high-temperature phases of zeolites of the … · anerican mi*eralogist vol. 57, pp. 499-510 (1972)...

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Anerican Mi*eralogist Vol. 57, pp. 499-510(1972) HIGH-TEMPERATURE PHASES OF ZEOLITES OF THE NATROLITE GROUP L. P. veN Renuwr.rx, Department o,fSoil Scian"ae, State Agri,aultwal Uruiuersitg , W agening,en, The Netherlands A-ssraAer The thermal changes occurring in zeolites of the natrolite group have been investigated by DTA, TGA, and continuous-heating X-ray photography. This combination of techniques facilitated a better description of the dehydration phenomena. Several as yet unknown metaphases have been recorded, and sta- bility ranges have been reassessed. Structurally, upon heating natrolite behaves entirely differently from its isotypes mesolite and scolecite which are mutually similar in behavior. Thomsonite and gonnardite also show similar X-ray diffrac- tion powder patterns, with aspects of both natrolite and mesolite,/scolecite. Edingtonite shows an individual pattern and is the only member of the group where heating does not result in a phase amorphous to X-rays (X-amorphous). The only feature common to all members of the group is that the room temperature phase reacts upon heating by a considerable contraction along the o and b axeg and a slight expansion along the c axis, in accordance with the general structure of tlre group. INrnooucrrom The thermal propertiesof few natural zeoliteshave been studied as extensiyely as those of the members of the natrolite group. This applies particularly to the species natrolite, mesolite,and scolecite and to a lesser extent thomsonite,whereas gonnardite and edingtonite have received very little attention. As has been pointedout in an earlier communication (van Reeuwijk, 1971),previousstudiescould not possibly give accurateinformation aboutthe physicalchanges zeolites undergo upon thermal dehydration, due to the employment of inadequate methodsand techniques. The purpose of this reporb is to give an account of the thermal be- havior of all membersof the natrolite group as obtained by a com- binationof dynamic thermal analysis methods, aiz.,d\ff.eren|ial thermal analysis(DTA) , thermogravimetric analysis(TGA), differential scan- ning calorimetry (DSC), and continuous heating X-ray diffraction techniques. Mernirrer,s A representative specimen of each species was selected from our collection under study to illustrate the characteristic properties. The Guinier De Wolfr X-ra5r photographs (Co-Ko radiation) are given in Figure 1, the chemical analy- sesin Table 1. 499

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Anerican Mi*eralogistVol. 57, pp. 499-510 (1972)

HIGH-TEMPERATURE PHASES OF ZEOLITES OF THENATROLITE GROUP

L. P. veN Renuwr.rx, Department o,f Soil Scian"ae, State Agri,aultwalUruiuersitg , W agening,en, The N etherlands

A-ssraAer

The thermal changes occurring in zeolites of the natrolite group have beeninvestigated by DTA, TGA, and continuous-heating X-ray photography. Thiscombination of techniques facilitated a better description of the dehydrationphenomena. Several as yet unknown metaphases have been recorded, and sta-bility ranges have been reassessed. Structurally, upon heating natrolite behavesentirely differently from its isotypes mesolite and scolecite which are mutuallysimilar in behavior. Thomsonite and gonnardite also show similar X-ray diffrac-tion powder patterns, with aspects of both natrolite and mesolite,/scolecite.Edingtonite shows an individual pattern and is the only member of the groupwhere heating does not result in a phase amorphous to X-rays (X-amorphous).

The only feature common to all members of the group is that the roomtemperature phase reacts upon heating by a considerable contraction along theo and b axeg and a slight expansion along the c axis, in accordance with thegeneral structure of tlre group.

INrnooucrrom

The thermal properties of few natural zeolites have been studiedas extensiyely as those of the members of the natrolite group. Thisapplies particularly to the species natrolite, mesolite, and scoleciteand to a lesser extent thomsonite, whereas gonnardite and edingtonitehave received very little attention.

As has been pointed out in an earlier communication (van Reeuwijk,1971), previous studies could not possibly give accurate informationabout the physical changes zeolites undergo upon thermal dehydration,due to the employment of inadequate methods and techniques.

The purpose of this reporb is to give an account of the thermal be-havior of all members of the natrolite group as obtained by a com-bination of dynamic thermal analysis methods, aiz., d\ff.eren|ial thermalanalysis (DTA) , thermogravimetric analysis (TGA), differential scan-ning calorimetry (DSC), and continuous heating X-ray diffractiontechniques.

