1 Introduction

7075 aluminum alloy is one of the most preferred materials in aerospace [1]. And, to enhance the alloy's mechanical qualities, some hardening procedures, such as T651 precipitation, are applied [2]. 7075 aluminum alloy, to which this process is applied, is used extensively in various industries such as aviation and automotive due to its low density and good mechanical properties [3, 4]. Drilling operations have an important place in many sectors and are also where this material is used [5]. It is estimated that the rate of drilling in total metal cutting operations is 36% when all machines are taken into account. This rate is approximately 40% for CNC machines, 25% for turning, and 26% for milling [6]. As drilling is done in a partially enclosed space, some problems may occur, for example, friction between the tool and the workpiece, high drilling temperatures, and challenges with chip removal [7]. The cut chips adhere to the cutting edges and chip evacuation channels of the drills used to drill aluminum materials. Thus, chip evacuation becomes difficult. This situation negatively affects the drilling process by causing the thrust force, torque, and spindle load to increase more than necessary. In addition, chips adhering to the drill cause the hole quality to deteriorate as they contact the hole simultaneously. Numerous experiments are conducted by altering the angles, coatings, and cutting parameters in drilling operations to remove these negative effects. Table 1 lists a few of these studies on drilling the alloy Al 7075.

Table 1 An overview of many investigations on drilling Al 7075 alloy

When the list is carefully examined, normal helical drills are generally preferred for drilling Al 7075 alloy. However, when the diameter of drills increases to drill larger holes, higher thrust forces occur due to the enlargement of the chisel edge in normal helical drills [8, 9]. Larger-diameter drills also have longer contact times with the workpiece. With the increased contact length, more workpiece material rubs and sticks to the cutting edges, margin, and chip evacuation channel. Due to the increased adhesion of more material to the cutter and the hole wall, the thrust force, torque, and spindle load are unusually increased. Furthermore, this results in increased energy consumption and the failure of the drilling operation. Even in some cases, the cutting edges and margins of the drill may become unusable due to the effect of adhering aluminum materials. In order to prevent this situation, peck drilling is performed. When the hole diameter increases too much, pre-drilling operations are required. This means extra time and costs in manufacturing. Alternatively, U drills with indexable inserts, without margin, and with a shorter contact length are used to overcome these disadvantages when drilling holes with a diameter larger than 12. It is stated that U drills have a market share of 53% in drilling tools and 8% in the total cutting tool sector [13]. However, there are very few studies on drilling holes using the U drill. When the studies using U drills are examined, steel materials are generally used as workpieces. These studies looked at how drilling parameters affected forces, surface quality, drill wear, vibration, and hole size, and they found that U drills generated higher-quality holes than standard helical drills [14, 15]. It has been found that using different geometry inserts has an effect on output parameters such as thrust force, torque, and surface roughness [16, 17]. Mathematical models are used to examine the impact of yield strength, forces, and cutting edge geometry on burr development [18]. The cutter wear, thrust force, torque, and surface quality of several cooling techniques, including dry, compressed air, emulsion, and MQL, were studied. It was discovered that emulsion cooling produced the least thrust force and surface roughness [19]. Compared to wet cooling, cryogenic liquid nitrogen (LN2) cooling has been found to reduce temperature, thrust, torque, surface roughness, and deviation from circularity and cylindricality [20]. Cylindricality and perpendicularity were estimated and optimized by gray relational analysis [21]. Investigating the effects of various insert coatings on thrust force, torque, and hole quality led to the conclusion that coating is a crucial factor [22, 23]. In a developed tool condition monitoring system using the current of spindle and axial feed motors, wear and hole diameter estimation have been made successfully [24]. Examining torsion, lateral regeneration chatter, and whirling in vibration and sound measurement findings led to the effective development of a mechanistic model [25, 26]. A specially made U drill was designed with an axially placed heat pipe. It has been determined that the heat pipes reduce the cutting temperature compared to dry machining [27]. The thrust force, torque, and temperature distribution of U drills were modeled using the finite element method. When the experimental and model data were compared, the torque was effectively modeled, but the anticipated thrust force had an inaccuracy of between 12 and 20 percent [28]. According to the studies in which steel group materials are drilled, different output responses are obtained due to the different mechanical and dynamic structures of the U drill and the normal helical drill. Therefore, further research on U drills and their effects on materials from different groups is required.

