<?xml version="1.0" encoding="UTF-8"?><!DOCTYPE article  PUBLIC "-//NLM//DTD Journal Publishing DTD v3.0 20080202//EN" "http://dtd.nlm.nih.gov/publishing/3.0/journalpublishing3.dtd"><article xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" dtd-version="3.0" xml:lang="en" article-type="research article"><front><journal-meta><journal-id journal-id-type="publisher-id">GEP</journal-id><journal-title-group><journal-title>Journal of Geoscience and Environment Protection</journal-title></journal-title-group><issn pub-type="epub">2327-4336</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/gep.2022.102006</article-id><article-id pub-id-type="publisher-id">GEP-115451</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Earth&amp;Environmental Sciences</subject></subj-group></article-categories><title-group><article-title>
 
 
  Petrology, REE Geochemistry and Tetrad Effect of Some Muscovite Granites at Wadi El Gemal Area, South Eastern Desert, Egypt
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Ahmed</surname><given-names>S. Shalan</given-names></name><xref ref-type="aff" rid="aff1"><sub>1</sub></xref></contrib></contrib-group><aff id="aff1"><label>1</label><addr-line>Nuclear Materials Authority, El-Maadi, Cairo, Egypt</addr-line></aff><pub-date pub-type="epub"><day>08</day><month>02</month><year>2022</year></pub-date><volume>10</volume><issue>02</issue><fpage>75</fpage><lpage>93</lpage><history><date date-type="received"><day>3,</day>	<month>November</month>	<year>2021</year></date><date date-type="rev-recd"><day>22,</day>	<month>February</month>	<year>2022</year>	</date><date date-type="accepted"><day>25,</day>	<month>February</month>	<year>2022</year></date></history><permissions><copyright-statement>&#169; Copyright  2014 by authors and Scientific Research Publishing Inc. </copyright-statement><copyright-year>2014</copyright-year><license><license-p>This work is licensed under the Creative Commons Attribution-NonCommercial International License (CC BY-NC).http://creativecommons.org/licenses/by-nc/4.0/</license-p></license></permissions><abstract><p>
 
 
  The muscovite granites at the study area are being emplaced into biotite granites and ophiolitic m&#233;lange settings. They occur in four exposures namely; Umm Seleimat, Sikait, Umm El Kheran and Umm Addebaa exposure. The presence of garnet and muscovite flakes may reflect the peraluminous nature of the studied muscovite granites. Petrographically, the studied granites are mostly subsolvus and consist of plagioclase, K-feldspars, quartz, muscovite and biotite. Garnet, zircon, allanite and opaques are accessories. The textural features of these granites are expressed by bent plagioclase lamellae, distorted microcline twinning, deformed mica flakes and development of myrmekite and recrystallization of feldspars into fine-grained aggregates. Umm Seleimat and Sikait exposures are more differentiated due to the presence of high content of K-feldspar and LREEs. The REE budget decreased from Umm Seleimat-Sikait exposures to Umm El Kheran-Umm Addebaa exposures as (514.5
   
  -
   
  495.6) to (195.9
   - 
  197.7), respectively. Umm Seleimat-Sikait exposures have lower HREE/LREE (0.12
   - 
  0.67), relative to Umm El Kheran-Umm Addebaa exposures (0.99
   - 
  2.06). The studied granites revealed that the chondrite normalized REE patterns are the normal M-type of tetrad effect, where TE1,3 tetrad effect is higher than 1 in all samples which implies that there was an interaction between melt and water-haloid-rich fluid when these granites are crystallized from magma. Spectrometric values of Umm Seleimat and Umm Addebaa indicate that U content is more than Th content. Applying the U mobilization equation proved that the studied granites have been originated from a late magmatic phase of magma very rich in radioelements, also the majority of measurements lie above the zero line indicating that the studied granites affected with hydrothermal solutions rich in uranium than thorium which indicates uranium addition.
 
</p></abstract><kwd-group><kwd>Wadi El Gemal</kwd><kwd> Umm El Kheran</kwd><kwd> REE Geochemistry</kwd><kwd> Tetrad Effect</kwd><kwd> Egypt</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>The study area is located between latitudes 24˚39'18&quot;N and 24˚34'30&quot;N and longitudes 34˚47'42&quot;E and 34˚53'43&quot;E (<xref ref-type="fig" rid="fig1">Figure 1</xref>) at about 52 km, southwest of Marsa Alam coastal city. In Egypt, peraluminous leucogranites represent phases of late orogenic to an orogenic granite complex. They brought about Mo, Sn, W, U, and Nb-Ta mineralization in the form of stock works or in the quartz veins within the granitic rocks (Hassan et al., 1984; Takla &amp; Nowier, 1980). In geosciences, tetrad effect-like REE patterns are reported both in magmatic rocks and in precipitates from hydrothermal fluids (Masuda &amp; Ikeuchi, 1978; Masuda &amp; Akagi, 1990; Akagi et al., 1993; Lee et al., 1994; Kawabe, 1995; Akagi et al., 1996; Bau, 1996). Recent discussions about the tetrad effect focus on highly evolved igneous rocks (Bau, 1997; Pan, 1997), which are often interpreted as transitional between the end-members of magmatic and high-temperature hydrothermal systems (e.g., Bau, 1996; Irber &amp; Bau, 1995). The objective of this contribution is to examine if the intensity of the tetrad effect correlates with parameters that reflect the evolution of granitic melts. Additionally, a Rayleigh REE fractionation is calculated to examine whether mineral fractionation can cause the gradual evolution of the tetrad effect or not. In this paper, the author throws some light on the geology, petrography, REE geochemistry and radioactivity of some muscovite leucogranites at Wadi El Gemal area.</p></sec><sec id="s2"><title>2. Geologic Setting</title><sec id="s2_1"><title>2.1. Regional Geology</title><p>The Migif-Hafafit metamorphic core complex represents one of three major domal structures in the Eastern Desert of Egypt: Gabal Meatiq (Loizenbauer et al., 2001), Abu Swayel (Abd El-Naby &amp; Frisch, 2002), and Migif-Hafafit area (Fowler &amp; El Kalioubi, 2002; Abd El-Naby et al., 2000). The geology of Hafafit area has been documented as highly complex, and many hypotheses have been proposed for the tectonic evolution of this area (Fowler &amp; Osman, 2001). The study area is a part of the Migif-Hafafit and Wadi Nugrus-Wadi El Gemal areas representing the geologic and tectonic key domains with great significance in the tectonic evolution of the Arabian Nubian Shield, which belongs to the Pan African events. The rock units along W. El Gemal differ in colors and tones, thus they easily to be recognized and delineated on a Landsat image (<xref ref-type="fig" rid="fig1">Figure 1</xref>(a)).</p></sec><sec id="s2_2"><title>2.2. Geology of the Study Area</title><p>The rocks exposed in the study area (<xref ref-type="fig" rid="fig1">Figure 1</xref>(b)) are dominantly ophiolitic m&#233;lange (oldest), metagabbros, biotite granites that intruded by small-to-large</p><p>bosses of muscovite granites with sharp contacts and post granite dikes and veins (youngest). No chilled margins are observed at the contact between the muscovite granites and their surroundings. These granites are localized in many exposures within this area namely; Umm Seleimat, Sikait, Umm El Kheran and Umm Addebaa exposures which considered a tributaries of W. Nugrus and W. El Gemal. 