American Mineralogist, Volume 72, pages 617-624, 1987 optics:Responseto (OH-) orientationand Amblygonite-montebrasite rapid estimationof F fram 2V DlNrnr- J. GnorNnnr* F. DoNll,o Br,oss Department of Geological Sciences,Virginia Polytechnic Institute and State University, Blacksburg,Virginia 24061, U.S.A. Assrnlcr For I I crystalsof the amblygonite-montebrasiteseries,LiAIPO.(F,OH), ranging in composition from 4.0 to 91.8 mol0/oF (and only 2 containing significant Na), 2Zand principal refractive indices were determined to 0.5oand 0.0005, respectively,by spindle-stagemethods. If the F content is <60 molo/oand therefore 2l/. < | l6o, as is true for the vast majority of natural specimens,the F content can usually be estimated to within 2 molo/ofrom evaluatingtFl: -66.3 + 1.08 x 2V, as well as from similar reglessionequationsinvolving the refractive indices a, B, and 7. Above 60 molo/oF, the optical properties are less sensitively (and nonlinearly) related to F content. Estimates of F content are feasible despite significant substitution of Na for Li. By contrast, this substitution may introduce significant errors when estimating F content by methods involving lattice parameters. Progressivesubstitution of (OH), a natural dipole involving a covalent bond, for the relatively nonpolarizable F anion causesall three principal refractive indices to increase; ,y increasesmore than a or B becauseits corresponding principal vibration ditection Z becomessubparallel to the O-H vector in the structure as (OH) content increases. INrnorucrroNi For the amblygonite-montebrasite solid-solution series, "(Li,NaCa)vI(Al,Fe,Mg)'uPOo(F,OH), the elements in boldface representthe primary constituents. Thus, in the common representativesof this series,less than 100/o of the five-coordinatedLi sitescontain Na andlor Ca and less than 0.lolo of the six-coordinated Al sites contain Fe and/or Mg. Thus these specimensrepresent essentially binary solid solutions betweenthe end members,amblygonite (amb), LiAIPO4F, and montebrasite (mtb), LiAlPO4(OH).Natural membersof the seriesrangefrom ambo to ambrr, but specimensmore F-rich than ambu,are rare. Members of the amblygonite-montebrasite series are triclinic and biaxial. If negative in sign, they are called amblygonites,and if positive, montebrasites.Phillips and Griffen (1981) indicated that the optic sign changesfrom (+) to (-) at amb-rr, but presentevidence,as will be demonstrated, places the change closer to amb.o. The structural similarity betweenamblygonite and titanite becomes apparent when a nearly monoclinic cell is chosen as suggested by Simonov and Belov (1958) and as employed recently by Hawthorne (pers. comm.) during refinements of amblygonite-montebrasitestructures. The dependenceofthe physical properties ofthe series on the dominant F-(OH) substitution has been studied by many investigators. The usual goal has been to find one or more physical properties to serve as reliable estimators of the F content. In such event, particularly if the * Present HerculesInc.,Bacchus Works,Magna,Utah address: 84044,U.S.A. 17$02.00 0003-004x/87/0506-06 physical property were quickly and preciselymeasurable, monitoring the F contents in members of the amblygonite-montebrasite seriescould permit recognition of the F-(OH) zoning in pegmatites, where these minerals exclusively occur. Although initiated by Bragg (1924), studies relating a crystal's optical properties to its composition and structure are infrequent in mineralogy, often due to the imprecision of available data. Thus, prior to the development of microprobe and spindle-stage techniques, a chemical analysisof a l- or 2-g sample of a biaxial mineral-itself renderedsuspectbecauseof the possiblepresenceof impurities in the sample-was often coupled with a refractive index a measured from one grain, B from another, and 7 from still a third. Moreover, the precision of their measurement,usually +0.002 or +0.003, was insufficient and frequently overly optimistic. Now, however, from one and the same grain it is possible to measure all indices to +0.0005 by spindle stage,transfer the goniometer head containing the grain to an X-ray camera for such X-ray studies as desired, and, ultimately, determine this same grain's composition by microprobe analys1s. Tight relations among optics, composition, and structure can thus be establishedand have led to an increasing numberof