=1,46 g/cm3) the mass of an epoxy priming sample having the size 1 x 1 cm2 constitutes 0,3 g. The total mass of an intermediate substrate with the tungsten particles bonded to the said substrate, constitutes 0,03 g (10 % of a sample mass). As this takes place, the mass of tungsten makes up 3/4 of a mass of the filler, i.e.
0,0225 r, that constitutes 7,5 % of a mass of a sample as a whole.

Furthermore, the mass of tungsten, equal to lead having width of 0,08 mm, constitutes 0,008 x 0,75 x 19,3 = 0,1158 g, which corresponds to 38,6 % of a sample mass.
Example 5. 5 % of mass of the intermediate substrate in the form of crumbled staple fibers (by-products of fulling and worsted industry), to which the poly-dispersed particles of tungsten having a size of between 10-9 and 10-3 m segregated within 20 minutes by intensive intermixing in a pseudo-liquefied layer were bonded, are introduced inside a matrix of dry gypsum. The relation of a mass of staple fibers to a mass of tungsten constitutes 1:3. 1'he prepared thus mixture is carefully intermixed up to obtaining of homogeneous gypsum-filamentary mass. After that water is added, the mass is being carefully intermixed again and samples having sizes of 1 x 1 cm and width 1 cm are casted of the obtained liquid substance.
After drying and solidifying of the samples they are underwent testing (at energy oi~ quantums - 60 keV). The X-ray testing with the subsequent matching with the stepped leaden weakener has shown, that the obtained samples have the protective properties equal to those of a leaden plate having width of 0,04 cm. This level of protection testifies about abnormally high reduction of X-radiation, since the same level of protection can be reached at usage of non-segregated particles of the filler only at content of tungsten particles -26,32 % of the mass (instead of 3,75 %, as in our case). For a considered example (width of a gypsum sample -1 cm, density thereof - 1,32 g/cm3) the mass of a sample constitutes 1,32 g.
Thus the mass share of tungsten particles in a sample constitutes:
1,32 x 0,05 x 0,75 = 0,0495 g, i.e. 3,75 % of the total mass of a sample. At the same time the mass of a tungsten equal to the mass of a leaden plate having width 0,04 cm (by results of the X-ray testing) is equal to 0,04 x 0,75 x 19,3 = 0,347 g, that corresponds to 26,32 % of the sample mass.
The above stated examples of particular X-ray absorbing materials embodiment (variants) and the ways of obtaining thereof testify about the industrial applicability of said materials in the indicated area of engineering.

Claims

CLAIMS:

1. An X-ray absorbing material comprising a matrix with a fixed X-ray absorbing metal-containing filler in the form of dispersed particles, wherein the filler is a poly-dispersed mixture containing metallic particles having a size of between 10 -9 and 10 -3 m, wherein the particles have been segregated by intermixing, wherein a textile base serves as a matrix; and wherein the particles are bonded to a surface of said textile base, and the density of X-ray absorbing material as a whole, .rho.m is within the range of 0.01.rho. p to 0.20.rho. P, wherein X-ray absorbing properties of the X-ray absorbing material as a whole are equal to those of the filler;
wherein .rho. m is the density of X-ray absorbing material as a whole, and .rho. p is the density of the material used for the particles of the X-ray absorbing filler.

2. An X-ray absorbing material comprising a matrix with a fixed X-ray absorbing metal-containing filler in the form of dispersed particles, wherein the filler is a poly-dispersed mixture containing metallic particles having a size of between 10 -9 and 10 -3 metres, wherein the particles have been segregated by intermixing, wherein the particles are surrounded by a volume of a matrix comprising at least one compound that solidifies under atmospheric pressure, and the total mass of the segregated poly-dispersed mixture consisting of particles of X-ray absorbing filler, M, is in the range of 0.05m to 0.50m, wherein M is the total mass of the segregated poly-disperse mixture consisting of the X-ray-absorbing filler particles, and m is the equivalent mass of the X-ray-absorbing filler material equal by its protective properties to the mass, M.

3. An X-ray absorbing material comprising a matrix with a fixed X-ray absorbing metal-containing filler in the form of dispersed particles, wherein the filler is a poly-dispersed mixture containing metallic particles having a size of between 10 -9 and 10 -3 m, wherein the particles have been segregated by intermixing, and wherein the particles are bonded to an intermediate substrate surrounded by a volume of a matrix comprising at least one compound that solidifies under atmospheric pressure.

4. An X-ray absorbing material as defined in claim 3, wherein a textile base is used as the intermediate substrate.

5. An X-ray absorbing material as defined in claim 3, wherein a mineral fiber is used as the intermediate substrate.