1) Umm Seleimat exposure: The muscovite granite at Umm Seleimat exposure is large in size (&gt;1.0 km<sup>2</sup>) and emplaced along NW-SE trend, reaching about 1 - 2 Km. in length and 200 - 300 m in width. It appears as small off-shoots of boss-like bodies, as dike-like bodies and a huge semicircular mass forms domal shape intrudes the biotite granites and the ophiolitic m&#233;lange (<xref ref-type="fig" rid="fig2">Figure 2</xref>(a)). It is characterized by white color, fine- to coarse-grained and occasionally pegmatitic. In some places, the</p><p>muscovite granite is highly deformed due to intensive tectonism. 2) Sikait exposures: the muscovite granites occur as masses or bosses with either rounded to elongated tops or even sharp peaks intruding the ophiolitic m&#233;lange which underwent high temperature-low pressure metamorphism (El Shazly &amp; Hassan, 1972; El Bayoumi &amp; Greiling, 1984) (<xref ref-type="fig" rid="fig2">Figure 2</xref>(b)). The studied granite at Sikait is small in size (&lt;1.0 km<sup>2</sup>) and emplaced along NW-SE trend, reached about 300 - 400 m. in length and 50 - 100 m. in width. It is characterized by white color and grain size ranges between coarse-grained to coarse pegmatite. Pelitic rocks, mainly schists, are abundant as a matrix in the ophiolitic m&#233;lange. 3) Umm El Kheran exposure: the studied granite is located close to the major Nugrus thrust and appears as a huge semi-circular masse, form rounded and domal shapes within the high topography ridge of the metagabbro rocks intrudes in the ophiolitic m&#233;lange (<xref ref-type="fig" rid="fig2">Figure 2</xref>(c)). The granite of Umm El Kheran exposure is relatively large in size (&gt;1.0 km<sup>2</sup>) emplaced along NW-SE trend, reached about 1.5 - 2.5 km. in length and 300 - 500 m. in width, characterized by white color, coarse-grained and occasionally pegmatitic in some places. Two conjugate faults dissect the Umm El Kheran muscovite granite, NNW-and WNW with opposite sense of movements (left and right hand respectively) (Mahmoud, 2009). Metagabbros and talc-carbonates are the most common mafic-ultramafic fragments of the ophiolitic m&#233;lange at Umm El Kheran exposure. It has NW-SE foliation dipping due to NE direction with dip angle ranges from 60˚ - 70˚. 4) Umm Addebaa exposure: it occurs as boss or dike–like body of the muscovite granite (&lt;1.0 km<sup>2</sup>) emplaced along the N-S trend, about 100 m. in length and 50 m. in width intrudes in the ophiolitic m&#233;lange (<xref ref-type="fig" rid="fig2">Figure 2</xref>(d)). They are deformed and show well-known spheroidal weathering. The periphery, about 1 m wide, of the studied muscovite granite is characterized by presence of monomineralic bands of visible spessartine garnet. An NNW-SSE strike slip faults dislocate the muscovite granite pluton with common displacement. Some basic dikes (NNW-SSE) are cut through the muscovite granite (<xref ref-type="fig" rid="fig2">Figure 2</xref>(e)). The ophiolitic melange is characterized by high foliation striking NW-SE and dipping (20˚ - 50˚) due to SW. Quartz-bearing beryl is present at Umm Addebaa exposure.</p></sec></sec><sec id="s3"><title>3. Methodology</title><p>Petrographical characteristics of the studied muscovite granites are examined in seventeen thin sections representing the muscovite granites in the four exposures. Fifteen of them [(4) from Umm Seleimat, (3) from Sikait, (4) from Umm El Kheran and (4) from Umm Addebaa], chemically analyzed for their rare earth elements by Induced Couple Plasma Spectrometer (ICP-OES) in the labs of Nuclear Materials Authority, Egypt. Analytical conditions were 1200 Watt R Watt RF current, 18 L/min. Coolant gas, 36 L/min. Neublizer gas pressure and 3 Replicant. The granitic samples were crushed and powdered in an agate mortar, 0.5-g was digested by 10 ml of 40% hydrofluoric acid (HF) and 5 ml of 98% sulfuric acid (H<sub>2</sub>SO<sub>4</sub>), it was heated at 200˚C till dryness and it was dissolved in 10 ml of 20% hydrochloric acid (HCl) the volume was completed to 50 ml by ultra-pure water. Na<sub>2</sub>CO<sub>3</sub> and H<sub>3</sub>BO<sub>4</sub> for alkali flux were high grade (EDWIK) The standard solutions of REEs used for calibration were prepared in 4% HNO<sub>3</sub> diluted from 1000 ppm standard solutions for atomic absorption spectrometry manufactured in Canada. Duplicate measurements provided a precision generally better than 2%, except for Er and Lu (&lt;3%). The accuracy of the analyses was monitored by a series of international reference materials. Based on the rock standard, accuracy was usually better than 5%, except for La, Er (&lt;10%), and Pr (&lt;30%). The detection limits for ICP-OES analyses are listed in <xref ref-type="table" rid="table1">Table 1</xref>.</p><p>Field ground γ-ray spectrometry survey has been done using γ-ray spectrometric multichannel analyzer instrument model RS-230 Canadian Type. Ground γ-ray spectrometric survey can detect dose rate (D.R.) in unit (nanosieverts per hour (nSvh-1)), potassium (K %), equivalent uranium content (eU ppm), and equivalent thorium content (eTh ppm).</p></sec><sec id="s4"><title>4. Petrography</title><p>Umm Seleimat muscovite granite is dominantly composed of quartz and feldspars (including plagioclase, microcline and perthite) in equal contents, muscovite and biotite. Garnet, allanite, zircon and iron oxides are common accessories. The abundant form of quartz is coarse-grained with more or less irregular boundaries. Plagioclase occurs as subhedral to euhedral tabular crystals of variable sizes exhibiting lamellar and albitic twining shows corrosional boundaries against perthite (<xref ref-type="fig" rid="fig3">Figure 3</xref>(a)). Microcline crystals with anhedral outlines distinguish by tartan or cross-hatched twinning (<xref ref-type="fig" rid="fig3">Figure 3</xref>(b)). Perthite is coarse and corroded by quartz. The muscovite occurs as subhedral flakes that are corroded by quartz (<xref ref-type="fig" rid="fig3">Figure 3</xref>(c)). Biotite shows a good cleavage and interference color from brown to green. Garnet occurs either as regular crystals, or as irregular crystals and skeletal forms, which are surrounded by quartz and biotite as inclusions (<xref ref-type="fig" rid="fig3">Figure 3</xref>(d)). Sikait muscovite granite is mainly composed of plagioclase, alkali feldspars, muscovite, biotite and quartz. Garnet, zircon, monazite and opaques are accessories. Plagioclase is represented by albite which occurs as subhedral crystals with high deformed and kinked lamellae (<xref ref-type="fig" rid="fig3">Figure 3</xref>(e)). Some crystals are granulated forming morter texture. Potash feldspars are mainly microcline perthite. Some crystals are strained and elongated forming fussy texture. Biotite is characterized by its anhedral