recentstudies(Selkreggand Bloss,1980;Armbruster and Bloss, 1982; Su et al., 1984; Mereiter and Preisinger,1986;Lager, 1986;to cite only a few). Combined X-ray, spindle-stage,and microprobe studiesof the membersof a solid-solution serieshave beenof particular interest. With the substitution of one atomic speciesfor 617 618 GREINER AND BLOSS: AMBLYGONITE-MONTEBRASITE TABLE1. Sampledescriptionsand pegmatitelocalities Samplenos. Descriptionand locality Bluish water-clearcrystals from pegmatite vugs with quartz and cleavelandite; F contentnot determined(Plumbago,Newry, Maine) AF-43-2 117775- Grayish-whitecleavagefragment(Gunnison Co., Colorado) e A-22" Brownishtranslucent,massive 4 A-98.Paleyellowtranslucentmass 5. Pale pink core of a zoned crystal (see A-2), slightlycontaminatedby secondarymontebrasite(-5%) 6. AF-46 1 0 5 9 1 4 ' Palebluishcleavagefragments(Karibib, South Africa) 7. AF-55 62576- Colorlesscleavablemass (Hebron,Maine) 8 AF-65 142741 Translucentfragmentswith faint bluishtint (Chursdorf,Saxony) 9. A-2+ Yellow outer rim of a zoned crystal (see A-1) 1 0 A-C+ Yellowtranslucent,veinedby A-4. 1 1 AF-50 10432', Pale brown transparent mass (Coolgardie, Western Australia) 1. AF-47 Note: Modifiedfrom Cerndet al. (1973).All crystals removedfrom these samplesand studiedopticallywere clear,containedtew inclusions,and showed no evidenceof zoning. Crystals for AF-43,A-22, AF-50, and AF65 each containeda few lamellaeof a polysynthetictwin component The crystal studied optically tor sample AF-43 is the same crystal for which Hawthorne(pers.comm.)performeda structureanalysis. . U S. NationalMuseumsamDlenumber t BritishMuseumof NaturalHistorysamplenumber. { Samplenumberof specimensfrom the Tanco pegmatite,BernicLake, Manitoba,Cern6et al. (1973). another in a solid-solution series,the optical properties often change, because the substitution may involve changesin atomic number and electronic shell structure, polarizability, ionic radius, valence, electronegativity, charge transfer, disposition and distances of nearest neighborsaround the site ofthe substituent, and/or even the proportion ofone bond type relative to another. The amblygonite-montebrasiteseries was thus of interest,becauseit involved the replacementof a relatively nonpolarizable anion, F , by a natural dipole, (OH)-, containing an appreciably covalent bond that tended to be directionally oriented in the structure. OPTICS of these crystals showed Mg and Fe to be below detectable limits and Ca to be below 0.1 molo/0.Na was below detectablelimits for all samplesexcept numbers 7 and 8, in which it exceeded2 wto/o.Al and P were nearly constant. This suggestedthat the eight crystals contained no significant substitutions other than F for (OH). Attempts to determine F content by calculation from microprobe analyseswere unsuccessful.An initial spindle-stagestudy of several different crystals from each specimen yielded 2V values,as calculatedby nxcelrnn (Bloss,l98l), that differed by two degreesat most except for one sample in which they differed by four degrees.Thus, it seemedvalid to assume that crystals from a given specimen differed little in optical properties and composition from each other. Accordingly, the F compositions (neutron activation) and (OH) compositions (gravimetric analysis) obtained by Cern6 et al. (Table 2, 1973) were acceptedas valid for thesecrystals.For sample8, Moss et al. (1969) determined F from its distillate using the zirconium-Eriochrome-cyaninemethod of Megregian(1954).No complementary (OH) analysishas been performed on sample 8. In this paper the F content will be expressedas mole percent F [F]-that is, as 100 times the atomic frequency of F in the formula unit. [F] and [OH] (mole percent hydroxyl) were calculatedby Cern6 et al. (1973) from the weight percentagesthey obtained for F and HrO. The values for [fl and [OH] were adjusted for the presenceof minor Na, Ca, K, Mg, and Fe. Complete chemical analysis of sample 8 has not been performed. Accordingly, for sample 8, [fl was calculatedfrom the equation lFl : 7.7845 x wto/oF. This equation correctly relates mole percent to weight percent F for samples wherein only the F-(OH) substitution occurs. Such a condition is not strictly valid for sample 8, sinceit contains significant (>2 wto/o)Na. Still, any errors introduced by falsely assuminga lack of substitutions other than F for (OH) for these sampleswill be very small. The equation w t o /Fo : 0 . 