When the studies in the literature in which aluminum alloys were drilled with U drills were examined, a few and insufficient studies could be found. While drilling AlCuMgPb-F34 alloy with a U drill, it was determined that the burr value decreased to almost zero with the minimum amount of lubrication compared to dry machining [29]. Under carbon dioxide snow jet and emulsion machining conditions, AlMgSi1 alloy was compared in terms of burr height, surface roughness, diameter, and deviation from circularity. It has been indicated that the cooling methods are ineffective in reducing the deviation from the diameter and circularity of the holes in this material. But, it should not be drilled in dry conditions due to the high adhesion of aluminum to the cutter [30]. In some drilling, Al 7050-T7451 material is also mathematically modeled. The estimated thrust force and lateral force were compatible with the experimental result after the pre-drilling [31]. But for the Al 7075 material, an error of 38% in lateral forces and 60% in thrust forces occurred between the experimental results obtained from the pre-drilling and the estimation results. According to some reports, the U drill's low center cutting speed and the side edge of the central insert's close proximity to this area are to blame for the high mistake rates [32]. When the studies in which aluminum alloys are drilled with U drills are examined, a very insufficient amount of research has been done. Further studies need to be investigated by drilling aluminum alloys with U drills. Because the U drill has very different mechanical and dynamic properties from a normal twist drill. Actually, the U drill is a drill with two indexable inserts, one in the center and one on the periphery [16]. The central insert is the first to come into contact with the material and is responsible for centering the U drill. The peripheral insert provides that hole quality, which is achieved by cutting the part between the central insert and the hole diameter. Since the inserts are positioned at different distances from the U drill center, different insert geometry, grade, and balance angle can be used to balance the radial forces [25]. In addition, the chip evacuation channels designed for each insert have different geometric properties [13]. Due to the mentioned mechanical properties of the U drill, mathematical modeling and modeling with the finite element method led to high false force estimates (12–60%). It is important to make estimates that approximate experimental results by using different modeling techniques. Therefore, it is necessary to model and optimize the input parameters by experimentally examining the output responses such as thrust force, torque, and spindle load. The Taguchi-based gray relational analysis approach is one of the techniques used for modeling and optimization. The best experimentation sequence is chosen using this multi-criteria decision-making process based on all output replies. The optimal input parameters and percentage contributions are determined by the main effects plot and response tables. As a result, output responses are estimated and experimentally verified according to the most optimal input parameters. This method has been used efficiently in various studies. For example, optimization of cutting force, temperature, and surface roughness obtained from experiments with cooling method, feed rate, and cutting speed input parameters has been carried out [33]. In a different investigation, the input parameters of the drill type, feed rate, and cutting speed were used to optimize the thrust force, temperature, and burr height [34]. The goal of optimization is to choose the proper drilling parameters. Thus, it will be possible to increase hole quality, achieve optimum drilling forces, and have a more efficient drilling process [6]. Monitoring the drilling process involves using a variety of techniques or output responses. A dynamometer can be used to measure the thrust and torque data used to track the drilling process in real time. There is a correlation between the thrust force and torque signals, the surface delamination, and the surface integrity of the drilled hole, according to research employing standard helical drills [35, 36]. The relationship between the thrust force and vibration signals has been established, and the thrust force signals can be used to monitor the tool status [37, 38]. The relationship between the thrust force and torque values and the feed rate and cutting speed has been established [39]. Therefore, while analyzing output reactions like thrust force and torque, feed rate and cutting speed should be taken into consideration as input variables. A comparison of U drills with different properties apart from the mentioned input parameters is important in terms of production efficiency. In general, U drills have two cooling holes for in-hole cooling [14]. The manufacturer drills a third cooling hole even though some have the same length to diameter ratio because they believe the coolant will penetrate the cutting media more deeply. However, since the effect of this third cooling hole on the cutting process has not been examined before, it is a matter of curiosity and a gap in the literature. The cutting process dynamics may become unstable as a result of variations on the U drill body [17]. The additional coolant hole can alter the U drill's dynamic behavior by adding extra space to the body. Rigidities on the body can cause the drill to rotate backward, causing instantaneous elongation and shortening, resulting in vibrations [25]. Vibrations can cause unbalanced forces and adversely affect the cutting process [40]. Unstable thrust forces and torque values can cause inefficient use of machine power, premature wear of cutters, worsening of hole quality, and noises that are harmful to human health in the working environment [41, 42]. Due to the low frequency range of the dynamometer, some vibration mechanisms obtained with the U drill cannot be detected during the drilling process. In addition to thrust force, torque, and spindle load, audio signals from the drilling environment can be used with a microphone can be used in real time to examine the drilling process in more detail. Because it has been stated that it is more useful to examine sound signals in order to detect high frequency levels [43]. It is also possible to control the instantaneous strain of the spindle due to the variable torque with the spindle load during the drilling process [44, 45]. Further research in this area could lead to the development of more effective drilling tools for aluminum materials, which would enhance manufacturing processes and reduce production costs.