shape with interference of color from green and brown (<xref ref-type="fig" rid="fig3">Figure 3</xref>(f)) with a good cleavage. Muscovite is common and occurs as tabular, isolated crystals. Garnet occurs either as euhedral polygonal crystals (<xref ref-type="fig" rid="fig3">Figure 3</xref>(g)) or as highly tectonically deformed subhedral to anhedral crystal. Zircon is found as euhedral crystals with color zonation included in plagioclase (<xref ref-type="fig" rid="fig3">Figure 3</xref>(h)). Monazite occurs as euhedral crystals included in quartz (<xref ref-type="fig" rid="fig3">Figure 3</xref>(i)). Umm El Kheran muscovite granite is medium to coarse-grained, showing hypidiomorphic equigranular texture. It is composed mainly of plagioclase, Quartz, rare K-feldspar, biotite and muscovite. Garnet, allanite and zircon are accessories. Fine-grained white mica aggregates and chlorite are secondary minerals. Myrmekitic texture is common. Plagioclase is the dominant feldspar in the</p><p>rock occurs as tabular cloudy crystals with albite and percline twinning (<xref ref-type="fig" rid="fig4">Figure 4</xref>(a)) and exhibit wide range of grain sizes and generally corroded by quartz; along their boundaries a myrmekitic texture was observed (<xref ref-type="fig" rid="fig4">Figure 4</xref>(b)). The presence of myrmekitic texture represents strong evidence for metasomatic origin, which are common in magmatic granite (Smith, 1974). Microcline perthite is observed in subordinate amount as anhedral megacrysts showing the characteristic cross-hatched or tartan pattern, as a result of albite and percline twins’ combination (Deer et al., 1992). Biotite and muscovite occur as fine-to medium-grained in both xenomorphic and subhedral flakes (<xref ref-type="fig" rid="fig4">Figure 4</xref>(c)). Umm Addebaa muscovite granite is coarse-grained and mainly composed of plagioclase, quartz, K-feldspar, muscovite and biotite. Plagioclase is dominant than K-feldspar. Fine-grained white mica aggregates and chlorite are secondary minerals, while, zircon, garnet and tourmaline are common as accessory minerals.</p><p>Myrmekitic texture is common. Plagioclase is represented by albite which occurs as subhedral to anhedral crystals with slight deformation (<xref ref-type="fig" rid="fig4">Figure 4</xref>(d)). Quartz occurs in appreciable amount as anhedral crystals, corroding all the preceding minerals. Muscovite is present in considerable amounts, although it is most common mica in the studied granite. Garnet; occurs as large oriented irregular crystals with pale pinkish color in plane polarized light, which appears in cracked or polygonal form (<xref ref-type="fig" rid="fig4">Figure 4</xref>(e) &amp; <xref ref-type="fig" rid="fig4">Figure 4</xref>(f)).</p><p>From petrographical point of view, the author classified the four exposures of the muscovite granites in the study area into two exposures as: Umm Seleimat-Sikait exposure and Umm El Kheran-Umm Addebaa exposure. Umm Seleimat-Sikait exposure is characterized by fine to pegmatitic granularity with high k-feldspar content and highly sheared and deformed rocks, while Umm El Kheran-Umm Addebaa exposure is characterized by fine- to coarse-granularity with low k-feldspar content and weak sheared rocks.</p></sec><sec id="s5"><title>5. REE Geochemistry and Tetrad Effect</title><p>Discussion</p><p>The geochemistry of the rare earth elements (REEs) has been found that the behavior of the REEs in most geological environments can be accounted for by differences in their ionic radii (increasing contraction of the 5s and 5p electron shells with increasing atomic mass) as well as variations in valence states (Ce<sup>+3</sup> or Ce<sup>+4</sup>, Eu<sup>+2</sup> or Eu<sup>+3</sup>). However, an additional feature in the distribution patterns of the REEs is the tetrad effect. It refers to the subdivision of the 15 lanthanide elements into four groups in a chondrite normalized distribution pattern: 1) La-Ce-Pr-Nd, 2) Pm-Sm-Eu-Gd, 3) Tb-Dy-Ho, and 4) Er-Tm-Yb-Lu, and each group forms a smooth convex (M-type) or concave (W-type) pattern (Masuda et al., 1987).</p><p>t 1 = ( C e C e t &#215; Pr Pr t ) 0.5       t 3 = ( T b T b t &#215; D y D y t ) 0.5</p><p>Degree of the tetrad effect TE1,3 = (t<sub>1</sub> &#215; t<sub>3</sub>)<sup>0.5</sup>.</p><p>An REE pattern that does not show a tetrad effect has values of TE 1.3 &lt; 1.1. The M-shaped pattern shows ТЕi &gt; 1.1 and the W-shaped TEi &lt; 0.9.</p><p>The REE tetrad effect is most visible in late magmatic differentiates with strong hydrothermal interactions or deuteric alteration. Moreover, the tetrad effect is often accompanied by other modified geochemical behavior of many trace elements, which is termed by Bau (1996) as non-CHARAC behavior (CHARAC = Charge-and-Radius-Controlled). Such behavior occurs typically in highly evolved magmatic systems enriched in H<sub>2</sub>O, CO<sub>2</sub> and elements such as Li, B, F and/or Cl, which suggests the increasing importance of an aqueous like fluid system during the final stages of granite crystallization (Bau, 1996; Irber, 1999). The modern advanced studies indicate that the REE budget of the hydrothermal fluids can be mobilized under particular conditions at metasomatic alteration (Michard, 1989). The REE mobility is controlled by pH, high water/rock ratios, and abundant complex ions CO 3 2 − , F<sup>−</sup>, Cl<sup>−</sup>, PO 4 2 − , and SO 4 2 − (Hass et al. 1995). The kinked pattern which is the characteristic REE tetrad effect, according to Masuda et al. (1987), extraction of a coexisting fluid from a peraluminous melt would result in both of the M-shaped and W-shaped REE tetrad effect, the former of which would be shown in the residual melt phase and the latter of which shown in the fluid. However, this corresponding relationship for a magma system has not been observed in the natural environment. Recently, it has been argued that peraluminous magmatic systems represent the transition from a silicate melt to a high-temperature hydrothermal system, and thus, the geochemical behavior of the isovalent incompatible elements in highly evolved granitic rocks are controlled mainly by chemical complexation with a variety of ligands (Bau &amp; Dulski, 1999; Bau, 1996, 1997; Dostal &amp; Chatterjee, 2000). Therefore, the origin of the REE tetrad effect was ascribed to the interaction between fluorine bearing fluid and silicate melt phases. Monecke et al. (2002), proposed that the tetrad effect might have formed within the magma fluid system before emplacement in the subvolcanic environment where phase separation caused a split of this system into fluid and magma subsystems, or that the tetrad effect might also be inherited from an external fluid influencing the system during or after the emplacement of the magma. Takahashi et al. (2002) recently found both W- and M-type tetrad effect in REE patterns for the water-rock systems in the Tono uranium deposit, central Japan, which is interpreted as that the preference of the groundwater for a W-type tetrad effect produces an M-type tetrad effect in the granitic rocks during weathering processes. It is important to notice that the reported cases are M- or W-type tetrad effects occurring separately in natural systems, however, the composite M- and W-type REE tetrad effect were firstly reported by Zhao et al. (2008). Thus, our study is important step in understanding the REE tetrad effect. The kinks in the REE patterns are camouflaged by prominent convex and concave tetrads and pronounced negative to slightly positive Eu anomalies. The second tetrad is comparably difficult to recognize due to the anomalous behavior of Eu and the fact that Pm does not occur in nature.