1 2 9 4 6 x [ F ] will convert these values to weight percent F for all amblygonites and montebrasitesin which substitutions exThe experimental methodsusedhavebeendescribed fully by cept (OH) for F can be consideredminimal. Table 2 sumGreiner(1986).In summary,opticalconstants weredetermined marizes the content of [fl and [OH] in the specimens for eachcrystal(Tablel) by spindle-stage methods.Estimated from which the crystals studied were drawn. precisions are2V (+0.5), refractive indices(+0.0005),andlocation of the principalvibration axesX Y, and Z (+0.5" or VlnHrroNs oF oprIcAL pRopERTIESwITH better).Transferofthe goniometer headfrom theSupperspindle MOLE PERCENT F stageto an X-ray precession camerapermitteddetermination of work Previous the angularattitudeofthe triclinic axes(Palache,1943)relative to X. Y. and Z. Researchon the optical properties of the amblygonitemontebrasite series is limited. Winchell and Winchell CrrsN{rsrnv (1951) plotted refractive index and the optic axial angle The amblygonite-montebrasitecrystalsexamined were 2 Z versus (OH) content, using data from the literature, from the same specimensstudied by Cern6 et al. (1973), but the data points were widely scattered.Dubois et al. ranging from translucent to gem quality and relatively (1972) performed least-squaresregressionson 2 Zand rehomogeneous in composition throughout each single fractive-index data measuredfor samplesin the ambo to specimen (P. Cernj', pers. comm.). Microprobe analyses ambrorange.Thedata show considerablescatterabout the ExpnnrnrnNTAr- METHoDS GREINER AND BLOSS: AMBLYGONITE-MONTEBRASITE Taele 2. F and OH contents lFl Sample (mol%) I e 4 o 7 9 10 '11 toHl tFl + toHl (mol%) (mol%) 4.0' 10.8 144 26 5 42.7 55.3 79 2 91I 27.9 34 8 96 5 85.3 834 70.2 54.8 47.0 25.0 96.1 97.8 96.7 97.5 102 3 104.2 J4 3 3J.J 65.9 53.6 93.8 88.4 108.0 tFl. HrO+* (wt%) HrO * (wt%) 0.30 1.40 1.88 3.44 5 56 7 .24 10.17 11.80 3 65 4.51 7.07 5.98 5.25 5.11 4.43 3.39 2.92 1.53 0.10 0.07 0.06 0.05 0.10 0.05 0.09 4.09 3.30 3.29 0.04 0.08 0.23 (wt%) - Calculatedvalue; see Cerndet al. (1973). trends, and theseregressionsindicated, for the most part, lower 2V and refractive-index values than those predicted by Winchell and Winchell's graphs over the same compositional range. Cern6 et al. (1973) measured the index 7' for crystalslying on the { 100} cleavageand found that it exceededthose that Winchell and Winchell had reported for .y. This underscored the need for a more accurateset ofoptical data for the series.The application of spindle-stagetechniques to the chemically well-characteized specimensassembledby Cern6 et al. (Table l) thus seemedin order. Optic orientation Burri (1956) introducedthe use ofEuler anglesto express quantitatively the optic orientation of the optical indicatrix's principal vibration axes(X, Y, and Z) relative to the crystallographic axes of a triclinic crystal. In essence,he related the intrinsically orthogonal set of axes (X, Y, and Q Io a second orthogonal set obtained by choosing(l) a reciprocal crystallographicaxis; (2) one of the two direct crystallographic axes perpendicular to it; and (3) a third axis that is perpendicular to both (l) and (2). The cleavageplanes for the amblygonite-montebrasite seriesmade it expedient to select from the crystallographic axes chosen by Palache et al. (1943) the orthogonalset (l) a*; (2) c; and (3) B, whereB symbolizes a direction perpendicular to both a* and c. Euler angles for Na light (Table 3) were calculated (Greiner, 1986) such that if the correspondingrotations were performed, 6t9 OPTICS X would coincide with B, I with a*, and Z with c (Fig. l). For the six crystalsfor which the optic orientation had beendetermined relative to the crystallographicaxeschosen by Palache et al. (1943), optic orientation changed systematicallyas [Fl varied from 4 to 92 (Fig. l). Note that with increasing[fl, the two optic axes(OA, and OA,) move away from Z and approachX so that the optic sign changesfrom (+) to (-). For [F] :79 and 92, however, note that OA, and OA, no longer move directly toward X but turn slightly away. Thus, 2V* ceasesto decrease (and 2V, to increase)as rapidly with increasedF when [F] exceeds-60. With increasedF, one optic axis (OA,) changesrelatively little in position, whereasOA, changes markedly. The situation is reminiscent of another triclinic solid-solution