Abstract
Friction is a complicated phenomenon involving nonlinear dynamics at different length and time scales. Understanding its microscopic origin requires methods for measuring force on nanometerscale asperities sliding at velocities reaching centimetres per second. Despite enormous advances in experimental technique, this combination of small length scale and high velocity remain elusive. We present a technique for rapidly measuring the frictional forces on a single asperity over a velocity range from zero to several centimetres per second. At each image pixel we obtain the velocity dependence of both conservative and dissipative forces, revealing the transition from stickslip to smooth sliding friction. We explain measurements on graphite using a modified Prandtl–Tomlinson model, including the damped elastic deformation of the asperity. With its improved force sensitivity and small sliding amplitude, our method enables rapid and detailed surface mapping of the velocity dependence of frictional forces with less than 10 nm spatial resolution.
Introduction
Many applications in tribology require an understanding of frictional forces on nanometerscale contacts^{1,2} moving with a velocity of at least 1 cm s^{−1}. Traditional nanoscale friction experiments use an atomic force microscope (AFM), where the frictional force on the tip or colloidal probe is measured while sliding on a surface at constant velocity^{3,4,5,6,7}. Friction induces a lateral force on the tip, resulting in a twist ϕ around the major axis of the AFM cantilever (see Fig. 1a), which is detected by optical beam deflection. The cantilever’s restoring torque is assumed to be in quasistatic equilibrium, in which case the cantilever twist gives the instantaneous lateral force on the tip. When measuring individual stickslip events with this method^{8}, one typically neglects cantilever inertia and damping, a valid approach if these events occur at low enough frequency.
The quasistatic method is typically limited by detector noise, where the unity signaltonoise ratio in a 1 ms measurement time defines a typical minimum detectable force F_{min}∼13 pN (see Methods). With the quasistatic method, individual stickslip events can be resolved^{9} up to velocities ∼3 μm s^{−1}, at least four orders of magnitude below the velocity scale relevant to applications. At higher velocity stickslip events can not be resolved, only the mean force of sliding friction. Scan velocities as high as 580 μm s^{−1} have been reached^{10}, but at this velocity a measurement time of 1 ms would limit spatial resolution to 580 nm.
In contrast, dynamic methods sense frictional force as a perturbation to the cantilever’s free linear dynamics near a highquality factor resonance. The high frequency of a stiff torsional resonance f_{0}∼2 MHz allows for a maximum tip velocity v_{max}=2πf_{0}A∼6 cm s^{−1} with very small amplitude of sliding oscillation A∼5 nm. Owing to the enhanced force sensitivity of the high Q resonance, a good AFM can see the thermal random torque acting on the cantilever, which is resolved near resonance as twisting Brownian motion noise, above the voltage noise floor of the detector. In this case, force measurement is at the thermal limit of sensitivity, which for the stiff 2 MHz cantilever gives F_{min}=0.88 pN in the same 1 ms measurement time (see Methods). While dynamic friction has been previously studied using flexural^{11} and torsional^{12,13,14} resonance, thus far dynamic methods have not been used to measure frictional force, only changes of oscillation amplitude and phase when the tip engages a surface.
Here we extend the force measurement methodology of intermodulation AFM^{15,16} to lateral forces which are important for understanding friction. We describe a calibrated and quantitative dynamic method of measuring frictional force. At every image pixel, we observe the transition from stickslip to smooth sliding friction as a characteristic shape in the amplitude dependence of the dynamic force quadratures F_{I}(A) and F_{Q}(A). In contrast to the quasistatic method, dynamic force quadratures do not give the instantaneous lateral force on the tip, but rather the conservative force F_{I} and dissipative force F_{Q}, integrated over one single oscillation cycle of the tip with amplitude A (see Methods).
Results
Measurements
Intermodulation AFM is based on the detection of highorder frequency mixing (intermodulation) near a mechanical resonance. In this work the first torsional eigenmode (a linear oscillator) is driven at two frequencies near resonance. When perturbed by the nonlinear frictional force, the resonator responds with a frequency comb of intermodulation products of the two drive tones^{15}. In the time domain this frequency comb corresponds to a rapid oscillation with a slowly modulated amplitude and phase. Extracting the modulation phase allows us to resolve two Fourier coefficients of force, one which is in phase with the rapidly oscillating motion and its quadrature. These two components can be plotted as functions of the slowly varying amplitude A. Thus, the amplitudedependent dynamic force quadrature F_{I}(A) is the integrated conservative force in phase with the cantilever motion, and F_{Q}(A) the dissipative force, in phase with the velocity^{17} (see equations (5) and (6)). The transition from stickslip to freesliding dynamics of the AFM tip is revealed by a characteristic shape of these two force quadrature curves.