</p><p>Results</p><p>In the granites studied the concentrations of REEs are determined. The analytical results of REE contents of whole rocks are listed in <xref ref-type="table" rid="table1">Table 1</xref> and plotted on the chondrite-normalized REE patterns are shown in <xref ref-type="fig" rid="fig5">Figure 5</xref> &amp; <xref ref-type="fig" rid="fig6">Figure 6</xref>. The concentration of any given REE in any given rock has proved useful to normalize with standard reference materials. This is appropriate when using graphical plots for REE data. The chondrite normalized patterns in (<xref ref-type="fig" rid="fig5">Figure 5</xref>) are reflected the characters of the solutions which effected in the original rocks. The REE budget decreased from Umm Seleimat-Sikait exposures to Umm El Kheran-Umm Addebaa exposures as (514.5 - 495.6) to (195.9 - 197.7), respectively, as in <xref ref-type="table" rid="table1">Table 1</xref>.</p><p>The muscovite granites of Umm Seleimat-Sikait exposures are characterized by LREEs (average 363.4 - 418.6 ppm) higher than HREEs (151.2 - 76.9 ppm) while the muscovite granites of Umm El Kheran-Umm Addebaa exposures characterized by LREEs (average 87 - 83.1 ppm) lower than HREEs (109 - 114.6 ppm) (<xref ref-type="table" rid="table1">Table 1</xref>), reﬂected in (La/Lu)n values from 0.53 to 1.2. This likely reﬂects preferential depletion of LREE elements by fractionation of accessory phases such as monazite (Mittlefehldt &amp; Miller, 1983) or attributed to the presence of the garnet, which is an excellent host for HREE. Umm Seleimat-Sikait exposures have lower HREE/LREE (0.12 - 0.67), relative to Umm El Kheran-Umm Addebaa exposures (0.99 - 2.06). The REE patterns show strongly negative Eu anomalies</p><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> REE contents of the studied muscovite granites (ppm)</title></caption><table><tbody><thead><tr><th align="center" valign="middle"  rowspan="2"  >Sample</th><th align="center" valign="middle"  colspan="4"  >Umm Seleimat</th><th align="center" valign="middle"  colspan="3"  >Sikait</th><th align="center" valign="middle"  colspan="4"  >Umm El Kheran</th><th align="center" valign="middle"  colspan="4"  >Umm Addebaa</th><th align="center" valign="middle"  rowspan="2"  >Det. Limit (ppb)</th></tr></thead><tr><td align="center" valign="middle" >Sm1</td><td align="center" valign="middle" >Sm2</td><td align="center" valign="middle" >Sm3</td><td align="center" valign="middle" >Sm4</td><td align="center" valign="middle" >S1</td><td align="center" valign="middle" >S2</td><td align="center" valign="middle" >S3</td><td align="center" valign="middle" >Kh1</td><td align="center" valign="middle" >Kh2</td><td align="center" valign="middle" >Kh3</td><td align="center" valign="middle" >Kh4</td><td align="center" valign="middle" >D1</td><td align="center" valign="middle" >D2</td><td align="center" valign="middle" >D3</td><td align="center" valign="middle" >D4</td></tr><tr><td align="center" valign="middle" >La</td><td align="center" valign="middle" >123.1</td><td align="center" valign="middle" >138.54</td><td align="center" valign="middle" >101.22</td><td align="center" valign="middle" >35.87</td><td align="center" valign="middle" >158.75</td><td align="center" valign="middle" >73.01</td><td align="center" valign="middle" >49.65</td><td align="center" valign="middle" >18.4</td><td align="center" valign="middle" >8.6</td><td align="center" valign="middle" >11.3</td><td align="center" valign="middle" >29.01</td><td align="center" valign="middle" >12.01</td><td align="center" valign="middle" >19.06</td><td align="center" valign="middle" >24.12</td><td align="center" valign="middle" >15.1</td><td align="center" valign="middle" >50.0</td></tr><tr><td align="center" valign="middle" >Ce</td><td align="center" valign="middle" >119.87</td><td align="center" valign="middle" >140.24</td><td align="center" valign="middle" >97.64</td><td align="center" valign="middle" >49.84</td><td align="center" valign="middle" >164.2</td><td align="center" valign="middle" >113.72</td><td align="center" valign="middle" >52.62</td><td align="center" valign="middle" >20.13</td><td align="center" valign="middle" >31.2</td><td align="center" valign="middle" >16.4</td><td align="center" valign="middle" >12.5</td><td align="center" valign="middle" >13.04</td><td align="center" valign="middle" >17.76</td><td align="center" valign="middle" >25.3</td><td align="center" valign="middle" >11.23</td><td align="center" valign="middle" >50.0</td></tr><tr><td align="center" valign="middle" >Pr</td><td align="center" valign="middle" >67.42</td><td align="center" valign="middle" >114.5</td><td align="center" valign="middle" >89.8</td><td align="center" valign="middle" >53.31</td><td align="center" valign="middle" >67.98</td><td align="center" valign="middle" >56.21</td><td align="center" valign="middle" >60.86</td><td align="center" valign="middle" >13.37</td><td align="center" valign="middle" >11.93</td><td align="center" valign="middle" >14.72</td><td align="center" valign="middle" >8.12</td><td align="center" valign="middle" >16.07</td><td align="center" valign="middle" >18.85</td><td align="center" valign="middle" >21.9</td><td align="center" valign="middle" >13.03</td><td align="center" valign="middle" >30.0</td></tr><tr><td align="center" valign="middle" >Nd</td><td align="center" valign="middle" >33.76</td><td align="center" valign="middle" >66.74</td><td align="center" valign="middle" >77.56</td><td align="center" valign="middle" >42.41</td><td align="center" valign="middle" >169.52</td><td align="center" valign="middle" >137.1</td><td align="center" valign="middle" >64.75</td><td align="center" valign="middle" >24.5</td><td align="center" valign="middle" >23.68</td><td align="center" valign="middle" >32.4</td><td align="center" valign="middle" >36.47</td><td align="center" valign="middle" >20.63</td><td align="center" valign="middle" >21.03</td><td align="center" valign="middle" >25.85</td><td align="center" valign="middle" >15.34</td><td align="center" valign="middle" >50.0</td></tr><tr><td align="center" valign="middle" >Sm</td><td align="center" valign="middle" >28.45</td><td align="center" valign="middle" >33.86</td><td align="center" valign="middle" >19.02</td><td align="center" valign="middle" >18.05</td><td align="center" valign="middle" >32.65</td><td align="center" valign="middle" >31.06</td><td align="center" valign="middle" >21.34</td><td align="center" valign="middle" >15.94</td><td align="center" valign="middle" >3.02</td><td