series,the plagioclases(Reinhard, l93l), in which one optic axis changesmarkedly in position as Ca content changes,whereas the other does not (Bloss, l 978). Refractive indices and 2V Principal refractive indices (a, B, and 7) and values of 2V, calcl.:Jated by excer-rnn for Na light (Table 3) were determinedfor specimensI to 11. Exceptfor samplesI and 8, an F analysis and an independent (OH) analysis had been reported for each (Cern6 et al., 1973).These F and (OH) analyseswere consistent for specimens2 to 7 in that [F] + [OH] = 100. For specimens9, 10, and ll, however, the sum deviated by more that 5o/ofrom l000/0. Accordingly, the data for specimens9, 10, and ll were omitted from the calculationswhen regressionswere performed. The following models relating optical parameters to [fl (: mole percentF), and indeed all subsequentones, were derived by a combined use of the srepwrse and (Cp option) proceduresof the SASInstitute (Ray, RSeUARE l 982). R2 a: 1.617 55(78)- 5.3r(27)x 10 alFl + l l4(33)x l0-'o[r]4 0;996 (1) p : r . 6 2 57 0 ( l l ) - 3 . 0 7 ( l l )x l 0 o l F l + 3.98(29)x l0 6[F]'z + 3.60(22)x l0-8[F]3 0.999 (2) TneLe3. Refractiveindices,2V, and EuleranglesO, O, and V as observedfor Na light Sample IF] 1 4.0' 10.8 14.4 26 5 42.7 55.3 79.2 91.8 27.9 34.8 54.5 2 4 o 7 I I 10 11 dT 1.61476 1. 6 1 08 8 1.61043 1.60536 1.59530 1.58856 1.57923 1 . 5 7 72 3 1.60052 1 59532 1 59123 PI 1 62440 1 . 6 2 19 0 1.62067 1.61533 1. 6 0 81 6 1.60263 1. 5 9 4 1 7 1.59180 1.61283 1. 6 0 84 0 1. 6 0 53 6 tt 1.64589 1.64026 163800 1 62963 1 . 6 1 78 4 1.60913 1 . 5 9 74 9 1.59560 1.62488 1. 6 1 75 3 1.61273 2V.f 66.27 82.4 71.63 72.82 85.15 86.3 100.76 92.0 112.57 100.5 125.98 43.0 129.47 55.5 92.87 99.31 106.98 f c, B, and 7 shouldbe roundedto the 4th and zvzto the 1st decimalplace. " Calculatedvalue,see Cern6et al. (1973). -26.0 77.8 -23.9 -20.8 - 14.3 14.7 18.2 76.4 77.8 8 1. 0 18.0 30.0 GREINER AND BLOSS: AMBLYGONITE-MONTEBRASITE 620 OPTICS .= bt" ,P bp oAz B Or 45 oxa F o4 9? lzg 26 43 55 79 92 OH^Z 2t.6 17.3 t5.5 t7.9 40.9 45.8 Fig. l. Stereographicdepiction of the variation in orientation of the two optic axes (OA, and OAr) and the three principal vibration axes(X, Y, and Z\ relative to c and a* as mole percent F varies in the amblygonite-montebrasiteseries.The dots represent data for the six crystals whose optic orientations were determined empirically; the numbers adjacent to the dots representmole percent F for these crystals.The subscript p indicates crystal axes chosenby Palacheet al. (1943); the subscript m and the small squaresdesignatethe almost monoclinic axes employed by Hawhorne (pers. comm.). The triangle representsthe O-H bond direction as determined by Hawthorne. The inset representsthe anglebetween Z and the O-H vector for the six crystalswhose [Fl values are listed. The Palacheaxesa* and c were chosenbecausethey are defined by the perfect {100} cleavageand the good {l 10} cleavage.Thus, a* is normal to the perfect cleavageand c representsthe trace ofthe good cleavageon this perfect cleavage. 7: zvz: 1 . 6 4 8 8 4 ( 3 1- ) 7 . 5 0 ( 1 1x) l 0 - ' [ F ] + 2 . 1 7 ( 1 6 )x l O - ' o [ l 4 0.999 (3) 60.86(95)+ 0.96(3)[fl 0.998 (4) + 2.73(40)x l0-'[F]o Thesemodels and the data from which they were derived, along with the data for specimens9, 10, and I l, are plotted in Figure 2. The dashedcurve (22.') represents2Zz as calculated from the refractive-index curyes below it. Note that it closely conforms to the solid curve (22'*) representinga regression(Eq. a) on the 2V. vahrcs calculated by rxcerrnn. Although the nonlinear refractive-index and 2V' curves in Figure 2 appearto suitably relate sample I through 8 to F content, similar relations could not be established with F content taken as the dependentvariable. It appears from Figure 2, however, that 2V and the principle refractive indices for the amblygonite-montebrasiteseriesmay actually vary linearly between 0 and 60 [F]. Indeed, of regressionstested on only the optical data for specimens I to 6. linear models, with F content as the dependent variable, most aptly fit the data and are given below: R2 a : r . 6 t 7 2 7 ( 7 r ) - 5 . 1 0 ( 2 3 )x l 0 - o l F i P : 1 . 6 2 6 s 1 ( 2 0 ) 4 . 2 9 ( 6 )x l O + [ F ] 1: r.64834(22) 7.rr(7) x 10-o[fl 2 V z : 6 r . 3 0 ( 8 1 )+ 0 . 