The aim of the current study is to optimize the effect of machining parameters on thrust force, torque, spindle load, and audio signals, which occur when drilling Al 7075-T651 material with U drills with different properties, by modeling with Taguchi-based gray relational analysis, one of the multi-criteria decision making methods. Additionally, the analysis of the impact of the additional cooling hole is the study's major contribution to the literature. A standard U drill with the same nominal diameter and the same length/diameter ratio will be used to experimentally compare the effects on the output responses of the third extra coolant hole drilled by the U drill manufacturer. So, in this paper, the effects of the length/diameter ratio of the U drills, as well as the effect of the extra coolant hole, on the output responses were compared. The influence of mechanical changes between U drills on dynamic thrust force, torque, spindle load, and audio signals was investigated. For modeling and optimization of output responses, a Taguchi-based gray relational analysis method was applied. Thus, optimal input parameters were determined. The information obtained can be useful in the research and product development stages of U drills, as well as in increasing the quality of the drilled parts and the drilling efficiency.

2 Materials and methods

2.1 Experimental material

Al 7075-T651 aluminum alloy was used for the experimental studies. The workpiece has dimensions of 40 × 40 × 40 mm. Hardness measurements and spectrum analysis were measured with at least three replications and averaged. The average hardness of the Al 7075-T651 material was determined at 172 Brinell. Table 2 shows the chemical composition of the material based on the spectrum analysis.

Table 2 Al 7075-T651 aluminum alloy chemical composition,% by weight

2.2 Machine tool used in experiments

In the experiments, a CNC milling machine tool named the Johnford VMC-850 was used. The machine has a spindle power of 7.5 KW, a maximum spindle speed of 8000 rpm, a measuring accuracy of 0.001 mm, and a Fanuc operating system. For the cooling process, the emulsion mixture was prepared with 5% semi-synthetic cutting fluid and water. The current investigation was carried out in accordance with the flow chart depicted in Fig. 1. Drilling tests were performed using the principles of through-hole and normal-hole drilling. The coolant was sprayed from the exterior and in one direction, as in the experimental configuration depicted in Fig. 2.

Fig. 1
figure 1

Process steps of the experimental study

Fig. 2
figure 2

The experimental setup

2.3 Cutting tool and cutting parameters

U drills with different length/diameter ratios (LD) (see Fig. 3) were used in the experiments. Totally, three different lengths of the U drill, such as 3D, 4D, and 5D, were preferred for experimental works. But tests were conducted for four types of the U drill. The fourth U drill is 4De, which has an extra cooling hole in the center. In Table 3, the size information of the U drills used in the experiments is given.

Fig. 3
figure 3

U drills used in experiments

Table 3 U drill dimensions used

In Fig. 4, there is dimension information for the used inserts. Typically, no two inserts are the same; both edge geometry and coating might change as they work at varying cutting rates and under varying load situations.

Fig. 4
figure 4

Inserts and sizes

The geometric parameters of the central and peripheral inserts of the U drill in this study differ, although both are uncoated carbide inserts appropriate for aluminum machining. XOET-ND 07T205 geometry was used as the central insert, and SPET-ND 07T208 geometry was used as the peripheral insert. Both inserts are of H01 quality. U drills of the same nominal diameter and inserts with the same specifications were used. A BT-40 VT-25 90 Veldon type tool holder was used to connect the U drill to the spindle. While determining the drilling parameters, the cutting tool catalog recommendations and literature information were taken into account. Table 4 lists the drilling variables.

Table 4 Drilling variables used in the experiments

Fz and Mz forces were measured using a Kistler 9272 dynamometer. Kistler’s 5070A was used as an amplifier. The samples were obtained at a rate of 100 Hz. The measured force and torque values, as well as the average numerical values, were obtained using the dynamometer's proprietary software, DynoWare. Spindle load values are taken from the control panel of the machine. The audio levels were taken from the cutting environment with the help of a LYM-333 microphone and recorded on the computer. The sampling amount of the audio signals was chosen as 44,100 Hz. The microphone position is fixed for all drilling experiments. All machines except the working CNC machine tool were turned off, and the audio signals were recorded by performing the experiments at a time when the ambient sound was minimal. The received audio signals were normalized, and then their root mean square (RMS) was taken to obtain the final experimental results.

2.4 Grey relational analysis

The optimal result of each output response may be different from each other. Thus, the selection of optimal drilling parameters becomes difficult. Multi criteria decision-making methods are used to overcome such problems [21]. One of these methods is grey relational analysis. It is widely used in studies published recently. In this study, Al 7075-T651 alloy was drilled with U drills with different LD ratios. A Taguchi-based grey relational analysis approach was utilized to identify the optimal drilling variables by multi-response optimization of the drilling process's thrust force, torque, spindle load, and audio signal outputs.