Figure 2a,b shows the measured force quadrature curves for a graphite surface at different interaction strengths, realized in the experiment by lowering the scanning feedback setpoint, which moves the AFM probe closer to the surface. At each interaction strength the double curves show measurement with increasing and decreasing amplitude. The net interaction which loads the frictional contact is the sum of the adhesive forces and the cantilever bending force. The latter could in principle be measured by monitoring the vertical deflection of the cantilever. However, with the rather stiff cantilever used in this experiment we could barely resolve a change in static bending. With a softer cantilever adhesive forces cause a ‘jumptocontact’ instability, making it very difficult to continuously regulate the load force. In our experiment we are able to smoothly regulate the load to observe a gradual evolution of the force quadrature curves, from zero interaction to sufficiently large interaction, where linear F_{I}(A) is observed below a critical amplitude.
From simulations (see Theory section) we understand that this lowamplitude linear dependence of F_{I}(A) corresponds to the tip apex being stuck to the surface. The measured cantilever motion is the result of elastic tip deformation. Above the critical amplitude where F_{I}(A) has a distinct minimum, stickslip dynamics begins. With increasing amplitude one observes a transition to smooth sliding, characterized by decreasing F_{I}(A) and asymptotic approach of F_{Q}(A) to a constant value. One can see how reducing the interaction force results in the gradual disappearance of the lowamplitude sticking regime. The horizontal scale of Fig. 2a,b also shows the maximum velocity of the tip base relative to the surface, v_{max}=2πf_{0}A, occurring when the cantilever crosses its torsional equilibrium point, twice each single oscillation cycle.
Theory
Our interpretation of the measured force quadrature curves in terms of stickslip dynamics of a damped elastic asperity is based on comparison of the measured data with numerical simulation of a modified Prandtl–Tomlinson (PT) model^{1,18,19,20,21,22}. In our model (see Fig. 1b) the particle is coupled via a spring and damper (damped elastic tip apex) to an intermediate support (rigid base of the tip), which in turn is coupled via a linear oscillator (cantilever torsional resonance) to a driven support (cantilever base). The inclusion of a damped elastic tip was necessary to explain the experimental data.
Figure 2c,d shows the simulated force quadratures (see Methods). Adjusting the parameters of the asperity, we can achieve good qualitative agreement between the experimental and simulated curves. Simulation allows for detailed examination of the system dynamics during the transition from stickslip to sliding friction. In the frequency domain (Fig. 3a), the periodic motion of the tip base is represented by a frequency comb. In the time domain (Fig. 3b,c), the motion of both the tip base and tip apex is plotted over exactly one period T=1/Δf, where Δf=f_{2}−f_{1} is the frequency difference of the two drive tones.
At low drive amplitude the tip apex becomes stuck in a local minimum of the potential. The tip base continues to oscillate because the elastic tip can deform. With increasing drive amplitude the tip apex begins to slip between local minima of the potential as shown in Fig. 3d. When the drive amplitude is large enough, wellseparated slips events give way to smoothsliding over many minima in the surface potential.
Discussion
The experimental curves in Fig. 2a,b show how the transition from stickslip to smoothsliding changes with applied load. With sufficient interaction strength, the tip can stick to the surface and the low amplitude slope of F_{I}(A) gives the elastic stiffness of the tip k (see Methods). For this probe we measure k=4 N m^{−1}, consistent with estimates made by other groups on similar probes^{18,20}. At lower load force a detailed examination of the experimental curves shows hysteresis in the force quadratures, as the low amplitude sticking regime (F_{Q}=0) gradually disappears with reducing load force. The simulations in Fig. 2c,d capture the qualitative shape of the force quadrature curves at higher load force, but at lower load force we find that the simulations become unstable, when the tip is just grazing the surface.
