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This fact is normally not considered as a problem in most industries [1].
Table 1 - Throughput time for the identification of nuisance alarms Alarm Description Number of announced alarms Number of announced alarms < 5s <5s / Announced (%) Throughput time (s) Mean Minimum Maximum Standard deviation Low flow 16 15 93,8 2,3 1 4 0,82 High temperature (liquid) 15 14 93,3 2,3 1 4 0,93 Solenoid valve open - problem 15 3 20,0 3,3 2 4 1,15 Setpoint 11 2 18,2 3,5 3 4 0,71 Pump start - problem 9 1 11,1 4,0 4 4 0,00 Solenoid valve close - problem 8 1 12,5 4,0 4 4 0,00 High Pressure in the tank 5 4 80,0 3,0 2 4 1,15 High Level in the tank 3 0 0,0 0,0 0 0 0,00 Emergency 3 0 0,0 0,0 0 0 0,00 Command off 2 0 0,0 0,0 0 0 0,00 Circuit breaker off - Pump 2 0 0,0 0,0 0 0 0,00 High temperature in the pump 1 0 0,0 0,0 0 0 0,00 The Heuristic Miner algorithm was employed in order to identify the links between the events, which consists of a process mining algorithm that makes use of a statistical approach for mining the dependence relation between the activities represented by
References [1] E.
Aalst, Process Mining Applied to the Test Process of Wafer Steppers in ASML, IEEE Transactions on Systems, Man, and Cybernetics - Part C: Applications and Reviews, Vol. 39, No. 4, pp. 474–479, 2009
Elsevier, Vol. 11.2010, 1, pp. 17-41, 2010

Rhodamine b has the molecular formula C₂₈H₃₁N₂O₃Cl with its molecular mass of 479 gmol-¹ [2].
Next, 1 ml of 80% Hydrazine was added to the mixture and stirred at 600 rpm for 1 hour.
Fig.1.
Table 1.
Inorganic and Nano-Metal Chemistry, 1-9

Fig. 1.
Table 1.
Other peaks were noted at 2726 cm−1, 2904 cm−1 and can be associated with 2D and D+G bands, respectively.
References [1] W.
Abdel-Rehim, Polyacrylonitrile / graphene oxide nanofibers for packed sorbent microextraction of drugs and their metabolites from human plasma samples, Talanta. 201 (2019) 474–479

The strength of magnetic field is applied normal to the flow as shown in Fig.1.
Tables 1 exhibited the variations of friction factor and Nusselt number for Carreau fluid.
References [1] S.
Ain Shams Engineering Journal, 5(1) (2014) 293-304
Propulsion and Power Research, 5(1) (2016) 70-80

Table 1 Properties of composite Portland cement.
The test mold and pads are shown in Fig. 1.
References [1] X.P.
Mater. 41 (2013) 1–8
Eng. 479 (2019) 012053

Introduction Electromagnetic absorption (EMA) materials have attracted extensive attention for electromagnetic protection and stealth [1-3].
Fig. 1 shows SEM images of spherical carbonyl iron powder and flake carbonyl iron powder under different ball grinding time.
It can be seen from Fig. 1(a) that the SCI particles are approximately spherical, with a diameter of about 1-6 µm.
References [1] J.
Chen, Preparation of rGO/PVA/CIP composites and their microwave absorption properties, Journal of Magnetism and Magnetic Materials. 479 (2019) 337-343

It can be concluded that increasing the ratio of DAHP/urea from 2/1 to 4/1 has a negative effect on the flame retardant properties.
Fig.1.
Fig. 2 shows the test results of samples of tapestry fabric treated with flame-retardants in the ratio DAHP/urea = 3/1.
References [1] P.J. 
Emen, The use of sol-gel method for obtaining fire-resistant elastic coatings on cotton fabrics, Materials Science Forum, 1038 (2021) 468–479

The procedure is illustrated in Figure 1.
Table 1 repots the investigated values of p and d parameters.
References [1] Karbasian, Hossein, and A.
Journal of the Chinese Institute of Engineers 42.6 (2019): 479-487
No. 1.

The investigated workpiece material is a Ti6Al4V alloy (chemical composition in Table 1).
Machining parameters for turning tests Factors No. of levels Values Cutting tools 3 Inserts “S”, “L”, “LC” Cutting speeds (Vc) 2 40 and 50 [m/min] Feed rates (f) 2 0.2 and 0.3 [mm/rev] Depth of cut (b) 1 1.2 [mm] Cutting fluid 1 Hocut 795/I at a concentration of 5% and a flow rate of 2 [l/min] The ANOVA has been used as the statistical method to determine if each investigated factor significantly affects the measured responses.
Mechanical characterization of material Tensile Strength TS [MPa] 933.67 Elongation at fracture [%] 18.01 Yield Strength YS0.2% [MPa] 866.94 Post-fracture reduction of area [%] 46.22 Fig. °1.
References [1] S.
Mativenga, Wear mechanisms analysis for turning Ti-6Al-4V—towards the development of suitable tool coatings, The International Journal of Advanced Manufacturing Technology 58 (2012) 479-493