3 Experimental results and discussion

A total of 36 experiments (4 × 3 × 3) were carried out in order to investigate the thrust force (Fz), torque (Mz), spindle load (SL), and RMS value of the audio signal (SRMS) in relation to the drilling variables. The repeatability of randomized experiments is over 98%. Table 5 contains the test results.

Table 5 Experimental results

3.1 Evaluation of thrust force

Fz happens when the cutting tool enters the workpiece during drilling. In regular twist drills, the chisel edge is in charge of the most Fz, whereas in U drills, the central insert is in charge. Fz may result in excessive power consumption of the machine, premature dulling of the cutter, and deterioration of the quality of the drilled hole. As a result, it is critical to keep Fz under control [3]. The effect of drilling settings on Fz was explored in this work when drilling Al 7075-T651 material with a U drill. Table 5 shows the Fz values acquired as a result of the experiments. According to these results, the highest Fz value was produced utilizing the 4De U drill at the highest Vc and f values. The lowest Fz value was reached by combining the 5D U drill with the highest Vc and the lowest f. Figure 5 is obtained by considering the experimental results. Fz increased with the increase of f for all U drills when Fig. 5 is analyzed. This outcome is consistent with the literature [3, 7]. According to the literature, when f grows, the cutter penetrates the part faster; thus, as the chip cross-section increases, chip creation becomes more difficult, and Fz increases [3]. Although it was stated in some studies that Fz decreased with the increase of Vc [4], there was no significant decrease in the current study. The values showed little variation with the increase in Vc [8]. When all Vc is averaged, the average percentage increase in Fz is 13% for 3D, 22.1% for 4D, 14.4% for 4De, and 18.9% for 5D, with a 50% rise in f from 0.06 to 0.09 mm/rev. While f grew by 33.3% from 0.09 to 0.12 mm/rev, the average percentage of Fz increase was 9.7% for 3D, 9.6% for 4D, 7.7% for 4De, and 9.9% for 5D. Table 6 displays the Anova evaluation findings for Fz with a 95% confidence interval. The R2 value for the test was calculated at 97.6%. According to these results, the effects of drilling parameters on Fz were ranked as LD (76.45%), f (16.57%), and Vc (2.43%) according to p < 0.05 significance values. The LD was determined to be the most effective drilling parameter on Fz. It has also been found in similar studies that drill length and feed rate are important parameters for the thrust force [46]. It was concluded that other cutting parameters and their combinations did not have a linearly significant effect like the studies in the literature [8], since p > 0.05.

Fig. 5
figure 5

Variation of Fz depending on drilling parameters

Table 6 Anova results for Fz

Considering the mean Fz according to LD, Fig. 6 is obtained. The values were calculated by taking the average of nine experiments for each U drill. The 4De U drill with the extra coolant hole produced a 39.89% higher average Fz than the 4D U drill without the extra coolant hole. Figure 6 shows that a 5D U drill produced the lowest average Fz value, while a 4De U drill produced the greatest average Fz value. Compared to the 3D U drill, the 4D U drill produced higher average Fz values, while the 5D U drill produced lower average Fz values. 4De U drill produced the highest average Fz values compared to all U drills. The highest Fz values occurring in the 4De U drill are thought to be caused by the extra coolant hole shown in Fig. 7 blocking or disrupting the chip flow produced by the central insert. In Fig. 8, there is an example of swarf clogging or adhering to the coolant hole and the chip evacuation channel. After a drilling test at Vc 300 m/min and F 0.06 mm/rev, this sample image was obtained for the 4De U drill. Even after the drilling test, there are still chips clogging or adhering to the coolant hole and chip evacuation channel in the part where the central insert is. The cut chips' adhesion to the drill flutes restricts the exit path of the newly removed chips, resulting in a considerable increase in Fz [4]. The influence of the extra cooling hole on the Fz force is also seen in the dynamometer's real-time force data in Fig. 9. The chips removed by the central insert may have tried to enter the coolant hole, causing the chips to clog or stick in that area and thus increase the forces. It is also understood from the graphs obtained with the dynamometer that the forces decrease once the clogged or adhering chips are freed and that this process continues with constant repetition. The shift in force along the hole axis of the cutter increases the stress on the chip, resulting in intermittent chip production [47]. The increase in intermittent chip formation causes the periodic fluctuation amplitude to increase [48]. Especially when the graphs of 4De and other U drill bodies in Fig. 9 are examined, this fluctuation in Fz is clearly seen. The extra cooling hole in 4De caused the Fz signal amplitude to differ from the others. The signal amplitudes of the other U drills other than 4De are similar. The graph in Fig. 9 shows the change in Fz values for the 1 s drilling process after each U drill bit is fully engaged in the material. The amplitude and frequency of the graph curve formed by the Fz values obtained for the 4De U drill are distinctly different from the graph curves obtained for the other U drills. For the 4De U drill, the low frequency and high amplitude are thought to be caused by chips trying to enter the coolant hole. In addition, it is stated that torque values may cause the drill to turn backwards and open the chip grooves, thus increasing the thrust forces [49]. In the current study, it is thought that the extra cooling channel in the U drill body may cause this phenomenon by creating an extra space.