Intermodulation frictional force microscopy (ImFFM) provides a unique ability to quantitatively probe friction at high velocity with high spatial resolution. Only 2 ms are needed to measure the force quadrature curves at the nN force scale and cm s^{−1} velocity scale. This time is short enough to scan at a typical rate for dynamic AFM (1 line per second, 256 pixels per line) and create an image of the transition from stickslip to smooth sliding. Figure 4a shows such a scan over a graphite surface, where the response amplitude at drive frequency f_{1} is shown by colour. The feedback adjusts the probe height to keep this amplitude constant, and the feedback set point was changed at regular intervals during the scan, resulting in the horizontal bands seen in the image. Stable imaging was observed and there was no discernible evidence that the tip was damaging the surface, even at the highest load force.
Graphite serves as a wellstudied test sample for demonstration of ImFFM but the image is basically featureless because the friction is so homogeneous. However, a change in the response is observed when scanning across an atomic step, seen as a diagonal feature in Fig. 4a. The inset Fig. 4b shows a zoom of the step region where the colour map codes for the critical oscillation amplitude at which F_{I}(A) is minimum. In this region three pixels are marked, and the F_{I} and F_{Q} curves are shown in Fig. 4c,d with corresponding colour. Taking this critical amplitude for the onset of sliding friction, one can see how the presence of the atomic step pushes the critical amplitude to larger values. The shape of the force quadrature curves near this step also differ considerably from those of the simulation of a corrugated surface, which did not include a step. We expect the presence of a step would inhibit smooth sliding, qualitatively explaining the broad minimum observed in F_{I}(A) at much larger amplitude.
The zoom inset Fig. 4b is derived from the intermodulation spectra at each pixel and it shows features that are not present in any single amplitude or phase image. The zoom demonstrates the remarkable detail with which high velocity friction can be studied using ImFFM. The fact that neighbouring pixels (independent measurements) show similar critical amplitude demonstrates the extreme sensitivity of the method to small variations in frictional force, with spatial resolution limited only by the extent of the lateral tip oscillation, 2A≃7.2 nm for this scan. With its high spatial resolution, and its ability to capture the full amplitude dependence of friction at each image point, we anticipate that ImFFM will have large impact on our understanding of the origins of friction on heterogeneous nanostructured surfaces.
Methods
Sample, cantilever and calibration
We scanned a freshly cleaved highly oriented pyrolytic graphite sample under ambient conditions. The cantilever (MPP13120 also known as Tap525, Bruker) was calibrated using the noninvasive thermal noise method. The normal Sader method^{23} is used to get the flexural stiffness k_{f}=53 N m^{−1} from the resonance frequency f_{0,f}=470 kHz and quality factor Q_{f}=384 determined by fitting the thermal noise spectrum of the first flexural eigenmode^{24}. Similarly, the first torsional resonance f_{0,t}=2,400 kHz, Q_{t}=704 and the torsional Sader method^{23} gives a torsional stiffness k_{ϕ}=239 × 10^{−9} N m rad^{−1}. The Sader method together with the fluctuationdissipation theorem gives us the detectors inverse responsivity^{25} =1.2 × 10^{3} rad V^{−1}. The torsional stiffness corresponds to a stiffness for inplane forces acting on the tip, K=k_{ϕ}=827 N m^{−1} (manufacturerspecified tip height h_{tip}=17 μm). We formulate the equations of motion below in terms of this equivalent lateral stiffness of the torsional eigenmode, with its associated mass M=K(2πf_{0,t})^{−2} and damping coefficient MΓ=K(2πf_{0,t}Q_{t})^{−1}, where Γ is the width of the resonance.
Force sensitivity and image resolution
The sensitivity of a cantilever as transducer of force is enhanced by a factor Q on resonance, in comparison with the quasistatic (zero frequency) limit. Owing to this enhancement the thermal Brownian motion of the cantilever can often be observed as a noise peak at resonance, where the Brownian motion noise exceeds the detector noise. In this case the minimum detectable lateral force acting on the tip is given by the thermal noise force, with power spectral density,
Note that this noise force depends on the damping coefficient, not the stiffness, but it is convenient to express it in terms of stiffness, quality factor and resonant frequency, as the latter two quantities are easily accessible in the experiment. For a specified measurement bandwidth B (inverse of the measurement time), the minimum detectable force is the force signal which just equals this noise F_{min}=. At the first torsional eigenmode of our cantilever with B=1 kHz, we find F_{min}=0.88 pN.