Mernirrer,sA representative specimen of each species was selected from our collection

under study to illustrate the characteristic properties. The Guinier De WolfrX-ra5r photographs (Co-Ko radiation) are given in Figure 1, the chemical analy-ses in Table 1.

499

_ N

N

. ' - ' . - - YG

- j

- a

L. P, VAN REEUWIJI<

Frc. 1. Guinier X-ray photographs of zeolites of the natrolite group. A. natrolite,B. mesolite, C. scolecite, D. thomsonite, E. gonnardite, F. edingtonite.

500

HIGH TEMPERATUNE NATROLII'E

Table 1. CHEMICAL ANALYSES 0F I, ' INEMLS OF THE NATRoLITE GRoUP.

501

s i02 47 .06

A I 2 0 3 2 6 . 6 6

N a 2 0 1 5 . 3 6

C a o 0 . 2 7

BaO

H z O 9 , 7 6

4 6 . 2 1 4 5 , 9 7

2 6 , 4 2 2 5 , 6 9

5 . 0 8 0 , 2 6

1 0 . 4 0 1 4 . 2 1

1 3 . 3 4 1 4 . 4 4

3 8 . 6 2 4 2 , 8 3 3 5 , 1 +

3 1 , 0 + 2 8 , 7 9 2 0 " 1 2

) . 2 6 8 . 0 2

1 a o 1 ? q A

1 3 . 4 8 1 3 . 7 8 1 3 . 1 6

Tota l 99 .06 1 0 1 . 0 s 1 0 0 . 5 7 1 0 0 , 2 1 1 0 0 . 9 8 9 9 . 6 0

A . N a t r o l i t e , N . 1 s . 2 g C . o . i 5 A t t g . o g S i r u . o r O g o . 1 6 . 5 8 H 2 0 ( A u v e r g n e , F r a n c e )

B . M e s o l i t e , 3 ( N . 5 . o 9 a u 5 . r 6 A l j s . e o S i z g . g s o B o . 2 4 , 0 + H 2 O ) , ( O r " g o t , U . S . A . )

c . S c o l e c i t e , N " o , 2 6 C . 7 . g 6 4 1 l s . g , + S i z q . o g O g o ,

2 5 . 2 2 H r O , ( T e i g a n h o n n , I c e l a n d )

h r L ^ - ^ ^ - i + ^ r r ^ ^ . A 1 " ^ - ^ S i ^ ^ - ^ O ^ ^ . 2 3 . 9 9 H ^ 0 , ( K i t p a t n i c k , S c o t l a r dt . + v l . J l l v . 3 U l U . o Z o v

E. Gonnand i te , Na^ . -Ca^ . -A I . - - ^S i^^ , . ^O^^ . 24 .12 H^0, (Auvengne, Frobe)d . l a J . l f l l . l Y Z Z . + t 6 u z

I . Ed ins ton i te , l (n . r . r rRr . , u .osS iz3 . gzogo . 29 .74 H20) , (B6h le t , sweden)

Pnocnnunng

DTA, TGA, and DSC were performed according to the methods describedearlier (van Reeuwijk, 1971) with the only difference that in the present study aheating rate of l0'C/min. was used for DTA and TGA. Continuous heating X-raydiffraction patterns were recorded using a Guinier-Lenn6 camera with an averageheating rate of ca. 0.3"C/min. and a filmspeed of 2 mm/hr. Here, Cu-Ka radia-tion was used.

Rnsur,rs

The DTA and TGA curves are presented in Figure 2 and the resultsof the DSC in Table 2. The continuous heating X-ray diffractogramsare given in Figure 3.

Natrol;ite

The DTA and TGA traces of natrolite are the simplest of the group.Dehydration occurs, with an initial temperature of. ca. 24A"C, in asingle process in which all 16 molecules HzO are given off. Variationwithin the group of available samples was negligible. The heatingX-ray diffractogram (Fig. 3A) shows the corresponding transition tometanatrolite to take place at 280oC, again clearly illustrating thatpeak maxima in DTA curves (c/. Fig. 2A) cannot be used in deter-

5M L. P. VAN NEEUWIJK

l

IR{o@

o

Fre. 2. DTA and TGA curves of zeolites of the natrolite group. A. natrolite, B.mesolite, C. scolecite, D. thomsonite, E. gonnardite, F. edingtonite.