Fig. 6
figure 6

Average Fz values according to LD ratio

Fig. 7
figure 7

Coolant holes of U drills

Fig. 8
figure 8

Chips accumulated in the 4De U drill after drilling

Fig. 9
figure 9

The first 1 s that the U drill bit is fully engaged

3.2 Evaluation of torque

According to the findings of the current study's experiments, the highest average Mz value of 651.8 N cm was obtained at the lowest Vc and highest f values by using a 4D U drill. The smallest value, 325.44 N cm, was obtained using a 5D U drill at the largest Vc and the smallest f value. Figure 10 depicts the effect of drilling settings on Mz for all U drills as a three-dimensional graphic. According to the obtained visuals, Mz values grew as f increased for all bodies. This conclusion was also obtained in several studies published in the literature [7]. Although it was stated in some studies that Mz values decreased with the increase of Vc [10], a similar situation did not occur in the current study. When the Anova test results for Mz are examined, it is clear that the most effective parameter is f. The images for all U drill bodies produced very identical results. According to the Mz values calculated by taking the average of nine experiments for each U drill, the 4De U drill (477.7 N cm) with an extra coolant hole produced a 3.26% lower average Mz than the 4D U drill (493.8) without an extra coolant hole. When all Vc averages were considered, the mean percentage of Mz increase was estimated as 42.6% for 3D, 39% for 4D, 33.2% for 4De, and 38.8% for 5D, with a 50% rise in f value from 0.06 to 0.09 mm/rev. While f grew by 33.3% from 0.09 to 0.12 mm/rev, the average Mz increase percentage was found to be 15.7% for 3D, 23.7% for 4D, 25.8% for 4De, and 26.3% for 5D. An Anova test for Mz was performed at a 95% confidence interval. The R2 value for the test was calculated at 98.84%. Calculation results are given in Table 7. According to Table 7, f was 96.04% effective on the Mz output response, according to p < 0.05 significance values. In accordance with the literature, the most effective cutting parameter for Mz was the input parameter f [46]. It was concluded that other cutting parameters and their combinations did not have a significant effect as p > 0.05. It was determined that Vc, LD, and combinations were not effective on torque since the insert positions were similar in all U drills.

Fig. 10
figure 10

Effect of drilling parameters on Mz

Table 7 Anova results for Mz

The f value, which is one of the input parameters for the Anova test, has a very high effect on the Mz output response. It is clear that the LD, which is highly effective on Fz, is not effective on Mz. So different U drill sizes have no effect on Mz for drilling aluminum material. When Fig. 11 is examined, the change in Mz is seen depending on time. It can be seen that all U drill bodies fluctuate at the same rate at the start of drilling. Then, short-term, sudden increases and decreases in Mz draw attention in U drills other than 4De U drills. According to the literature, it is stated that Mz rises and falls momentarily as the chips stick to the chip evacuation channel and then break off [17]. However, if attention is paid to the Mz graph for the 4De U drill, it has consistently moved between the same Mz values from the beginning of the hole to the end. However, when looking at the graph for the other 4D U drill with the same LD ratio, instant rises and falls are remarkable. Although the extra cooling hole opened into the U drill body causes a significant increase in Fz, it can be said that it causes more stable values when Mz is taken into account. With the increase in f, sudden Mz increases are seen in the 4De U drill graph. However, these increases were not as extreme as in other U drills. The cutting speed increases as the drill moves from the center to the periphery. Since the extra coolant hole for the 4De U drill is in the center, it is thought that the clogging or adhesion of the chips has a greater effect on the Fz value but less on the Mz value. In other words, it is determined that while the chips are clogging or adhering to the chip evacuation channel where the central insert is located, less smearing occurs in the chip evacuation channel where the peripheral insert is located. Therefore, while the Fz values were higher for the 4De U drill, the Mz values were similar to the other U drills.