9 2 ( 3 ) [ F l 0.996 0.999 0.999 0.998 (s) (6) (7) (8) If these models were also plotted in Figure 2, their lines would closely follow along the nonlinear models until [fl exceeded-60 (Fig. 3). Above [F] : 60, the linear models begin to deviate markedly from the nonlinear curves of Figure 2 and do not adequatelyfit the 2V and refractiveindex data. Upon examination of Figure 3, one might suspectthat GREINERAND BLOSS:AMBLYGONITE-MONTEBRASITE OPTICS 621 | 50' |20' ?YZ ?YZ 90" 6o" r.55 OU r65 . ",o F (mol%) Fig. 2. Nonlinearmodelsfor 2V, and refractiveindicesvs. [Fl (mole percentF). Solid refractive-indexcurvesobtain from regression Equations1,2, and3. The solidcurvedenoted2ll"* (Eq. 4) of Excelrsn-derived,2V.values represents a regression vs. [fl; the dashedcurve(denoted2Z^,)represents 2V, as calculatedfrom the refractive-index curvesbelow.For samples9, 10, and I 1, whoseF contentswereuncertain,horizontallines extendfrom analyzed [Fl to 100minusthe analyzed[OH] value (l - OH)]. The verticalticksindicatethe valuesof [symbolized molepercentF for thesesamplesif [fl plus [OH] is normalized to 100molo/0. the F contents of samples 7 and/or 8 may actually be lower and that the linear models of refractive index are valid acrossthe entire series.If this were true, the "yand B refractive-index curveswould intersectand result in the existenceof a pseudo-uniaxial amblygonite at the composition having 7: B. Examination of Figure l, however, clearly shows that the migration curves of the two optic axesdo not convergeso as to eventually coincide with a principal direction, X in this case,as would be required of a biaxial mineral approaching uniaxiality. PnnorcuoN oF MoLE pERcENT F Previouswork Moss et al. (1969), using uncalibratedpowder films and diffractometer tracings, determined the relationship of F content to cell parameters and to 2d,r,(CuKa,) for the amblygonite-montebrasiteseries.Cern6 et al. (1973) used diffractometer tracings of amblygonite and montebrasite powder, intermixed with quartz, as an internal standard, to accomplish this. Even though the unit-cell parameters showed only small variations in responseto F content, the F contents proved predictable to +4 molo/ofrom values of 2d,r,(CuI(a,).Cern6 et al. also plotted, relative to F content, the peak differences(2000,- 20,or),where 200u, representedthe l2l, I 10, 021, 0l l, and 120 successively 40 60 roo 80 F (mol%) Fig. 3. Linear models(dashed)comparedto the nonlinear modelsfor 2V.and refractiveindicesvs. [Fl. The linearmodels represent Equations5-8. peaks.Again, estimatesof F content to +4 molo/oresulted. Although the method is faster than the 2d,r, method, these peaks may overlap within several compositional ranges. Kallio (1978) utilized four uncalibrated reflections between46 and 54 20 (CuKar) to estimate F contents to +5.5 molo/0. Fransolet and Tarte (1977) studied infrared spectraof this seriesand establishedlinear relationships betweenF content and the frequenciesof both the stretching (vo") and bending (Do")vibrations of the (OH) molecule. Thus, zo" arrd 6o, servedto estimate F content to +4 mol9oand +3 molo/0,respectively.Cern6 et al. (1973) examined the applicability of specificgravity and of differential thermal analysis as determinative techniques. Neither proved useful because,as they stated,"specific gravity is too sensitive to the presenceof impurities, and diferential thermal behavior is too strongly dependent on the experimental setup." This study Regressions,performed on the data for specimensI to 6 using [F] as the dependentvariable, yielded the following models, which are only valid for [Fl < 60 molo/oand t h u s f o r a > 1 . 5 8 7 ,p > 1 . 6 0 1 ,7 > 1 . 6 0 6 ,a n d 2 V , < ll6.: - r946(87)a IFI : 3148(139) 2327(3s)p 3785(56) tFl: 2317(22) 1405(14)1 tFl: tn: R2 0.992 (9) 0.999 (10) 0.9e9 (l l) -66.3(2.6)+ 1.08(3)x 2V, 0.997 (r2) Of these models, Equation 12 seemsthe most practical 622 GREINER AND BLOSS: AMBLYGONITE-MONTEBRASITE TeeLe4. Observedand estimatedF contentsin molTofor samples with [Fl < 60 F predicted from F observed from Sample [F]1oo_ro"I [FJo," '1" e o 9 10 11 H? AA 3.5 14.7 16.6 29.8 452 530 34 1 46.4 46.5 40 10.8 14.4 26.5 42.7 553 279 348 c+.c 170 450 1 00 tFl" tFl, tFl, IFl", 5.1 12.6 5.0 1 08 3.5 11.4 14.5 55 11. 3 12.6 z6-J ZJ.V 42.9 s5.1 32.9 43.3 500 342 42.8 55.6 34.3 41.3 49.6 230 ( E q . 9 ) ( E q . 1 0 ) ( E q . 1 1 ) (Eq.12) 1Q E tJ.o 23.4 43.0 260 42.7 co. I cc.o 32.8 42.9 50.9 31.9 59.1 31.8 42.1 49.2 36.1 4-O cz.