align="center" valign="middle" >5.9</td><td align="center" valign="middle" >7.16</td><td align="center" valign="middle" >8.72</td><td align="center" valign="middle" >10.96</td><td align="center" valign="middle" >14.19</td><td align="center" valign="middle" >6.72</td><td align="center" valign="middle" >30.0</td></tr><tr><td align="center" valign="middle" >Eu</td><td align="center" valign="middle" >0.29</td><td align="center" valign="middle" >0.53</td><td align="center" valign="middle" >0.46</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >0.97</td><td align="center" valign="middle" >0.93</td><td align="center" valign="middle" >0.66</td><td align="center" valign="middle" >0.71</td><td align="center" valign="middle" >0.773</td><td align="center" valign="middle" >0.684</td><td align="center" valign="middle" >0.939</td><td align="center" valign="middle" >0.37</td><td align="center" valign="middle" >0.25</td><td align="center" valign="middle" >0.31</td><td align="center" valign="middle" >0.27</td><td align="center" valign="middle" >20.0</td></tr><tr><td align="center" valign="middle" >Gd</td><td align="center" valign="middle" >20.12</td><td align="center" valign="middle" >26.46</td><td align="center" valign="middle" >52</td><td align="center" valign="middle" >22.86</td><td align="center" valign="middle" >19.72</td><td align="center" valign="middle" >17.48</td><td align="center" valign="middle" >10.82</td><td align="center" valign="middle" >32.02</td><td align="center" valign="middle" >21.66</td><td align="center" valign="middle" >27.88</td><td align="center" valign="middle" >33.64</td><td align="center" valign="middle" >28.58</td><td align="center" valign="middle" >25.95</td><td align="center" valign="middle" >24.4</td><td align="center" valign="middle" >24.8</td><td align="center" valign="middle" >20.0</td></tr><tr><td align="center" valign="middle" >Tb</td><td align="center" valign="middle" >22.95</td><td align="center" valign="middle" >23.61</td><td align="center" valign="middle" >61.86</td><td align="center" valign="middle" >22.97</td><td align="center" valign="middle" >14.89</td><td align="center" valign="middle" >16.9</td><td align="center" valign="middle" >11.77</td><td align="center" valign="middle" >7.11</td><td align="center" valign="middle" >4.2</td><td align="center" valign="middle" >10.24</td><td align="center" valign="middle" >26.77</td><td align="center" valign="middle" >8.31</td><td align="center" valign="middle" >10.6</td><td align="center" valign="middle" >6.1</td><td align="center" valign="middle" >8.52</td><td align="center" valign="middle" >20.0</td></tr><tr><td align="center" valign="middle" >Dy</td><td align="center" valign="middle" >24.8</td><td align="center" valign="middle" >55.63</td><td align="center" valign="middle" >74.22</td><td align="center" valign="middle" >19.03</td><td align="center" valign="middle" >12.48</td><td align="center" valign="middle" >32.38</td><td align="center" valign="middle" >12.68</td><td align="center" valign="middle" >37.78</td><td align="center" valign="middle" >27.12</td><td align="center" valign="middle" >36.68</td><td align="center" valign="middle" >16.92</td><td align="center" valign="middle" >25.96</td><td align="center" valign="middle" >27.78</td><td align="center" valign="middle" >23.65</td><td align="center" valign="middle" >42.21</td><td align="center" valign="middle" >20.0</td></tr><tr><td align="center" valign="middle" >Ho</td><td align="center" valign="middle" >2.12</td><td align="center" valign="middle" >1.099</td><td align="center" valign="middle" >2.01</td><td align="center" valign="middle" >0.839</td><td align="center" valign="middle" >1.99</td><td align="center" valign="middle" >1.56</td><td align="center" valign="middle" >1.18</td><td align="center" valign="middle" >1.29</td><td align="center" valign="middle" >1.42</td><td align="center" valign="middle" >1.87</td><td align="center" valign="middle" >1.25</td><td align="center" valign="middle" >2.01</td><td align="center" valign="middle" >1.13</td><td align="center" valign="middle" >1.91</td><td align="center" valign="middle" >2.22</td><td align="center" valign="middle" >10.0</td></tr><tr><td align="center" valign="middle" >Er</td><td align="center" valign="middle" >21</td><td align="center" valign="middle" >17.79</td><td align="center" valign="middle" >53.25</td><td align="center" valign="middle" >17.91</td><td align="center" valign="middle" >10.56</td><td align="center" valign="middle" >12.38</td><td align="center" valign="middle" >14.56</td><td align="center" valign="middle" >26.07</td><td align="center" valign="middle" >18.55</td><td align="center" valign="middle" >23.1</td><td align="center" valign="middle" >13.12</td><td align="center" valign="middle" >30.7</td><td align="center" valign="middle" >29.34</td><td align="center" valign="middle" >25.47</td><td align="center" valign="middle" >39</td><td align="center" valign="middle" >10.0</td></tr><tr><td align="center" valign="middle" >Yb</td><td align="center" valign="middle" >13.81</td><td align="center" valign="middle" >18.6</td><td align="center" valign="middle" >14.68</td><td align="center" valign="middle" >8.11</td><td align="center" valign="middle" >12.24</td><td align="center" valign="middle" >19.03</td><td align="center" valign="middle" >4.33</td><td align="center" valign="middle" >8.48</td><td align="center" valign="middle" >22.48</td><td align="center" valign="middle" >9.32</td><td align="center" valign="middle" >19.2</td><td align="center" valign="middle" >11.37</td><td align="center" valign="middle" >14.98</td><td align="center" valign="middle" >26.12</td><td align="center" valign="middle" >8.45</td><td align="center" valign="middle" >10.0</td></tr><tr><td align="center" valign="middle" >Lu</td><td align="center" valign="middle" >1.82</td><td align="center" valign="middle" >1.83</td><td align="center" valign="middle" >1.95</td><td align="center" valign="middle" >1.3</td><td align="center" valign="middle" >1.13</td><td align="center" valign="middle" >2.1</td><td align="center" valign="middle" >0.6</td><td align="center" valign="middle" >1.68</td><td align="center" valign="middle" >1.68</td><td align="center" valign="middle" >2.03</td><td align="center" valign="middle" >2.4</td><td align="center" valign="middle" >1.96</td><td align="center" valign="middle" >2.5</td><td align="center" valign="middle" >2.85</td><td align="center" valign="middle" >1.66</td><td align="center" valign="middle" >5.0</td></tr><tr><td align="center" valign="middle" >∑HREE</td><td align="center" valign="middle" >106.6</td><td align="center" valign="middle" >145.1</td><td align="center" valign="middle" >259.9</td><td align="center" valign="middle" >93.1</td><td align="center" valign="middle" >73.01</td><td align="center" valign="middle" >101.8</td><td align="center" valign="middle" >55.9</td><td align="center" valign="middle" >114.4</td><td align="center" valign="middle" >97.11</td><td align="center" valign="middle" >111.1</td><td align="center" valign="middle" >113.3</td><td align="center" valign="middle" >108.9</td><td align="center" valign="middle" >112.3</td><td