Fig. 11
figure 11

Change of Mz with time

3.3 Evaluation of spindle load

In one aspect, the SL found on CNC machines shows how hard the spindle is forced during machining in real time. Therefore, SL provides the opportunity to determine the appropriate drilling parameters at the beginning of the work or to intervene in the drilling parameter values used during the operation of the machine. According to the results of the current study's experiments, the maximum SL value of 120% was reached utilizing the 4D U drill at the highest Vc and f values. The smallest value, 40%, was obtained at the middle Vc and the smallest f value by using a 4De U drill. According to Fig. 12, which depicts the effect of drilling parameters on SL, when f increases, SL tends to grow. The effect of increasing Vc on SL was more uncertain. According to the SL values calculated by calculating the average of nine experiments for each U drill, the 4De U drill with an extra coolant hole (56.11%) produced a 41.28% lower average SL value than the 4D U drill without an extra coolant hole (95.56%). The lowest SL was obtained with a 4De U drill. Despite a 50% increase in f from 0.06 to 0.09 mm/rev, the mean SL increase percentage in all Vc was computed as 33.4% for 3D, 24.7% for 4D, 7.8% for 4De, and 13.3% for 5D. While f grew by 33.3% from 0.09 to 0.12 mm/rev, the average SL increase percentage was 9.8% for 3D, 20.7% for 4D, 14.1% for 4De, and 8.8% for 5D. An Anova test for SL was performed at a 95% confidence interval. The R2 value for the test was calculated at 97.4%. Calculation results are given in Table 8. According to the significance values of p < 0.05 according to Table 8, LD (53.33%), f (21.27%), and Vc (8.95%) were effective on the SL output response, respectively. The most effective drilling parameter for SL was the LD ratio. Since all cutting parameters and combinations were p < 0.05, it was concluded that all of them had a linearly significant effect on the result. This finding is consistent with other research in the literature [50].

Fig. 12
figure 12

Effect of drilling parameters on SL

Table 8 Anova results for SL

Considering the Mz graphics in Fig. 11 and the SL values calculated here, the drilling of Al 7075-T651 alloy with a 4De U drill resulted in a very stable result. It is interesting that while Fz values were higher for 4De, the lowest values were found for SL values. Because it is stated in various studies that higher thrust forces cause more power consumption and forced [14]. In U drills, the chip thickness acting on each insert changes due to the axial runout of the central and peripheral inserts and their geometric structure [31]. We can mention that while clogging and/or sticking occurs in the extra coolant channel in the center of the 4De U drill, less clogging or adhesion occurs in the chip evacuation channel where the peripheral insert is located. As a result of this, the cutting speed value increases as you go from the center of the drill to its circumference; we can say that it does not cause an increase in Mz since the speed is zero in the center.

3.4 Evaluation of audio signal

An audio signal is a combination of sounds from different sources. These sources consist of torsional-axial chatter, lateral chatter, rotational vibrations, coolant flow, evacuation of chips, background noises in the workshop, the noise of the spindle and gearboxes, and the noises from the hydraulic and lubrication systems of the machine tool [26]. In this study, vibration-induced audio signals were taken into account. When a cutter starts to drill a material, dominant sound waves are emitted into the environment. These sounds give us information about the dynamics of the cutting process, such as poor surface quality, dull cutting tools and loud noise [42]. Especially the sounds that occur in U drills can tell us about vibration and its causes. In one study, it was stated that the detection of vibrations above 1000 Hz with a dynamometer was insufficient, but a microphone was a useful device for detecting chatter [43, 51]. When similar studies in the literature are examined, it has been stated that the sampling frequency of the microphone should be higher than 40 kHz in experiments using U drill [26], while higher sampling frequencies are preferred in some [52]. The influence of drilling parameters on audio signals should be investigated in this regard. Instead of evaluating the highest values in audio signal analysis, the RMS value of the signal is frequently compared [53]. \({x}_{\mathrm{RMS}}\), which is the RMS value of an \(x(n)\) signal, is calculated by considering Eq. 1. In the RMS computations, N is the number of samples [54].

$${x}_{\mathrm{RMS}}=\sqrt{\frac{1}{N}\sum_{n=1}^{N}{x}_{n}^{2}} $$
(1)