HIGH TEMPERATARE NATROLITE

T A R : i t A c : i < ^ f , e f r . l r a i i ^ r a l ; \ - F r i n p r - l c ^ i i h c n : i F . l i r p d , . , ! n

503

nurber o f A l i

rno lecu le st K c a r / m o l e i . r /

nunber of AH

: e o \ n , o L e c u f e s a L ^ - r / - ^ t o F ^ l

Natrof i te 35oo c

l ,{esof i te 2)5

3 8 0

4 1 0

' 1 2

,/

8'10

5

5

I

2

1 2

1 0

7

2 1 , 8

c . 4

1 8 . 0

Thonsonite 2ooo c

3 5 0

t + 2 5

Gonnardi te '15

2 2 0

4 5 0

424

2 7 4

4 5 0

mining actual reaction temperatures. However, for the sake of com-parison with previous work, peak maxima will be used to indicatereactions. Maxima for natrolites were found to occur at 35OoC whichis from 50 to 100'C lower than those usually reported by previousworkers (Koizuma, 1953; Peng, 1955; F6csi-Don6th, 1962). However,Sveshnikov and Kusnetzov (1946) are quoted by Peng to have foundmaxima at 350"C.

The photograph (Fig. 3A) reveals that a contraction along the oand b axes together with a slight expansion along the c axis precedesthe transition to metanatrolite. In eontrast to what was hitherto be-lieved, metanatrolite is shown to consist of two phases, the secondstarting at 510'C accompanied by a small endothermic peak in theDTA due to heat of transition alone since no dehydration is involved.Metanatrolite as a single phase was described by Hey (1932); how-ever, at this stage it cannot be decided to which of the two presentphases his description applies.

Rehydration is possible until the structure becomes X-amorphousat 785'C. Peng (1955) and P6csi-Don6,th (1962) reported collapseof structure at temperatures well over g00oO.

At 900'C c-carnegieite is formed. This phase appears to exist overonly a short temperature range as gradual transformation to nephelineis initiated already at 910'C and completed at 970oC.

According to the known phase relations the formation of nephelinefrom carnegieite by heating is an unusual sequence (Smith and Tuttle,1957; Levin et aI.,1969) .

504 L. P, VAN NEEUWIJK

d (A)1 0 6 5 4 s 2 5 2 1 8

d ( A l! 0 6 5 4 3 2 5

Frc. 3 Continuous heating X-ray photographs of zeolites of the natrolitegroup. A. natrolite, B, mesolite, C. scolecite, D. thomsonite, E. gonnardite,F. edingtonite. The continuous reflections from top to bottom of the photographsare due to the Pt sample grid.

2 1 8

20a

300

400

500

xl

20100

2@

300

400

500

600

700

800

900

r000

r100

20'100

200

300

400

500

600

700

1000

11m

!:

"; ".,

: " : ;

HIGH TEMPERATARE NATROLITE 505

From the reaction equation

NaruAlruSirro8'.16 HrO --+ l6NaA.lSiO4 + 8 SiO, + 16 HrOn e t r o l i t € n e p h e l i n e

appears that about 17 percent of the material at high temperaturesconsists of silica, however, up to 1150'C (maximum temperature ofthe camera) no crystalline silica phase can be detected.

The occurrence of albite as a heating product of natrolite (P6csi-Don6th, 1968) has not been observed in any of the samples.

Mesol;ite

The dehydration of mesolite occurs in two main steps, the flrst ofwhich is a double reaction with peak maxima in the DTA trace at255o and 275'C (Fig.2B). During this reaction 2 x 6 molecules ofHzO are lost (per 80 oxygens). The heating X-ray diffractogram (Fig.38) shows that the transition to metamesolite is initiated aI' ca.175"C and entails merely a contraction of the crystal lattice along thea. and b axes. The (111) and (511) reflections at 6.13 and 5.t12 A dis-appear above 200oC but reappear upon rehydration.

The second main step, when THzO are given off occurs over a shortertemperature range than the first and is in most cases a double reactionas well at 380' and 410'C in the DTA trace. However, the magnitudeof the second peak varies considerably from specimen to specimenand is usually much smaller than that of the first or may even beabsent. Peng (1955) reported the first doublet at 310'C and the secondpeak as a single one at 440"C. P6csi-Dondr,th (1962) analysed onlyone specim,en which gave a single peak at 300'C and a double oneat 4l}o and 440'C. The fiudings of Koizumi (1953) agree most closelywith those reported here.