align="center" valign="middle" >110.5</td><td align="center" valign="middle" >126.86</td><td align="center" valign="middle" >-</td></tr><tr><td align="center" valign="middle" >∑LREE</td><td align="center" valign="middle" >372.9</td><td align="center" valign="middle" >494.4</td><td align="center" valign="middle" >385.7</td><td align="center" valign="middle" >200.4</td><td align="center" valign="middle" >594.1</td><td align="center" valign="middle" >412.03</td><td align="center" valign="middle" >249.8</td><td align="center" valign="middle" >93.05</td><td align="center" valign="middle" >79.2</td><td align="center" valign="middle" >81.4</td><td align="center" valign="middle" >94.2</td><td align="center" valign="middle" >70.84</td><td align="center" valign="middle" >87.9</td><td align="center" valign="middle" >111.7</td><td align="center" valign="middle" >61.69</td><td align="center" valign="middle" >-</td></tr><tr><td align="center" valign="middle" >Total REEs</td><td align="center" valign="middle" >479.5</td><td align="center" valign="middle" >639.4</td><td align="center" valign="middle" >645.7</td><td align="center" valign="middle" >293.4</td><td align="center" valign="middle" >667.08</td><td align="center" valign="middle" >513.9</td><td align="center" valign="middle" >305.8</td><td align="center" valign="middle" >207.5</td><td align="center" valign="middle" >176.3</td><td align="center" valign="middle" >192.5</td><td align="center" valign="middle" >207.5</td><td align="center" valign="middle" >179.7</td><td align="center" valign="middle" >200.2</td><td align="center" valign="middle" >222.2</td><td align="center" valign="middle" >188.6</td><td align="center" valign="middle" >-</td></tr><tr><td align="center" valign="middle" >Average</td><td align="center" valign="middle"  colspan="4"  >514.5</td><td align="center" valign="middle"  colspan="3"  >495.6</td><td align="center" valign="middle"  colspan="4"  >195.9</td><td align="center" valign="middle"  colspan="4"  >197.7</td><td align="center" valign="middle" >-</td></tr><tr><td align="center" valign="middle" >HREE/LREE</td><td align="center" valign="middle" >0.28</td><td align="center" valign="middle" >0.29</td><td align="center" valign="middle" >0.67</td><td align="center" valign="middle" >0.46</td><td align="center" valign="middle" >0.12</td><td align="center" valign="middle" >0.25</td><td align="center" valign="middle" >0.22</td><td align="center" valign="middle" >1.23</td><td align="center" valign="middle" >1.23</td><td align="center" valign="middle" >1.36</td><td align="center" valign="middle" >1.20</td><td align="center" valign="middle" >1.54</td><td align="center" valign="middle" >1.28</td><td align="center" valign="middle" >0.99</td><td align="center" valign="middle" >2.06</td><td align="center" valign="middle" >-</td></tr><tr><td align="center" valign="middle" >Eu/Eu*</td><td align="center" valign="middle" >0.04</td><td align="center" valign="middle" >0.05</td><td align="center" valign="middle" >0.04</td><td align="center" valign="middle" >0.14</td><td align="center" valign="middle" >0.12</td><td align="center" valign="middle" >0.12</td><td align="center" valign="middle" >0.13</td><td align="center" valign="middle" >0.10</td><td align="center" valign="middle" >0.29</td><td align="center" valign="middle" >0.16</td><td align="center" valign="middle" >0.18</td><td align="center" valign="middle" >0.07</td><td align="center" valign="middle" >0.05</td><td align="center" valign="middle" >0.05</td><td align="center" valign="middle" >0.06</td><td align="center" valign="middle" >-</td></tr><tr><td align="center" valign="middle" >(La/Sm)<sub>N</sub></td><td align="center" valign="middle" >2.70</td><td align="center" valign="middle" >2.56</td><td align="center" valign="middle" >3.32</td><td align="center" valign="middle" >1.24</td><td align="center" valign="middle" >3.04</td><td align="center" valign="middle" >1.47</td><td align="center" valign="middle" >1.45</td><td align="center" valign="middle" >0.72</td><td align="center" valign="middle" >1.78</td><td align="center" valign="middle" >1.20</td><td align="center" valign="middle" >2.53</td><td align="center" valign="middle" >0.86</td><td align="center" valign="middle" >1.09</td><td align="center" valign="middle" >1.06</td><td align="center" valign="middle" >1.40</td><td align="center" valign="middle" >-</td></tr><tr><td align="center" valign="middle" >(La/Lu)<sub>N</sub></td><td align="center" valign="middle" >7.02</td><td align="center" valign="middle" >7.86</td><td align="center" valign="middle" >5.39</td><td align="center" valign="middle" >2.86</td><td align="center" valign="middle" >14.58</td><td align="center" valign="middle" >3.61</td><td align="center" valign="middle" >8.59</td><td align="center" valign="middle" >1.14</td><td align="center" valign="middle" >0.53</td><td align="center" valign="middle" >0.58</td><td align="center" valign="middle" >1.25</td><td align="center" valign="middle" >0.64</td><td align="center" valign="middle" >0.79</td><td align="center" valign="middle" >0.88</td><td align="center" valign="middle" >0.94</td><td align="center" valign="middle" >-</td></tr><tr><td align="center" valign="middle" >(La/Yb)<sub>N</sub></td><td align="center" valign="middle" >6.06</td><td align="center" valign="middle" >5.06</td><td align="center" valign="middle" >4.68</td><td align="center" valign="middle" >3.00</td><td align="center" valign="middle" >8.81</td><td align="center" valign="middle" >2.61</td><td align="center" valign="middle" >7.79</td><td align="center" valign="middle" >1.47</td><td align="center" valign="middle" >0.26</td><td align="center" valign="middle" >0.82</td><td align="center" valign="middle" >1.03</td><td align="center" valign="middle" >0.72</td><td align="center" valign="middle" >0.86</td><td align="center" valign="middle" >0.63</td><td align="center" valign="middle" >1.21</td><td align="center" valign="middle" >-</td></tr><tr><td align="center" valign="middle" >T1</td><td align="center" valign="middle" >1.92</td><td align="center" valign="middle" >1.82</td><td align="center" valign="middle" >1.46</td><td align="center" valign="middle" >1.82</td><td align="center" valign="middle" >0.89</td><td align="center" valign="middle" >1.10</td><td align="center" valign="middle" >1.38</td><td align="center" valign="middle" >1.07</td><td align="center" valign="middle" >1.87</td><td align="center" valign="middle" >1.12</td><td align="center" valign="middle" >0.43</td><td align="center" valign="middle" >1.27</td><td align="center" valign="middle" >1.26</td><td align="center" valign="middle" >1.30</td><td align="center" valign="middle" >1.10</td><td align="center" valign="middle" >-</td></tr><tr><td align="center" valign="middle" >T3</td><td align="center" valign="middle" >4.04</td><td align="center" valign="middle" >7.43</td><td align="center" valign="middle" >7.33</td><td align="center" valign="middle" >5.28</td><td align="center" valign="middle" >2.41</td><td align="center" valign="middle" >4.96</td><td align="center" valign="middle" >3.78</td><td align="center" valign="middle" >2.82</td><td align="center" valign="middle" >2.13</td><td