The highest SRMS value was obtained at medium Vc and the lowest f value when the 4De U drill was used, while the lowest SRMS value was obtained at middle Vc and the highest f value when the 3D U drill was used, as shown in Table 4. The effect of drilling parameters on SRMS is given in Fig. 13. According to this fig, the highest SRMS values are obtained by using the 4De U drill. The lowest values were obtained by using the 3D U drill. When the graphs are inspected, the SRMS tends to grow as f increases. On the other hand, the effect of the increase in Vc was uncertain. According to the SRMS values calculated by taking the average of nine experiments for each U drill, the 4De U drill with an extra coolant hole (0.1405 Pa) produced a 95.17% higher average SRMS value than the 4D U drill without an extra coolant hole (0.072 Pa). According to this result, it can be said that the extra cooler hole opened in the U drill causes vibration and increases the sound levels. An Anova test for SRMS was performed at a 95% confidence interval. The R2 value for the test was calculated at 96.11%. Calculation results are given in Table 9. According to the significance values of p < 0.05 according to Table 9, LD (87.53%) and f (2.89%) were effective on the SRMS output response, respectively. It was concluded that other cutting parameters and their combinations did not have a significant effect in accordance with the literature as p > 0.05 [55]. The most effective drilling parameter for SRMS was the LD.

Fig. 13
figure 13

Effect of drilling parameters on SRMS

Table 9 Anova results for SRMS

As in Fig. 14, different amplitude sounds occur in the time domain with the drilling process performed by using different U drills. In order to make meaningful inferences from these data, the frequency domain is passed. Thus, vibrations produced by the use of U drills can be distinguished. For the transition to the frequency domain, the fast Fourier transform (FFT) method is used. Figure 15 depicts the frequency domain graph created as a result of the transformation in this investigation. When examining Fig. 15, 6313 Hz for 3D U drill, 79.47 Hz for 4D U drill, 4810 Hz for 4De U drill, and finally 715.4 Hz for 5D U drill are the dominant frequencies, respectively. The amplitude of the frequency obtained with the 4De U drill was very high compared to the other U drills. This means that the vibrations obtained with the 4De U drill are higher than the others. As stated in the previous sections, it can be said that the third extra cooling hole opened in the 4De U drill body is the cause of this result. It can be said that the extra coolant hole opened on the U drill body causes more vibrations by causing dynamic instability in the drilling process. The differences in Fz and Mz caused by each insert are said to induce torsional and axial vibrations [25]. It has been stated that torsional rigidity determines how much the drill can rotate under the cutting torque, while the torsional stiffness decreases with the effect of the cooling holes drilled into the drill [56].

Fig. 14
figure 14

Time domain representation of audio signals (300 m/min, 0.12 mm/rev)

Fig. 15
figure 15

Display of audio signals in the frequency domain (300 m/min, 0.12 mm/rev)

3.5 Insert, disc and chip images

Figure 16 shows the rake and flank faces of the central and peripheral inserts for Vc 300 m/min and f 0.12 mm/rev. Smearing occurred on the rake and flank faces of both the central and peripheral inserts as a result of drilling operations done with all U drills. When looking at the flank faces of the central inserts with 4De and 5D U drills, there are very few friction marks marked in a red circle. It is considered that this result may have occurred due to the effect of scratching [57]. Furthermore, the edge width influenced by cutting is higher on the flank sides of both the central and peripheral inserts utilized with the 4De U drill. It is thought that this result may have been achieved by the fact that the cutter was exposed to more vibration by being vulnerable to dynamic loads due to the effect of the extra cooling hole opened in the body [56]. As a result of drilling through the hole with a U drill, a disc is generated at the hole's exit. All discs were collected within the scope of this experiment. The evolution of the disk images for all U drills is similar. When the images in Fig. 17 were evaluated, the best stable cutting result was found with a 3D U drill at 200 m/min and 0.06 mm/rev drilling parameters. There are no chatter marks on the disc, and it is very smooth [13]. In parallel with the increase of f, the chatter marks on the disc increase. With the increase in Vc, the chatter marks slightly changed. When Fig. 18 is examined, there is the evolution of the chips obtained during the drilling process. All of these images were obtained with a 3D U drill. Chip images obtained with other U drills are similar to these images. When the images are examined, there are typical U drill chips at 200 m/min–0.06 mm/rev. Long chips were generated by the peripheral insert, while short chips were generated by the central insert. With the increase of f, the chips became shorter and irregular. With the increase of Vc, the wavelength of the chips obtained with the peripheral insert shortened and the chips began to jam.

Fig. 16
figure 16

Used insert images (300 m/min, 0.12 mm/rev)

Fig. 17
figure 17

Examples of disc formed by 3D U drill

Fig. 18
figure 18

Typical examples of chips cut by a 3D U drill

3.6 Multiple optimization with Taguchi based grey relational analysis

At this stage of the study, all of the output responses obtained when drilling Al 7075-T651 alloy using a U drill were optimized according to the drilling parameters. First, each output response is normalized. The “smaller is better” approach for normalization is preferred for all output responses. In the next step, the coefficients of each output response were determined and the grey relational grades (GRG) were calculated. The higher the GRG value, the closer the result of that experiment is assumed to be to the optimum result. By determining the GRG values, the optimum test sequence was determined. Table 10 shows the outcomes of the trials and computations.

