Research Article  Open Access
Optimization of Electrostatic Force System Based on Newton Interpolation Method
Abstract
The measurements of micro/nanoforces are of great importance in both science and engineering. We developed a traceable system for micro/nanoforces based on electrostatic force using two electrodes. Noises (creep, ground vibration, and airflow) are one of the limitations for force resolution. The forces are distorted by noise and cannot be measured accurately. Although ABA method can be used to eliminate linear creep, it is invalid for nonlinear noise. In this paper, a new method known as the Newton interpolation method (NIM) has been adopted in capacitance gradient and the calibration of cantilever stiffness to reduce the effect of nonlinear noise. The results show that the capacitance gradient, with a relative standard deviation of 0.004%, is stable and has good repeatability. The stiffness of cantilever was measured using electrostatic force. The typical value of stiffness ranged from 5.1 to 48 N/m. The relative standard deviation was small, i.e., less than 0.6% owing to Newton interpolation method. These results show that our system is very stable and repeatable. This research may assist in the designing of force measurement systems based on electrostatic force.
1. Introduction
The measurement of micro/nanoforces is of great importance in both science and engineering [1–15]. It is useful in the fields of precision instruments, biology [16, 17], magnetic field distributions [18], distance measurement [19], and tribological properties of materials [20–23]. Atomic force microscope (AFM) is one of most popular microforce measurement instrument. Being the key component of AFM, the cantilever must be calibrated to measure microforces accurately. A considerable number of researches have been done on the calibration of cantilevers. The National Institute of Standards and Technology (NIST) in the USA [2], the National Physical Laboratory (NPL) in the United Kingdom [3], the Center for Measurement Standards (CMS) in Taiwan [7, 8], and the PhysikalischTechnische Bundesanstalt (PTB) in Germany [4] have all developed traceable systems that could be used for the calibration of cantilevers.
In this study, the stiffness of AFM cantilever is calibrated by an electrostatic system [2, 9] using the forcedisplacement curve. In general, for microforce measurements, the signal would be drowned in noise and cannot be measured accurately. The traditional force measurement systems, such as resistance strain gauge and piezo electric sensor, are vulnerable to environmental disturbances. Although linear noise may be reduced by the ABA method, higher order noise cannot be reduced. To reduce vibrations, the system at NIST was built 12 m underground. At the PTB in Germany, the nanoNewton force metrology group designed an aluminium plate pendulum; however, the resolution of the setup was constrained by noise. In order to reduce this noise, PTB set up two identical systems. This setup has a resolution of 10^{−12} N and can measure forces less than 10^{−5} N [6]. In this paper, the Newton interpolation method (NIM) is proposed to reduce the effect of noise in both the capacitance gradient determination and cantilever calibration.
2. The Electrostatic Force System
A pair of coaxial cylindrical capacitors are used to generate the electrostatic force, as shown in Figure 1. The system is placed at the centre of a 1200 mm × 900 mm optical isolation platform with a natural vibration of 1 Hz. The system is covered by a transparent box to reduce airflow. The experimental setup of the system is located in the China Metrology Institute Small Force Measurement Laboratory 4 m underground. The inner electrode is fixed at the end of a spring, and it moves freely along the vertical direction. The outer electrode is fixed on the frame. The electrostatic force is proportional to the square of the applied voltage across the capacitor [2], as shown in (1): where is the voltage applied across the inner and outer electrodes, is the generated electrostatic force and is the capacitance gradient, as shown in (2): where is the radius of the inner electrode, is the radius of the outer electrode, and is the absolute permittivity.
(a)
(b)
The capacitance gradient must be determined ahead of force measurement. The capacitance gradient is linearly proportional to the electrostatic force; the uncertainty of will affect the force directly. To measure accurately, the coaxial alignment of capacitor and ultraprecision machining were adopted.
A deviation from the coaxial alignment of the inner and outer electrodes results in a deviation from the ideal capacitance gradient value. A CCD camera with a pixel resolution of 2448 × 2050 and highintensity backlight source was used to check the coaxial aligning status of the two cylinders. Using this setup, deviations in eccentricity and tilting of the electrode can be detected up to values of μm and °. Therefore, the maximum relative deviations in the capacitance gradient caused by eccentricity and tilt error are 0.0018% and 0.01%, respectively.