align="center" valign="middle" >2.97</td><td align="center" valign="middle" >3.63</td><td align="center" valign="middle" >2.14</td><td align="center" valign="middle" >3.51</td><td align="center" valign="middle" >1.95</td><td align="center" valign="middle" >2.83</td><td align="center" valign="middle" >-</td></tr><tr><td align="center" valign="middle" >T1,3</td><td align="center" valign="middle" >2.79</td><td align="center" valign="middle" >3.68</td><td align="center" valign="middle" >3.27</td><td align="center" valign="middle" >3.10</td><td align="center" valign="middle" >1.46</td><td align="center" valign="middle" >2.34</td><td align="center" valign="middle" >2.28</td><td align="center" valign="middle" >1.73</td><td align="center" valign="middle" >1.99</td><td align="center" valign="middle" >1.82</td><td align="center" valign="middle" >1.25</td><td align="center" valign="middle" >1.65</td><td align="center" valign="middle" >2.10</td><td align="center" valign="middle" >1.59</td><td align="center" valign="middle" >1.76</td><td align="center" valign="middle" >-</td></tr></tbody></table></table-wrap><p>The TE 1,3 are calculated by the formulae of Irber (1999).</p><p>(Eu/Eu<sup>*</sup> 0.04 - 0.2); this ﬁnding suggests extensive fractionation of feldspar. The normalized REE patterns of the studied granites show elevated (Pr), (Tb, Dy), and (Tm, Yb) relative to the neighboring REE, which may be a weak expression of the tetrad effect (Irber, 1999). This effect is typical of transitional magmatic-hydrothermal systems and is often found in highly evolved, volatile-rich granites (Monecke et al., 2002). According to Jahn et al. (2001), it is unlikely that mineral fractionation alone could generate the tetrad effect in evolved granites. Rather, they emphasized the increasing importance of exchange with aqueous ﬂuid during the ﬁnal stages of granite crystallization. <xref ref-type="fig" rid="fig5">Figure 5</xref> &amp; <xref ref-type="fig" rid="fig6">Figure 6</xref> show that samples of the studied granites have strong M-type tetrad effect in the first and third tetrad. The index of tetrad effect intensity, TE1,3 is higher than 1 in all samples which implies that there was an interaction between melt and water-haloid-rich fluid when these granites are crystallized from magma.</p><p>Therefore, such REE fractionation during evolution, enrichment by accessory minerals and alteration can be interpreted to be the breakdown of accessory minerals and the formation of new minerals (Peterson &amp; Eliasson 1997; Hecht et al., 1999). The ratio La<sub>N</sub>/Yb<sub>N</sub> is considered by Rollinson (1994) as a measure of the degree of fractionation of REEs in the melt. Plotting of the same ratio versus CeN showed that; Umm Seleimat and Sikait exposures are more differentiated than Umm El Kheran and Umm Addebaa exposures, referring to increasing of degree of fractionation with increasing of the LREE represented by Ce (<xref ref-type="fig" rid="fig7">Figure 7</xref>).</p></sec><sec id="s6"><title>6. Spectrometric Investigations</title><p>Discussion: Rogers and Adams (1969) stated that the average content of eU in granite is 4 ppm and that of Th is 16 ppm. Moreover, Darnely (1982) defined the uraniferous granites as any granitic mass containing eU at least twice as Clark value (4 ppm) for normal granites. Such granites may or may not be associated with eU-mineralization. Uranium mobilization (eUm) in the studied</p><p>rocks can be calculated as follows: the uranium mobilization is calculated difference between the measured eU and the expected original uranium, which is calculated by dividing the measured eTh by the average eTh/eU ratio in the crustal acidic rocks (original uranium = eTh/3.5 according to Clark et al., 1966) to give the leaching values of uranium (eUm = eU–eTh/3.5). Positive values indicate uranium addition by mobilization, whereas negative values indicated migration of uranium by leaching. The eU, eTh, K% and other variants in all studied granitic rocks are illustrated in <xref ref-type="table" rid="table2">Table 2</xref>. Some ratios were also calculated (eTh/eU and eU/eTh).</p><p>Results: eU and eTh data of the studied granites of the present study when compared with the published data indicates that these granites can be described as uraniferous granite except granite of the Sikait area considered as not uraniferous where the average U content is less than twice as Clark value (4 ppm). The spectrometric values of Umm Seleimat and Umm Addebaa indicate that U content is more than Th content. Uranium content is more than twice Clark value (4 ppm), while eTh content is too less than Clark value (18 - 20 ppm) suggesting that they are fertile granites.</p><table-wrap id="table2" ><label><xref ref-type="table" rid="table2">Table 2</xref></label><caption><title> Field spectrometric analysis of the range and average contents of eU, eTh, and K % of the studied muscovite granites, SED, Egypt</title></caption><table><tbody><thead><tr><th align="center" valign="middle"  colspan="2"  >(K %)</th><th align="center" valign="middle"  colspan="2"  >eTh/eU</th><th align="center" valign="middle"  colspan="2"  >eU/eTh</th><th align="center" valign="middle"  colspan="2"  >eTh (ppm)</th><th align="center" valign="middle"  colspan="2"  >eU (ppm)</th><th align="center" valign="middle"  rowspan="2"  >The study areas</th></tr></thead><tr><td align="center" valign="middle" >Av.</td><td align="center" valign="middle" >Range</td><td align="center" valign="middle" >Av.</td><td align="center" valign="middle" >Range</td><td align="center" valign="middle" >Av.</td><td align="center" valign="middle" >Range</td><td align="center" valign="middle" >Av.</td><td align="center" valign="middle" >Range</td><td align="center" valign="middle" >Av.</td><td align="center" valign="middle" >Range</td></tr><tr><td align="center" valign="middle" >3.9</td><td align="center" valign="middle" >2.6 - 5.9</td><td align="center" valign="middle" >1.04</td><td align="center" valign="middle" >0.4 - 1.8</td><td align="center" valign="middle" >1.3</td><td align="center" valign="middle" >0.5 - 2.3</td><td align="center" valign="middle" >15.73</td><td align="center" valign="middle" >6 - 28.5</td><td align="center" valign="middle" >21.4</td><td align="center" valign="middle" >4.5 - 41.8</td><td align="center" valign="middle" >Umm Seleimat (n = 17)</td></tr><tr><td align="center" valign="middle" >5.5</td><td align="center" valign="middle" >2.4 - 7.8</td><td align="center" valign="middle" >0.8</td><td align="center" valign="middle" >0.3 - 2.1</td><td align="center" valign="middle" >1.7</td><td align="center" valign="middle" >0.4 - 2.8</td><td align="center" valign="middle" >3.2</td><td align="center" valign="middle" >1.3 - 7.7</td><td align="center" valign="middle" >4.3</td><td align="center" valign="middle" >2.7 - 5.1</td><td align="center" valign="middle" >Sikait (n = 15)</td></tr><tr><td align="center" valign="middle" >3.9</td><td align="center" valign="middle" >2.8 - 4.9</td><td align="center" valign="middle" >1.6</td><td align="center" valign="middle" >1.2 - 2.9</td><td