The photograph (Fig. 38) shows that the metastructure is destroyedafter dehydration at 320oC, and from then on only some diffuse re-flections are discernable. Rehydration from beyond this transition isnot possible. This implies that, not all the water in this mineral isreversibly removable, the remaining water (if this is water as such)is gradually given off during further heating. The disappearance ofthe remaining reflections at 490'C is accompanied by a weak endo-thermic peak at 540'C in the DTA curve, which indicates a totalcollapse of the structure remnants.

At 910'C a high temperature feldspar phase is formed, which shows,when compared with a set of X-ray photographs of members of the

albite-anorthite series, close resemblance to bytownite (Ab26Anso) .

506 1.. P. VAN REEUWIJK

Not all available material can be incorporated in this phase andfrom 975'C onwards a nepheline phase can be observed as well.

If all Na and Ca is incorporated in AbzoAneo and nepheline, thensilica is left over as in the case of natrolite:

Nas. 3Car. sAlr6 Sirnoso. 24 H2O --+ 2.3 Nao. rCar. 3Alr Siror4m o s o l i t e

Again'no crystalline form

Scaleeite' The dehydration of scolecite is very similar to that of mesolite andalso occurs in two main steps. The fir,st reaction, initiated aL ca.160'C shows a single but non-symmetrical DTA peak with a maximumat250"C (F ig .2C) .

During this reaction SHzO are removed. The second dehydrationstep, when another 10H2O are lost, is in some cases a double reactionwith peak maxima at 430' and 450'C followed by a smaller separatepeak at 480'C whereas other specimens may show a real triple peakat, 430o, 450", and 470"C as shown in Figure 2C. This, however, isneither reflected in the TGA trace nor in the heating X-ray diffracto-gram (Fig. 3C).

This photograph shows that after the second dehydration stepreflections of metascolesite continue, but they are much weaker andslightly shifted. Rehydration of this phase is not possible. As withmesolite, the remainder of the water is lost gradually upon furtherheating. At 490"C the material becomes X-arnorphous correspondingwith an endothermic DTA peak at 560'C. At 950'C high temperatureanorthite is formed without any apparent accompanying phase, al-though according to the stoichiometry again silica is left over:

CaeAlroSLaOso.24H,O ---+8Ca,ALSrrOs * 8 SiO, + 24H.,Or o o l e o i t o a n o r t b i t €

, In addition to differences in temperatures of reaction, a diagnosticdifference between mesolite and scolecite is the course of both theDTA and TGA curves between the two main dehydration steps. Formesolite this part is sloping, whereas for scolecite it is virtuallyhorizontal.

ThomsoruiteThe dehydration of thomsonite appears to be somewhat more com-

plex. During the first rather long range of dehydratioir initiated at

o a . A b r o A n e o

+ 4.6 NaAlSiO4 + 3.2 SiO, + 24I .,Oucphe I iuo

of silica could be detected, however.

HIGH TEMPEBATURE NATROLITE 547

ce. 100oC and having a DTA maximum at 200"C (Fig. 2D) 8HzOare lost accompanied by a slight but definite contraction of the latticemainly along the o-axis and a still smaller expansion along the c-axis(F ig .3D) .

The next step is a double reaction with a small peak at 325"C anda large one at 350"C in the DTA trace during which another SHzOare removed and a distinct crystallographic metaphase is formed(Fig. 3D, at 290"C).

Upon further heating, yet another metaphase is formed aL 325"Caccompanied by a double endothermic DTA peak with maxima at400o and 440"C, respectively, and during which the base line shiftsto a higher level culminating in a small exothermic peak at 450"C.This corresponds with a temperature of 390'C on the heating X-raydiffractogram where a transition to a phase with very weak reflec-tions occurs. Rehydration of this phase is not possible' Collapse ofthe structure is indicated by the endothermic peak at 520'C in Figure2D. Milligan and Weiser (1937) and Koizumi (1953) reported nocrystallographic changes during dehydration of thomsonite, however,they analyzed their samples after cooling in air.

Just below 900'C a bytownite/anorbhite phase is formed (about

AbroAngo) followed by nepheline at 910'C.