+ t4.c * is trom direct [OH] measurement,and [F]orRis calculated [F],oo-rort from 100 [OH] for this sample. . ' H a a p a l a( 1 9 6 6 ) . t Mookherieeet al. (1979). $ Gallagher(1967) because(l) 2Vz can be quickly measuredto a fraction of a degree by using a simple detent spindle stage (Bloss, 1981) to collect extinction data for Na light and then processingthe data with ExceLBn; and (2) accordingly, if 2V? < - I 16o,F shouldbe predictableto within 2 molo/0. Thus, unless [fl exceeds60 mol0/0,which is rare, Equation 12 probably representsthe most rapid method yet known for precisely calculating the F content of a montebrasite or amblygonite from a physical property. Table 4 compares the observed F contents-namely, those determined directly by chemical analysis [F]o," or by hydroxyl diference, 100 - [OH] or [F]r00-roHr-with the F contents determined by inserting the measuredoptical parametersof samples I to 6 and 9 to 1l into Equations 9 to 12. Clearly, 2V, and all three refractive indices are successfulestimators of F contents between 0 and 60 mol0/0.However, if the chemically determined F contents taken from the literature for specimens I to 6 were systematically high or low, the same will be true of the valuesdeterminedfrom Equation 12. For specimens9, 10, and 11, wherein a discrepancy existedbetween [flo,* and [Fl,oo-rorr,the value predicted from 2V. almost coincided with [F],oo-,or1for specimen 9 and fell between[F]o,* and [F],ooro.rfor specimensl0 and ll. Note also that the optical properties of sample 10 closelyconform to those of sample5. A searchof the literature disclosedthree specimens(A, B, and C in Table 4) for which F contents and partial optical analyseswere available (Haapala, 1966; Mookerjeeet al., 1979;,Gallagher,1967).However, significant discrepanciesexist betweentheir reported F contentsand thosepredicted by inserting their reported optical parametersinto Equation 9, 10, I l, or 12. Thesediscrepancies may have resultedfrom incorrect chemical and/or optical data, or there may actually have been differencesin F contentbetweenthe samplesexaminedoptically and those chemically analyzed. OPTICS Cern6et al. (1973)carefullyselectedhomogeneousmaterial for each of the samples used in their study and, subsequently,in severalother studies,including this one. Such attentive preparation of samplesmay have been absent in previous optical work, and thus, as statedby Cern6 et al., "the diferences between the analyzed and the optically studied materials in many earlier studiesare the most probable explanation for the poor correlation of optics with fluorine content in Winchell and Winchell's (1951) graph." Concerningdifferencesin F content between samplesanalyzedchemically and samplessubjected to measurement of physical properties, Cern6 et al. (1973) stated,"grains and crystalsof amblygonite-montebrasiteminerals frequently show primary compositional zoning and/or secondaryreplacementby members of the same serieswith different fluorine contents." Discrepanciesbetween optically and chemically determined F contentsmay also be due to the presenceof fluid inclusions and daughter minerals that contain F in concentrations greater or less than that of the host mineral. F contained within fluid inclusions and daughter minerals would be incorporated into the F analysisof a sample by a technique such as neutron activation. By contrast, F estimatesbased on optical properties refer only to that contained in the host mineral, assumingthat the equations used for estimation were derived, as they indeed were, from a suite of sampleswith few inclusions. Cern6et al. (1973)reportedtheir specimenAF-1, which contained abundant inclusions, to contain 62.7 molo/oF by neutron activation (: [F]",.) but 73.0 molo/oby hydroxyl difference(: [F],oo ro"r).The angle 2V, measured for a crystal of AF-I, estimated [F] by use of Equation 12, at 57.0. The sample is very cloudy; thus, refractive indicescould only be roughly estimated.Estimationsfrom them placed [F] at 55 to 60. Finally, the optic orientation of AF- I is nearly identical to that of sample 6 (n : 55.3).Thus, it appearsthat the host amblygonitefor AF-1 contains 55 to 60 molo/oF and that possibly F is present in a higher concentration in the fluid inclusions and daughter minerals. Microscopic examination of the fluid inclusions in AF-l revealed the presence of a cubic daughter mineral, possibly villiaumite (NaFt