align="center" valign="middle" >0.6</td><td align="center" valign="middle" >0.3 - 0.8</td><td align="center" valign="middle" >9.5</td><td align="center" valign="middle" >3.2 - 15</td><td align="center" valign="middle" >6.9</td><td align="center" valign="middle" >2.9 - 11.5</td><td align="center" valign="middle" >Umm El Kheran (n = 12)</td></tr><tr><td align="center" valign="middle" >2.8</td><td align="center" valign="middle" >1.4 - 3.9</td><td align="center" valign="middle" >0.4</td><td align="center" valign="middle" >0.2 - 0.6</td><td align="center" valign="middle" >2.7</td><td align="center" valign="middle" >1.5 - 6.5</td><td align="center" valign="middle" >4.2</td><td align="center" valign="middle" >1.5 - 6.9</td><td align="center" valign="middle" >10.5</td><td align="center" valign="middle" >4.9 - 15.7</td><td align="center" valign="middle" >Umm Addebaa (n = 15)</td></tr><tr><td align="center" valign="middle" >-</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >0.25</td><td align="center" valign="middle" >0.33</td><td align="center" valign="middle" >19</td><td align="center" valign="middle" >18 - 20</td><td align="center" valign="middle" >4</td><td align="center" valign="middle" >1 - 9</td><td align="center" valign="middle" >Adams et al., 1959 ; Clarke et.al., 1966</td></tr><tr><td align="center" valign="middle" >4</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >0.25</td><td align="center" valign="middle" >0.1 - 0.5</td><td align="center" valign="middle" >18</td><td align="center" valign="middle" >5 - 20</td><td align="center" valign="middle" >4.5</td><td align="center" valign="middle" >1 - 12</td><td align="center" valign="middle" >Crustal acidic igneous rocks (after IAEA, 1979 and Boyle, 1982 ).</td></tr></tbody></table></table-wrap><p>The binary relations of eU, eTh, and eTh/eU may provide an indicator of the geochemical behavior of U and Th in the studied granitic samples. The plot of eU versus eTh illustrates that there are very strong positive relations between the variants in all of the rocks indicating their magmatic origin (<xref ref-type="fig" rid="fig8">Figure 8</xref>(a)). The eTh/eU ratio versus eU diagram <xref ref-type="fig" rid="fig8">Figure 8</xref>(b) shows that Umm Seleimat and Umm Addebaa samples show indirect relation reflect the uranium enrichment is strong where the eU content of Umm Seleimat ranges between 4.5 and 42.8 ppm with an average of 21.4 ppm, and the eTh content ranges between 6 and 28.5 ppm with an average of 51.73 ppm, whereas eU content of Umm Addebaa ranges between 4.9 and 15.7 ppm with an average of 10.5 ppm, and the eTh content ranges between 1.5 and 6.9 ppm with an average of 4.2, while Sikait and Umm El Kheran samples, uranium has a narrow range of values.</p><p>Result of the equation eU–(eTh/3.5) revealed that some of the measurements lie near the zero line, and this means that these samples have been originated from a late magmatic phase of magma very rich in radioelements with uranium concentration more than thorium. On the other side, the majority of measurements lie above the zero line indicating that the granites affected with hydrothermal solutions rich in uranium than thorium which indicates uranium addition (<xref ref-type="fig" rid="fig8">Figure 8</xref>(c) &amp; <xref ref-type="fig" rid="fig8">Figure 8</xref>(d)).</p></sec><sec id="s7"><title>7. Conclusions</title><p>1) The study area at Wadi El Gemal area consists mainly of ophiolitic m&#233;lange, cataclastic rocks, biotite granites and muscovite leucogranites. The studied muscovite granites are exposed in four exposures namely: Umm Seleimat, Sikait, Umm El Kheran and Umm Addebaa that belong to the younger granites of the Pan African rock units.</p><p>2) The muscovite leucogranites were intruded through the ophiolitic m&#233;lange and biotite granites with sharp contacts paralleling to the foliations of metasediments of ophiolitic m&#233;lange along the thurst fault.</p><p>3) Petrographically, muscovite granites are composed mainly of quartz, plagioclase of albitic composition, potash feldspar and muscovite. Monazite, zircon, allanite, garnet and opaques are accessory minerals. The presence of two feldspars suggests that the studied muscovite granites are mostly subsolvus and crystallized under high water pressure (Greenberg, 1981; Deer et al., 1992). Also, the presence of bent, kinked and gliding of plagioclase lamellae as well as high cracking and strongly undulatory quartz, all these features point to subsolidus deformation (Paterson et al., 1989). Such deformation should be the result of extensive regional thrusting (Greiling et al., 1987), to which the area had been subjected.</p><p>4) The REE compositions of the muscovite granites were determined using ICP-OES analytical method, the REE budget decreased from Umm Seleimat-Sikait exposures to Umm El Kheran-Umm Addebaa exposures as (514.5 - 495.6) to (195.9 - 197.7), respectively and the results consistently show the tetrad effect.</p><p>5) Similar M-type REE tetrad effect and strong Eu depletion are observed in whole-rock granitic samples. Consequently, the tetrad effect represents the integrated behavior of the entire members (=individual phases) of the rocks. The REE tetrad effect is accompanied by strong Eu negative anomalies.</p><p>6) Highly fractional crystallization leads to the enrichment of volatile, alkaline, rare earth elements and rare metals in residual melts which may result in a co-existing magmatic-hydrothermal system. The fluid/melt interaction in this system produces the REE tetrad effect in the melt and in the rock-forming and accessory minerals crystallizing from this melt. The minerals inherited the REE composition and distribution characteristics of the melt. Therefore, the interaction between granitic melt and coexisting volatile-rich fluid is the most important factor controlling the formation of REE tetrad effects in the studied muscovite granites.</p><p>7) Spectrometric investigation using binary diagrams revealed that the distribution of uranium and thorium in the studied granites increases gradually from Sikait, umm El Kheran, Umm Addebaa to Umm Seleimat. The binary relations of eU, eTh, and eTh/eU for all granitic exposures show strong positive relations exist with U and Th indicating their magmatic origin. Meanwhile, the result of mobilization equation proved that the studied granites samples have been originated from a late magmatic phase of magma very rich in radioelements.</p></sec><sec id="s8"><title>Conflicts of Interest</title><p>The author declares no conflicts of interest regarding the publication of this paper.</p></sec><sec id="s9"><title>Cite this paper</title><p>Shalan, A. S. (2022). Petrology, REE Geochemistry and Tetrad Effect of Some Muscovite Granites at Wadi El Gemal Area, South Eastern Desert, Egypt. Journal of Geoscience and Environment Protection, 10, 75-93. https://doi.org/10.4236/gep.2022.102006</p></sec></body><back><ref-list><title>References</title><ref id="scirp.115451-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Abd El-Naby, H. H., &amp; Frisch, W. (2002). 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