Ganmard,ite

No detailed study of the structure of gonnardite has been, made,but it is believed to be similar to that of thomsonite (Smith, 1963).This relation is expressed by the thermal behavior. The most imporbantdifference is the occurrence of an early dehydration step below 100"C(Fig. 2E) when 5HzO are given off' This water loss induces a markedcontraction of the lattice along the a and b axes as shown by Figure3E. This shift, resulting in a merging of reflections' occurs just aboveroom temperature and could only be shown clearly when the heatingwas started somewhat later than the film transport. The subsequentdehydration steps, where 5, 9, and 2 molecules HzO are lost', respee-tively, are very similar to those of thomsonite except that doublepeaks in the DTA curve of the latter appear to be single ones here'

During heating of the first metaphase, up to 300oC, contraction ofthe lattice along the o and b axes continues together with a slightelongation along the c axis. At 30O'C there is a transition to a nextmetaphase (Fig. 3E) accompanied by a sharp endothermic peak at350"C in the DTA curve (Fig. 2E). Ttis phase disappears at 36OoCon the photograph; from then on some weak reflections continue toabout 500oC. No rehydration is possible beyond the 360"C trans-

508 L, P. VAN REET]WIJK

formation. The occurrence of the weak endothermic peak at 460'C(Fig.2E) indicates final collapse of the structure.

The subsequent high temperature phases are the same as thosefor thomsonite.

Ed;ingtonite

A DTA curve of the Biihlet edingtonite has been reported byP6csi-Don6th (1962) and differs from ours only in temperaturemeasurement. It shows two rather broad and one sharper endothermicpeaks at aa.170",280o, and 465o, respectively (Fig. 2F). The cor-responding steps in the dehydration curve indicate water losses of12, 10, and 7 molecules, respectively. The TGA curve indicates thatno more water is available so tha;t edingtonite contains 29 H2O per80 oxygen atoms. Hey (1934) reports that edingtonite contains 32H2O per 8O oxygen atoms on grounds that air-dry material takes upmore water on raising the water vapor pressure. As this feature is byno means restricted to this mineral, the argument does not apply.For this reason our powdered zeolites are stored and manipulated atthe arbitrary but constant relative humidity of 51 percent at 2b'C(Barrer and Langley, 1958).

Margaret Foster (1965) concludes from Koizumi's (1gSB) andPeng's (1955) dehydration curves that HzO that is an intrinsic partof the structure does not begin to come off below lb0oO and, there-fore, she recommends that HzO- be routinely determined in zeolitesat 110'C. Our experimenLs also indicate adsorption of H2O otherthan that incorporated in the structure, but a general rule that HzOcoming off below 150'C is not such incorporated water is incorrect,as is illustrated by gonnardite and edingtonite (Fig. BE, F).

As with the other members of the group, dehydration of edingtoniteeffects a lattice contraction along the a and, b axes together with anexpansion along the c axis (Fig. BF) resulting in a merging of a num-ber of reflections. These shifts are completely reversible.

After the final dehydration reaction the DTA curve shows a rela-tively strong exothermic peak at 500"c, not due to lattice desintegra-tion as suggested by P6csi-Don6,th (1962), but to the irreversibletransformation to celsian and an unidentified phase with the follow-ing reflections: (d in A, at room temperature) 5.60 (w) ,4.74 (vs),4 .48 (s ) ,4 .22 (vs ) ,3 .b8 (w) ,8 .5b (w) ,2 .68 (s ) ,2 .80 (w) .Remarkab leis the small weight increase accompanying this reaction (Fig. 2F).When a TGA was carried out in a dry N2 stream, transformation tocelsian did not occur at the end of dehydration and no weight increase

HIGH TEMPERATT]RE NATROLITE 509

was observed. Experiments to establish whether water or possibly

oxygen is involved failed so far.At 925"C celsian is transformed to hexacelsian with the simultane-

ous disappearance of the unidentified phase. The transformation of

edingtonite to hexacelsian is represented by the following equation:

BarAl,sSir0s'.2g H,O --+ 8 BaALSi,O, * 8 SiO, + 29 H,Oed iDgton i t6 hexeoe l s i o l

hence again silica is left over. Unlike the reactions shown by othermembers of the group, this silica crystallizes as p-cristobalile at' aa'1050'C, indicated by some weak reflections on the original heatingX-ray diffractograrn (Fig. 3F). The co-existence of hexacelsian and

B-cristobalite at such a relatively low temperature is not representedin the BaAlzSizOe-SiOz phase diagram of Foster and Lin (1969).