Table 10 Grey relational analysis results

Anova was estimated for the GRG values using the "bigger is better" approach. The mean value of GRG was determined using the response table for GRG in Table 11. As a result, the initial cutting condition for Vc was determined to be level 1, level 2 for f, and level 3 for LD. Table 12 displays the calculated ANOVA results. According to the 95% confidence interval Anova results, f (57.52%) and LD (34.05%) were effective on GRG. Figure 19 shows the main effects plot for GRG according to the S/N ratios. The most successful drilling settings on GRG were identified to be 3D U drill for LD, 250 m/min for Vc, and 0.06 mm/rev for f, according to this graph.

Table 11 Response table for GRG
Table 12 Anova results for GRG
Fig. 19
figure 19

Main effects plot for GRG

3.6.1 Verification of GRA optimization

The verification of the derived optimum parameters is the final stage of Taguchi-based grey relational analysis. Table 13 shows the outcomes of the validation studies. While the initial GRG value was 0.637, the estimation result was calculated as 0.798. The GRG value obtained as a result of the validation experiments was 0.803. Estimated and experimental results were higher than the initial cutting conditions. In addition, the correlation between the estimated and experimental results is quite high. According to Table 13, an improvement of 0.166 was achieved in the GRG. The improvement in the percent GRG value was calculated at 26.06. In the study of Yağmur [33], 21.87% in GRG, Wang et al. [58] achieved an improvement of 13.88%. The value obtained in the GRG with the current study is quite compatible with the studies in the literature.

Table 13 Results of validation experiments

4 Conclusion

The effects of cutting parameters determined in this study on drilling were compared with the Fz and Mz obtained from the dynamometer, the SL from the CNC machine tool, and the RMS value of the sound information obtained with a microphone. Each output response is interpreted using the Anova test and graphs. Similarities and differences between the data were trying to be determined. Then, taking into account all output responses, optimal input factors were attempted to be discovered via multi-response optimization. For multiple response optimization, a Taguchi-based grey relational analysis method was applied. Obtained results are listed below.

  1. 1.

    While the ratio of length to diameter was the most effective parameter on Fz, Mz, and SRMS, the feed rate was the most effective parameter on SL. The Fz and Mz values grew as the feed rate increased. In drilling operations, it is critical to use the suitable U drill.

  2. 2.

    While the extra coolant hole caused an increase in Fz and SRMS values, it caused intermittent chip formation and a decrease in SL values. On the Mz, it did not cause a remarkable change due to its location close to the center. Users who want to avoid the negative effects of thrust force and excessive noise should not choose U drills with extra cooling holes.

  3. 3.

    When the images of the inserts as a result of the drilling process were examined, adhesion was found on the chip surfaces of almost all inserts. Considering the flank surfaces of the inserts used in the U drill with the extra coolant hole, the edge width affected by cutting is the highest. When a U drill with an extra coolant hole is used, the dynamic stiffness decreases, causing more chatter and thus an increase in the area affected by the cutting.

  4. 4.

    Considering the chips obtained as a result of drilling, with the increase in f value, the chip lengths were shortened and irregular, compacted chips were obtained.

  5. 5.

    The Anova analysis for each experimental output response revealed that the length/diameter ratio of U drills had the greatest effect on thrust force (76.45%), spindle load (53.33%), and audio signal (87.53%), but had no effect on torque.

  6. 6.

    The 4De U drill with the extra coolant hole produced 39.89% more thrust force, 95.17% more audio signal value, 41.28% less spindle load, and 3.26% less torque value than the 4De U drill without.

  7. 7.

    The calculated GRG value for the experimental output responses Fz, Mz, SL, and SRMS for the beginning parameters Vc1 f2 LD3 is 0.637, and the predicted GRG value for the optimal drilling parameter determination is 0.798. The GRG value of the output responses for the experimental drilling parameters Vc2 f1 LD1 determined as a result of the applied Taguchi-based gray relational analysis was found to be 0.803. Accordingly, with the statistical optimization method applied, a 26.06% improvement was achieved in the GRG value compared to the initial parameters. As the most optimal input parameter, the LD ratio was determined to be Vc 250 m/min, f 0.06 mm/rev, and the 3D U drill.

  8. 8.

    As a result of optimization with Taguchi-based gray relational analysis, an improvement of 16.41% in Fz and 36.56% in Mz was achieved.