R. J. Bodnar, pers. comm.). Thus, for samplesof amblygonite and montebrasitethat contain a significant amount of included material, 2V, measurement is clearly superior to chemical analysisin evaluating the F content of the host mineral. Influence of Na content on F prediction Most natural amblygonites and montebrasitescontain minor Na via substitution for up to l0 molo/oLi (Dubois el aI., 1972); thus, an evaluation of the influence of Na content on the accuracyof Equations 9-12 seemsin order. The substitution of Na for Li in this seriesresults in minor changesin density and involves ions that have very similar polarizabilities (Pirenne and Kartheuser, 1964) and electronegativities(Pauling, 1960). This suggeststhat Na content should have very little effect on the GREINER AND BLOSS: AMBLYGONITE.MONTEBRASITE OPTICS 623 relationships between optical properties and F content structure and causesthe correspondingrefractive index'y establishedin this study. Indeed, the refractive indices to increaseat a faster rate than a or B. 1.594,1.603,and 1.615reportedby Nriagu and Moore AcxNowr,nlcMENTS (1984), for a sample containing -56.0 molo/oNa and -46.5 molo/oF, agreewell with the values 1.594, 1.607, We thank Petr Cernj'and Iva Cern6(University of Manitoba) for kindly providing analyzedsamples and for their prompt replies to numerous and I .6 I 5 predicted by Equations 5, 6, and 7, when [fl : 46.5 was inserted. Thus, unless Na content only affects questions.We are grateful to Frank Hawthome (University of Manitoba) for supplying structural data, which proved invaluable. We thank Paul the B refractive index, which seemsvery unlikely, the Na Ribbe, who read the manuscript and made suggestionsthat contributed content of most natural sampleswill not affect F predic- greatlyto its improvement. Shu-ChunSu'sand Mickey Gunter's help with the statisticalaspectsofthis study is greatly appreciated,as is the drafting tions basedon Equations9-12. The differencein ionic radius between Na and Li is at of figuresby Melody Wayne and Tom Wilson. teast 0.26 A lshannon and Prewitt, 1969) if Li is sixRnrnnrNcrs coordinated. This is rather large when considering the 1.30-A radius of three-coordinatedF (Shannon and Armbruster, Thomas, and Bloss, F.D (1982) Orientation and effectsof channel HrO and CO, in cordierite. American Mineralogist, 67,284Prewitt) and the I .34-A radius of three-coordinated(OH) 291 (Ribbe and Gibbs, l97l). Thus, predictionsof F content Bloss,F.D. (1978) The spindle stage:A turning point for optical crystalbasedupon subtle variations in lattice parameterswill be lography.AmericanMineralogist,63, 433-447. (l 98 l) The spindle stage:Principlesand practice CambridgeUnisignificantlyin error if the measuredsamplecontainseven versity Press,Cambridge and New York, 340 p. minor Na. Measurementsof cell volume by Dubois et al. Bragg,W. L- (1924) The refractive indices of calciteand aragonite.Royal (1972)support this conclusion. Proceedings, A, 105,370-386. Rnr,l.rroN oF oprICAL pRopERTTES TO STRUCTURE AND POLARIZATION Cern6 et al. (1973) and Hawthorne (pers.comm.) have shown that as (OH) content increasesin the amblygonitemontebrasite series, the cell volume increases slightly, whereasthe density decreasesslightly. Both structural effects are ordinarily associatedwith a decreasein refractive indices. In this series,however, their effect appears to be overwhelmed by the increasein refractive indices resulting from substitution ofthe highly polarizableanion (OH)- for the relatively nonpolarizable F . Influence of the polarizability of (OH) on optics For hydroxyl-rich members of the amblygonite-montebrasite series, the principal vibration direction Z lies reasonablycloseto the O-H bond direction (triangle, Fig. l) locatedby Hawthorne (pers.comm.). Increasesin (OH) content thus cause"y to increaseat a greater rate than a or B. Conversely,the decreasein (OH) from left to right in Figure 2 causes7 to decreasefaster than a or B. This causesthe birefringence@ to decreasewith increas") ing F content and also contributes to the changein optic sign from (+) for montebrasitesto (-) for amblygonites. Positional changesin the two optic axes and X, Y, and Z appearedmuch more abrupt as [fl increasedfrom 55 to 79 (Fig. l) than when it increasedfrom 79 to 92. CoNcr,usroNs l. For montebrasite-amblygonite crystals for which [F] < 60 mol0/0,their F content can be estimated to -2 molo/ofrom their measuredvalues for 2V, a, B, or 7. Results seemedrelatively unaffectedby Na content. 