Although uncertainty in the capacitance gradient measurement is not a key factor for determining the stiffness of the cantilever [5], the capacitance gradient must be determined ahead of force measurement in electrostatic systems. The roughness of electrode surfaces affects the potential of the capacitor. A large curvature of the electrode surface leads to a small density of charge when a voltage is applied across the electrodes, while a small curvature results in a large charge density. Moreover, the burrs would lead to point discharge and affects . For manufacturing the capacitor, the effect of surface roughness on the potential and was simulated by Comsol. As shown in Figure 2(a), surface roughness causes a considerable change in the potential of a capacitor, compared to that of a capacitor with a smooth surface. The electric field lines are concentrated on the roughness. The effect of surface roughness on for different gaps between the two electrodes ( μm, 100 μm, 200 μm, and 300 μm) is shown in Figure 2(b). Obviously, the effect of surface roughness increased with the decrease in . For the gap of 300 μm, the relative uncertainty of was 0.04% at a surface roughness of 1.1 μm. Therefore, ultraprecision machining was employed for their manufacture. The cylindrical form deviations were below 1 μm. In order to minimize the electric charge accumulation phenomenon caused by the rough surface, the external surface of the inner electrode and the internal surface of the outer electrode were limited to 3 nm. This ensured uniformity in the energy density of the electric field between the electrodes.
(a)
(b)
3. Newton Interpolation Method
Noise (creep, ground vibration, and airflow) causes limitations in force resolution. The measured force will be drowned by the noise, and therefore, it cannot be measured accurately. Further, the noise will be amplified by the spring. As the inner electrode is fixed on the spring, the position of the inner electrode will vary due to noise. The ABA method can be used to eliminate the linear creep. is the real value, , , and are the measured values, and are the values measured without the load, and is the value with the load. The linear creep can be eliminated by fitting with . However, the ABA method would be invalid, as the nonlinear noise would lead to a large uncertainty, , as shown in Figure 3.
To eliminate the effect of nonlinear noise, the Newton interpolation method was adopted, as shown in Figure 3. Sample points and were added among and . In this way, 5 sample points were used to complete a single force measurement. To reduce the effect of higher order noise, more sample points are need. For example, four sample points can eliminate the effect of thirdorder noise; however, higher order noise still affects the results.
The red line indicates real noise, the blue line is the fitting line of the Newton interpolation method, and the black line is the fitting line of the ABA method. is the fitting value that uses , , , and with Newton interpolation according to (3): where and are the Newton interpolations. is the output of the loading force. The deviations of and are small, whereas the deviation of and are very large.
Unlike the “difference method,” NIM predicts the value of by the approximation of . Using the values of several known points, an approximation was made in the range of other points.
4. Capacitance Gradient Measurement Results
To measure , the outer electrode is fixed on a nanolifting stage with a resolution of 1 nm, which was calibrated using a laser interferometer. Meanwhile, a capacitance bridge (AH2700 with a resolution of 1 aF) is used to measure the capacitance. In this way, the capacitance gradient could be traced in SI units of length and capacitance.
The displacement value of the outer electrode and the capacitance between the electrodes are shown in Figures 4(a) and 4(b). The displacement range was 50 μm and the capacitance range was 0.05 pF. To evaluate the capacitance and displacement, the signals were averaged over a period of 6 s starting from 3 s, when the capacitance was stable.
(a)
(b)
(c)
(d)
The capacitance in each step is extracted by NIM, which is shown in Figure 4(c). The points (A1, A2, A3, and A4) are used to predict the value of . The real value, , is calculated by . In this way, the nonlinear noise would be reduced by NIM.
The displacementcapacitance curve was used to calculate with straightline fitting. It has a good linearity with the displacement and capacitance, as shown in Figure 4(d). It is observed that all the capacitances of the upward steps are larger than that of the downward steps. The deviation in capacitance between the upward and downward steps was about 30 fF. The capacitance values were very close in the process of upward and downward movement, and the capacitance gradient was stable. The average capacitance gradient for nine time measurements was found to be 0.93764 pF/mm, and the standard variance was 3.5 × 10^{−4} pF/mm. The relative standard deviation was 0.004%, which ensures good repeatability. If simply the mean of A1, A2, A3, and A4 is used as the estimated capacitance, the relative standard deviation will be much larger, about 0.03%.