The dimensions of the sheath are 1, and 1.2mm in inner diameter, 1.4mm in outer diameter, and 300, 450, 600mm in length.
Time Delay(㎲) according to UTS length Temperature (℃) (1)1050 ㎜ (2)990 ㎜ Notch position : 500㎜ (3)918 ㎜ Notch position : 150㎜ (b) 604 459 455 225 435 71 (c) 818.7 461 457 226 437 72 (d) 1000 463 461 227 439(+4) 73(+4) (e) 1216 465 462(+2) 228(+2) 441 74 (f) 1400 477 463 229 443(+2) 75(+2) (g) 1600 479 464 230 445 76 (h) 1800 481(-1) 466(+1) 231(+1) 447(+1) 76(+1) (i) 2400 483 467 (+1,+2) 232 449, 450 76, 77 (a) Normal Tem.; 20 441 433 425 70 Title of Publication (to be inserted by the publisher) Fig. 3.
At the third step, the sensor rod was applied to measure the in-vessel temperature of the LaVa experiment, but the measurement 0 1 0 0 0 0 2 0 0 0 0 3 0 0 0 0 4 0 0 0 0 5 0 0 0 0 - 1 . 0 - 0 . 5 0 . 0 0 . 5 1 . 0 4 6 3 . 0 µ s Amplitude T i m e u t s 1 - 1 0 5 7 0 1 0 0 0 0 2 0 0 0 0 3 0 0 0 0 4 0 0 0 0 5 0 0 0 0 - 1 . 0 - 0 . 5 0 . 0 0 . 5 1 . 0 4 6 5 µ s Amplitude T i m e u t s 1 - 1 2 1 6 0 1 0 0 0 0 2 0 0 0 0 3 0 0 0 0 4 0 0 0 0 5 0 0 0 0 - 1 . 0 - 0 . 5 0 . 0 0 . 5 1 . 0 4 1 0 µ s 1 0 5 0 m m F i r s t E n d S i g n a l Amplitude T i m e u t s 1 - N o r m a l - T e m . 0 1 0 0 0 0 2 0 0 0 0 3 0 0 0 0 4 0 0 0 0 5 0 0 0 0 - 1 . 0 - 0 . 5 0 . 0 0 . 5 1 . 0 4 5 9 µ s Amplitude T i m e u t s 1 - 6 0 0 0 1 0 0 0 0 2 0 0 0 0 3 0 0 0 0 4 0 0 0 0 5 0 0 0 0 - 1 . 0 - 0 . 5 0 . 0 0 . 5 1 . 0 4 7 7 µ s Amplitude T i m e u t s 1 - 1 4 3 1 0 1 0 0 0 0 2 0 0 0 0 3 0 0 0 0 4 0 0 0 0 5 0 0 0 0 - 1 . 0 - 0 . 5 0 . 0 0 . 5 1 . 0 4 8 3 µ s
Amplitude T i m e u t s 1 - 2 3 1 4 (i) (d) (c) (b) (a) (e) 0 1 0 0 0 0 2 0 0 0 0 3 0 0 0 0 4 0 0 0 0 5 0 0 0 0 - 1 . 0 - 0 . 5 0 . 0 0 . 5 1 . 0 2 3 2 µ s 4 6 6 µ s Amplitude T i m e u t s 2 - 2 3 1 4 0 1 0 0 0 0 2 0 0 0 0 3 0 0 0 0 4 0 0 0 0 5 0 0 0 0 - 1 . 0 - 0 . 5 0 . 0 0 . 5 1 . 0 7 4 µ s 4 4 1 µ s Amplitude T i m e u t s 3 - 1 2 1 6 0 1 0 0 0 0 2 0 0 0 0 3 0 0 0 0 4 0 0 0 0 5 0 0 0 0 - 1 . 0 - 0 . 5 0 . 0 0 . 5 1 . 0 7 4 µ s 4 3 9 µ s Amplitude T i m e u t s 3 - 1 0 5 7 0 1 0 0 0 0 2 0 0 0 0 3 0 0 0 0 4 0 0 0 0 5 0 0 0 0 - 1 . 0 - 0 . 5 0 . 0 0 . 5 1 . 0 7 2 µ s 4 3 5 µ s Amplitude T i m e u t s 3 - 8 1 8 0 1 0 0 0 0 2 0 0 0 0 3 0 0 0 0 4 0 0 0 0 5 0 0 0 0 - 1 . 0 - 0 . 5 0 . 0 0 . 5 1 . 0 7 2 µ s 4 3 7 µ s Amplitude T i m e u t s 3 - 6 0 0 0 1 0 0 0 0 2 0 0 0 0 3 0 0 0 0 4 0 0 0 0 5 0 0 0 0 - 1 . 0 - 0 . 5 0 . 0 0 . 5 1 . 0 N o t c h s i g n a l E n d s i g n a l 7 2 µ s 4 3 5 µ s 1 5 0 m m 9 1 8 m m
References [1] G.