Concr,usroNs

Upon dehydration, all members of the natrolite group react by a

contraction of the lattice along the o and b axes and often an expan-sion along the c axis. This is fully in accordance with the general

structure of these minerals which consists of parallel chains of (Al,

si)o+ tetrahedra in the a direction, less prominently linked together in

r and y directions.Although natrolite, mesolite, and scolecite are isotypes, the struc-

tural behavior of natrolite appears to deviate significantly from that

of mesolite and scolecite which show a good mutual resemblance.Thomsonite and gonnardite, supposedly isotypes too, are very similarin thermal behavior and show, moreover, properties of both natrolite(350'C endothermic peak, more than one prominent metaphase) arid

mesolite/scolecite (ca.. 200o and 400'C endothermic peaks, not all

the water reversibly removable) .Apart from thermal expansion of the crystal lattice, the structural

relationship of edingtonite with the group is not expressed by its

thermal behavior. unlike the behavior of the other members, after

dehydration further heating produces an irreversible crystallographictransformation without going through an apparent X-amorphousphase.

AcrNowloncnrvruwrs

The writer is indebted to the following persons and institutes who kindly

donated mineral specimens used in this study: Dr. Kazuo llarada, Tokyo, Japan;

Dr. Henno Nairis, Stockholm, Sweden; Dr. E. M. Taylor, Corvallis, Oregon,

U.S.A.; National Museum of Geology and Mineralogy at Leiden; and the

Geological Institute, University of Utrecht, The Netherlands.

510 L. P. VAN NEEUWIJK

Thanks are a,lso due to Dr. L. van der Plas for helpful discussions and forcritically reading the manuscript. Mr. R. Houghton corrected the English text.

RnrpnnNcns

Bannnn, R. M., eNo D. A. Lerrrcr,nv (1g58) Reactions and stability of chabazite-Iike phasm. Part I. Ion-exchanged forms of natural chabaaite. J. Chem. Soc.( Lond,on) 19s8, B804-B82S.

Fostnn, Mmcendr D. (1965) Studies of the zeolites. U.8. Geol. Swru. Prof. Pap.504-D.E.

Fosren, W. R.,.ewo IL C. LrN (1969) Studies in the system BaO-Al,O".SiO, II.The binary system celsian (BeALsi,Os)+ilica (SiO,). Amcr. J. Sci,. 267-A,LU-|M.

Hpv, M. I{. (1932) Studies on the zeolites. Part IIL Natrolite and metanatrolite.M ineral. XI ag. 23, 2+3-289.

- (1934) Studies on the zeolites. Part VL Edingtonite. Mi,neral. Ma4. 23,4W494.

Korzuntr, M. (1953) The differential thermal analysis curves and dehydrationcurves of zeolites. Mineral J . ( TokAo ) t, 3647 .

Lnvrrrr, E. M., C. R. RonarNs, AND I[. F. McMururn (lg6g) Phase Di,ogra:ms forCeramists, The American Ceramic Society, p. 181-184.

Mrlr,rcerv, W O., ewo H. B. Wnrsnn (lg37) The mechanism of dehydration ofzeolites. J. Phgs. Chem. 4!,1029-1040.

Pr6csr-DoN.{rs, E. (1962) Investigation of the thermal decomposition of zeolitesby the DTA method. Acta Geol.6,429442.

- (1968) Some contributions to the knowledge of zeolites. Acta Mi,neral.P e tro gr. XVIII, 127 -141.

PnNc, C. J. (1955) Thermal analysis study of the natrolite grotp. Arner. Mi,ner.40,834-856.

Srrrru, J. V. (1963) Structural classification of zeolites. Mineral. Soc. Amer.,Spec. Pap.1, 281-290.

ewo O. F. Tumr,p (1952) The nepheline-kalsilite system. I. X_ray datafor the crystalline phases. Amer, J, Sci. zSS, 282-808.

Yar.r Rnouwr.rK, L. P. (197f ) The dehydration of gismondite. Amer. Miner, 56,1655-1659.

Manuscri,pt receiued,, August 30, 1g/1; accepted lor publicatinn, Nouember pp,Im1.