5. AFM Cantilever Stiffness Measurement
The stiffness of AFM cantilever [13–15] was measured based on the electrostatic force. The typical value of stiffness ranges from 5.1 to 48 N/m. The cantilever was fixed on a nanolocator having a resolution of 1 nm and a range 100 μm.
The tip of the cantilever was moved to touch the load button tip, as shown in Figure 5(a). Null balance was adopted to measure the loaded force, and a discretized proportionalintegralderivative (PID) controller was used to control the position of the inner electrode. The nanolocator was moved in 2 μm steps from 0 μm to 10 μm. It took about 100 s to complete a single scan. This movement was repeated 10 times over a period of about 1000 s. The displacement and the voltages applied to restore the inner electrode to its initial position are shown in Figures 5(b) and 5(c).
(a)
(b)
(c)
The voltage required to restore the inner electrode to its initial position for each step was extracted by NIM and is shown in Figure 6. The voltage signal includes nonlinear noise and could not be used to calculate the force directly. The points (A1, A2, A3, and A4) were used to predict the value . The real value, , was calculated by . In this way, the nonlinear noise could be reduced by NIM.
The hysteresis is checked by applying electrostatic force. As hysteresis is rather small compared to the uncertainty of the electrostatic force, the uncertainty of hysteresis could be ignored in this experiment. Surface potential is the potential difference between the electrodes resulting from the hypothesized surface field effects. The relative uncertainty comes from surface potential can be calculated by where is surface potential. Though surface potential can be as large as a few tenths of a volt, the uncertainty comes from surface potential is very small, because the voltage is about hundreds of volts. is less than 0.1% and could be ignored in this paper.
The uncertainty of observation time would lead to the uncertainty of the measurement results. The observation time of displacement is controlled by crystal oscillator with a high precision. The effect of observation time could be ignored. All underlying instruments had been calibrated at China Metrology Institute [10].
The stiffness test results are shown in Table 1. The relative standard deviation is small (less than 0.6%). If simply the mean of A1, A2, A3, and A4 is used, the relative standard deviation will be much larger and could reach up to 2.5%. These results show that our system is very stable and produces repeatable results.

From the results of the capacitance gradient and stiffness calibration for various AFM cantilevers using the system, NIM could reduce the effect of nonlinear lowfrequency noise. NIM would be invalid for signals with highfrequency noise, because the highfrequency noise would lead to inaccurate approximation. The system was placed on an isolation platform with a natural vibration of 1 Hz. The noise above 1 Hz would be filtered by the isolation platform; therefore, NIM is valid for this system and the results are very stable and repeatable.
6. Discussion
The uncertainties due to many factors such as force, displacement, and position can be estimated from the type B evaluation.
Firstly, the uncertainty of the displacement was evaluated. The displacement was measured by a capacitive feedback sensor that was integrated into the nanostage. The nanostage was calibrated by a laser interferometer. The uncertainty was estimated as 3 nm. For NSG01 and NSG10, the nanolocator was moved from 0 μm to 10 μm in 2 μm steps. For NSG20 and TESP, the nanolocator was moved from 0 μm to 2.5 μm in 0.5 μm steps. The relative uncertainties for the 2.5 μm and 10 μm displacements were conservatively estimated to be 0.12% and 0.03%, respectively.
Secondly, the gravities of 1 mg and 10 mg standard weights were compared using electrostatic force, and the uncertainties of force was established as 1.3% and 0.8%, respectively, according to the uncertainty estimate in [11].
To avoid cantilever tip damage, the back of the cantilever was contacted with a load button, as shown in Figure 5(a). This scheme results in contact position error. To observe the contact position, a microscope (MX20) with an amplification factor of 20 was used to obtain the side view. The microscope was calibrated using a traceable block gauge. It is very important to reduce the effect of distortion, as it will cause a deviation in the length. To reduce the influence of distortion, the cantilever should be placed at the centre of the visual field. Considering the offset of the loadbutton tip position compared to its apex, we estimated the uncertainty in position as 0.5 μm. The stiffness of the rectangular reference cantilever is inversely proportional to the cube of the length of the cantilever. The lengths of NSG01, NSG10, and NSG20 were 125 μm, 95 μm, and 90 μm, respectively. The uncertainty due to positioning was 1.9%, 1.7%, and 1.4%. For the cantilever TESP, the uncertainty due to positioning was 0.7%, as estimated by finite element analysis (FEM).