2. Substitution of (OH)- for F in the amblygonitemontebrasite structure causesthe principal vibration direction Z to align subparallel to the O-H vector in the SocietyofLondon Burri, Conrad. (1956) Charakterisierungder Plagioklasoptik durch drei Winkel und Neuentwurf des Stereogrammsder optischenOnentierung ftir konstante Anorthit-Intewalle. SchweizerischeMineralogischeund PetrographischeMitteilungen, 36, 539-592. eern6, Iva, Cemj', Petr, and Ferguson,R.B. (1973) The fluorine content and some physical properties of the amblygonite-montebrasiteminerals.AmericanMineralogist,58, 291-301. Dubois, J, Marchand,J., and Bourguignon,P. (1972)Donn6esmin6ralogiquessur la s6rie amblygonite-montebrasite.Annales de la Soci6t6 G6ologiquede Belgique,95, 285-310. Fransolet, Andr6-Mathieu, and Tarte, Piene. (1977) Infrared spectraof analyzedsamplesof the amblygonite-montebrasiteseries:A new rapid semi-quantitative determination of fluorine. American Mineralogist, 62,559-564 Gallagher, M J. (1967) Phosphatesand other minerals in pegmatitesof Rhodesiaand Uganda. Mineralogical Magazine, 36, 50-59. Greiner,D.J (1986)Influenceoffluorine versushydroxyl contenton the optics of the amblygonite-montebrasiteseries.M.Sc thesis, Virginia PolytechnicInstitute and StateUniversity, Blacksburg,Virginia. Haapala, Ilmari. (1966) On the granitic pegmatitesin the PereseinejokiAlavus area, South Pohjanmaa, Finland Bulletin de la Commission G6ologiquede Finlande224,98 p Kallio, Pekka.(1978)A new X-ray method for the estimationoffluonne content in montebrasites.American Mineralogist, 63, 1249-1251. Lager,G A ( 1986)Prediction of refractive indicesby point-dipole models (abs.).International Mineralogical Association, l4th General Meeting, Abstractswith Program, 148-149. Megregian,Stephen.(l 954) Rapid spectrophotometricdetermination of fluoride with zirconium-eriochromecyanine R lake Analytical Chemi s t r y ,2 6 , I l 6 l - l 1 6 6 Mereiter, Kurt, and Preisinger,Anton (1986) Correlations betweenoptical properties and crystal structures of uranyl carbonate minerals (abs.). International Mineralogical Association, l4th General Meeting, Abstractswith Program,170. Mookherjee, Asoda, Basu, Kanika, and Sanyal, S. (1979) Montebrasite and metatriplite from zoned pegmatitesof Govinpal, Bastar District, M P Indian JournalofEarth Sciences, 6(2), l9l-199. Moss,A.A., Fejer,E.E.,and Embrey,P.G. (1969)On the x-ray identification of amblygonite and montebrasite Mineralogical Magazine,37, 4t4-422. Nriagu, J O., and Moore, P.B. ( I 984) Phosphateminerals,p. 81. SpringerVerlag, Berlin. Palache,Charles,Richmond,W.E.,and Wolfe, C.W (1943)On amblygonite. American Mineralogist, 28, 39-53. Pauling, Linus (1960) The nature of the chemical bond, third edition. Comell University Press,Ithaca, New York. 624 GREINER AND BLOSS: AMBLYGONITE-MONTEBRASITE Phillips, W.R., and Griffen, D.T. (1981) Optical mineralogy:The nonopaqueminerals,p.77-79. W.H. Freemanand Co., San Francisco. Pirenne,Jean,and Kartheuser,Edward. (l 964) On the refractivity ofionic crystals.Physica,30, 2005-2018. Ray, A.A. (1982)SASuser'sguide:Statistics1982edition.SAS Institute, Inc., Cary, Nonh Carolina Reinhard, Max. (1931) Universal Drehtischmethoden.Wepf, Basel. Ribbe, P.H., and Gibbs, G.V. (1971) Crystal structuresof the humite minerals: III Mg/Fe ordering in humite and its relation to other ferromagnesian silicates.AmericanMineralogist,56, I155-l 173. Selkregg,K.R., and Bloss, F.D, (1980) Cordierites: Compositional controls of A, cell parameters,and optical properties.American Mineralogist,65, 522-533. Shannon, R.D., and Prewitt, C.T. (1969) Effective ionic radii in oxides and fluorides. Acta Crystallographica,825, 925-946. OPTICS Simonov, V.L, and Belov, N V. ( 1958)The determination of the structure of amblygonite by the minimum function method. Kristallografiya, 3, 428-437 Su, S.-C.,Bloss,F.D., Ribbe, P.H , and Stewart,D.B. (1984)Optic axial angle,a precisemeasureofAl,Si ordering in Tr tetrahedral sites ofKrich alkali feldspars.American Mineralogrst, 69, 44U448. Winchell,A.N., and Winchell, Horace.(1951)Elementsof optical mineralogy, Part II. Descriptions ofminerals, fourth edition, p.223-224. Wiley, New York. MrNuscnrst MaNuscnrrr REcETvEDSeprsr4ger 19, 1986 AccEprED J.rxunnv 30, 1987
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