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Fig. 1.
Table 1.
References [1] Alshibly, H.
Internet Research, 21(4), 479-503
Information Systems Research, 13(1), 50-69

Fig. 1 represents effective density of Al2O3/water nanofluid with different particle volume fractions.
Table 1 represents the effect of particle concentration on effective viscosity.
Lett. 479 (2009), 264-269
Fund. 1 (1962) 187-191
(Hindawi Publishing Corporation), 172085 (2010) 1-4

The particle size is generally from 1 to 100 nm.
Table 1.
Reference [1] Ma X Y and Chen H B: China Medical Herald.
Vo5. 1-6 (2002)
Vo201. 479-484 (2018)

A (1 x 1) cm clear glass ground edges microscope slides (1.0-1.2) mm in thickness and high purity metallic Zn powder (1 gm, 99.99%, Japan) were used as a substrate and source material, respectively.
Figure 1.
Table 1.
References [1] T.
Alloys Compd. 479 (2009) L11-L14

The chemical methods using benzalkonium chloride (Fig. 1 E) and water:ethanol 1:1 (v/v) are the least effective methods; in these surfaces, a lot of biological remains are observed on the granite.
The most characteristic peaks of the crust are those around 1200-1700 cm-1, assigned as ester groups (1200 cm-1), C-N functional group (1300 cm-1), C=C link (1500-1650 cm-1, also considered indicative of chromophores of chlorophyll following [17]), ester, aldehyde and ketone groups (1600 cm-1) and C-H group (2890 and 2920 cm-1).
Table 1.
References [1] T.
El-Gohary: Experimental tests used for treatment of red weathering crusts in disintegrated granite – Egypt, Journal of Cultural Heritage 10 (2009) pp. 471-479

Fig. 1.
References [1] M.E. de A.
Technol. 87 (2012) 1-14
Part 1 43 (2004) 5455-5464
Maensiri, Fabrication and magnetic properties of electrospun copper ferrite (CuFe2O4) nanofibers, Solid State Sci. 11 (2009) 479-484

The minimum ferrite grain size obtained by the new TMCP is less than 1µm.
In Japan, the study of this process started by Kudo [1] in 1974.
References [1] H.
Aoki: Annals of CIRP, 51/1(2002), p.227 [10] K.
Kondo: Material Science Forum, Vols.475-479 (2004), p.245 [15] K.

coil core Fig. 1.
B = 0 mT f = 0 s-1 B = 40 mT f = 8 s-1 B = 60 mT f = 12 s-1 Fig. 4.
flux density 30 mT 12 s-1 40 mT 12 s-1 50 mT 12 s-1 60 mT 12 s-1 0 mT 0 s-1 field frequency beam power (cw-CO2-Laser) = 5 kW welding speed = 7.8 m/min shielding gas = 20 l/min He coaxial coil 50 mT 0 s-1 50 mT 5 s-1 50 mT 10 s-1 50 mT 15 s-1 Fig. 5.
In: Trans. of JWRI, 7 (1978) 1, 111-127
B, 12B (1981) 9, 479-486

Suo 1,a and Z.Q.
The trends of SFLP are shown in Fig.1.
The formulation of the DFLP is given below. 1 ( 1) 1 1 Min DFLP = SFLP( ) T T t t t t t A − + = = +∑ ∑ (1) where t is the number of periods in DFLP; At(t+1) is the rearrangement costs between each pair of adjacent periods; and T is the total number of periods in the whole period horizon.
References [1] A.R.
PROD.RES., Vol.25 (1987) No.4, pp.479

Table 1.
References [1] J.
Technol., vol. 35, no. 5–6, pp. 468–479, Oct. 2006
Technol., vol. 110, no. 1, pp. 1–9, Mar. 2001
Technol., vol. 170, no. 1–2, pp. 11–16, Dec. 2005.