The uncertainty sources, force, displacement, and position are independent. The covariance between the uncertainties could be estimated as zero. The stated combined total uncertainty, , is determined by taking the root sum square of the contributions of individual uncertainty sources to the total uncertainty, as shown in Table 2. Summarizing these rather systematic influences, the combined relative uncertainty was determined to be 2%.

7. Conclusions
In this study, to measure and the stiffness calibration of various AFM cantilevers accurately, Newton interpolation method was adopted. The effect of surface roughness on the capacitance gradient was analysed quantitatively. The capacitance gradient was measured accurately with a relative standard deviation of 0.004%, which indicates that this system is very stable. In addition, the AFM cantilever stiffness was measured using this system to evaluate the performance of the system, and the combined relative uncertainty was determined to be 2%. The results of stiffness calibration show that our system is very stable and produces repeatable results. From the results of the capacitance gradient calculation and stiffness calibration of various AFM cantilevers using the system, it can be seen that NIM is a valid and effective method for reducing the effect of nonlinear lowfrequency noise, which is difficult to be removed by other methods.
Data Availability
The data used to support the findings of this study are available from the corresponding author upon request.
Conflicts of Interest
The authors declare no conflict of interest.
Acknowledgments
The authors thank the National Natural Science Foundation of China (No. 51805367 and 51175377) and the Tianjin Natural Science Foundation (No. 17JCYBJC19000) for their support.
References
 Y. Fujii, “Dynamic force calibration method for force transducers,” in Proceedings of the 21st IEEE Instrumentation and Measurement Technology Conference (IEEE Cat. No.04CH37510), pp. 352–357, Como, Italy, 2004. View at: Publisher Site  Google Scholar
 D. B. Newell, J. A. Kramar, J. R. Pratt, D. T. Smith, and E. R. Williams, “The NIST microforce realization and measurement project,” IEEE Transactions on Instrumentation and Measurement, vol. 52, no. 2, pp. 508–511, 2003. View at: Publisher Site  Google Scholar
 R. Leach, D. Chetwynd, L. Blunt et al., “Recent advances in traceable nanoscale dimension and force metrology in the UK,” Measurement Science and Technology, vol. 17, no. 3, pp. 467–476, 2006. View at: Publisher Site  Google Scholar
 V. Nesterov, “Facility and methods for the measurement of micro and nano forces in the range below 10^{−5} N with a resolution of 10^{−12} N (development concept),” Measurement Science and Technology, vol. 18, no. 2, pp. 360–366, 2007. View at: Publisher Site  Google Scholar
 J. R. Pratt and J. A. Kramar, “SI realization of small forces using an electrostatic force balance,” in Proceedings of IMEKO XVIII World Congress, pp. 1–6, Rio de Janeiro, Brazil, September 2006. View at: Google Scholar
 M. S. Kim, J. H. Choi, Y. K. Park, and J. H. Kim, “Atomic force microscope cantilever calibration device for quantified force metrology at micro or nanoscale regime: the nano force calibrator (NFC),” Metrologia, vol. 43, no. 5, pp. 389–395, 2006. View at: Publisher Site  Google Scholar
 S.J. Chen and S.S. Pan, “Nanonewton force generation and detection based on a sensitive torsion pendulum,” IEEE Transactions on Instrumentation and Measurement, vol. 58, no. 4, pp. 897–901, 2009. View at: Publisher Site  Google Scholar
 S. J. Chen and S. S. Pan, “A force measurement system based on an electrostatic sensing and actuating technique for calibrating force in a micronewton range with a resolution of nanonewton scale,” Measurement Science and Technology, vol. 22, no. 4, article 045104, 2011. View at: Publisher Site  Google Scholar
 Y. Zheng, L. Song, G. Hu et al., “Improving environmental noise suppression for micronewton force sensing based on electrostatic by injecting air damping,” Review of Scientific Instruments, vol. 85, no. 5, article 055002, 2014. View at: Publisher Site  Google Scholar
 Y. Zheng, L. Song, G. Hu et al., “The multiposition calibration of the stiffness for atomicforce microscope cantilevers based on vibration,” Measurement Science and Technology, vol. 26, no. 5, article 055001, 2015. View at: Publisher Site  Google Scholar
 L. Song, Y. Zheng, G. Hu et al., “Highly sensitive, precise, and traceable measurement of force,” Instrumentation Science & Technology, vol. 44, no. 4, pp. 386–400, 2016. View at: Publisher Site  Google Scholar
 Y. S. Ku, “Optimization of axisymmetric parametric model for electrostatic force balance,” Measurement Science and Technology, vol. 15, no. 10, pp. 2108–2112, 2004. View at: Publisher Site  Google Scholar
 S. J. Chen, S. S. Pan, Y. S. Yeh, and Y. C. Lin, “Measurement of cantilever spring constant using an electrostatic sensing and actuating force measurement system,” Measurement Science and Technology, vol. 25, no. 11, article 115006, 2014. View at: Publisher Site  Google Scholar
 A. Torii, M. Sasaki, K. Hane, and S. Okuma, “A method for determining the spring constant of cantilevers for atomic force microscopy,” Measurement Science and Technology, vol. 7, no. 2, pp. 179–184, 1996. View at: Publisher Site  Google Scholar
 D. Georgakaki, S. Mitridis, A. A. Sapalidis, E. Mathioulakis, and H. M. Polatoglou, “Calibration of tapping AFM cantilevers and uncertainty estimation: comparison between different methods,” Measurement, vol. 46, no. 10, pp. 4274–4281, 2013. View at: Publisher Site  Google Scholar
 L. Wang and Q. Zhou, “Nepenthes pitchers: surface structure, physical property, antiattachment function and potential application in mechanical controlling plague locust,” Chinese Science Bulletin, vol. 59, no. 21, pp. 2513–2523, 2014. View at: Publisher Site  Google Scholar
 L. Wang and Q. Zhou, “Friction force of locust Locusta migratoria manilensis (Orthoptera, Locustidae) on slippery zones of pitchers from four Nepenthes species,” Tribology Letters, vol. 44, no. 3, pp. 345–353, 2011. View at: Publisher Site  Google Scholar
 X. Huang, S. Chen, S. Guo, W. Zhao, and S. J. Jin, “Magnetic charge mad magnetic field distributions in ferromagnetic pipe,” Applied Computational Electromagnetics Society Journal, vol. 28, no. 8, pp. 737–746, 2013. View at: Google Scholar
 H. Wu, F. Zhang, S. Cao, S. Xing, and X. Qu, “Absolute distance measurement by intensity detection using a modelocked femtosecond pulse laser,” Optics Express, vol. 22, no. 9, pp. 10380–10397, 2014. View at: Publisher Site  Google Scholar
 C. L. Dong, C. Q. Yuan, X. Q. Bai, X. P. Yan, and Z. Peng, “Tribological properties of aged nitrile butadiene rubber under dry sliding conditions,” Wear, vol. 322323, pp. 226–237, 2015. View at: Publisher Site  Google Scholar
 C. Dong, C. Yuan, X. Bai, X. Yan, and Z. Peng, “Study on wear behaviour and wear model of nitrile butadiene rubber under water lubricated conditions,” RSC Advances, vol. 4, no. 36, pp. 19034–19042, 2014. View at: Publisher Site  Google Scholar
 L. Gao, Y. Liu, T. Ma, R. Shi, Y. Hu, and J. Luo, “Effects of interfacial alignments on the stability of graphene on Ru(0001) substrate,” Applied Physics Letters, vol. 108, no. 26, article 261601, 2016. View at: Publisher Site  Google Scholar
 L. Gao, X. Ding, T. Lookman, J. Sun, and E. K. H. Salje, “Metastable phase transformation and hcpω transformation pathways in Ti and Zr under high hydrostatic pressures,” Applied Physics Letters, vol. 109, no. 3, article 031912, 2016. View at: Publisher Site  Google Scholar
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Copyright © 2018 Yelong Zheng et al. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.