We compare with the quasistatic sensitivity where the measurement bandwidth is centered at zero frequency. Detector noise is typically limiting sensitivity with a noise equivalent force given by,
We take voltage noise S_{VV}=8.0 × 10^{−12} V^{2} Hz^{−1} and inverse responsivity =1.2 × 10^{−3} rad V^{−1} typical of our detector. Quasistatic measurements typically use a softer cantilever^{6} k_{ϕ}∼3 × 10^{−9} N m rad^{−1} which, for the same h_{tip}=17 μm and B=1 kHz, gives =13 pN, a factor of 15 less sensitive than our experiment.
For quasistatic force measurement the time B^{−1} and constant sliding velocity v determine the distance over which the force is measured, which defines a minimum feature size δ=vB^{−1}. Increasing the measurement bandwidth (decreasing the measurement time) improves resolution, but at the expense of force sensitivity. With dynamic force measurement the minimum feature size is independent of the measurement bandwidth, given only by the amplitude of sliding oscillation δ=2A, or in terms of the maximum velocity achieved in the oscillation δ=v_{max}(πf_{0})^{−1}. High resolution (small δ), high force sensitivity (small F_{min}) and high velocity (large v_{max}) are all achieved with a small bandwidth measurement on resonance using a cantilever with large f_{0} and large Q.
Intermodulation measurement and scanning feedback
The cantilever is excited with a splitpiezo actuator at two frequencies f_{1}, f_{2} centered on torsional resonance f_{0,t} and separated by Δf=f_{2}−f_{1}<<f_{0,t}. The drive frequencies f_{1} and f_{2} are chosen such that they are both integer multiples of Δf. The drive is synthesized, and the response is measured with a synchronous multifrequency lockin amplifier (Intermodulation Products AB; http://www.intermodulationproducts.com/)^{26} which also calculates the feedback error signal used by the host AFM. A proportionalintegral feedback loop adjusts the probe height to keep the f_{1} response amplitude at the setpoint value. The exact type of feedback used is not critical to the method, only that it is responsive enough to track the surface topography at the desired scan speed. We also desire that the feedback error is small enough, such that we can approximate the probe height as being constant during the time T=(Δf)^{−1} needed to measure the response. This time defines one pixel of the 42 amplitude and phase imagepairs acquired at each frequency, during a single scan.
Model and equations of motion
A schematic representation of the model can be seen in Fig. 1. Performing force balance on both masses results in two coupled onedimensional equations of motion in the lateral position of the tip apex x_{t}, and tip base x_{b}.
The coupling force is linear in the deformation of the tip, d=x_{t}−x_{b}, and damping linear in . F_{noise}(t) is a random noise force with a Gaussian distribution^{1,27}. The strength of the noise is characterized by the standard deviation σ_{noise}, given in Table 1. The nonlinear frictional force is derived from damped motion in a periodic potential U(x_{t})=U_{0} cos(2πx_{t}/a_{0}). The drive force F_{d}=K[A_{1} cos(2πf_{1}t)+A_{2} cos(2πf_{2}t)] is applied at two frequencies as described above.
Dynamic force quadratures
We probe friction by measuring two dynamic quadratures of the nonlinear force which is perturbing the harmonic motion of the torsional resonance. The method was originally developed for normal forces and flexural resonance by Platz et al.^{17,28} From the measured intermodulation spectrum and the calibrated transfer function of the torsional eigenmode, we determine the oscillation amplitude dependence of the force quadratures, without any assumptions as to the nature of the perturbing force. For the model described above, F_{I} gives the integrated coupling force F_{c} that is in phase with the motion of the tip base, and F_{Q} that is quadrature to the motion, or in phase with the velocity.
where
When F_{fric}≫F_{c}, the tip apex is stuck in a minimum of the surface potential, x_{t}≈const, and motion of the tip base is due to tip deformation alone. In this case we can solve the integrals in equations (5) and (6),
Thus, the slope of F_{I}(A) at low amplitude and high load gives the stiffness of the asperity. Similarly, the slope of F_{Q}(A) gives the damping of the asperity, which is not resolvable in our experiment.
Simulation
We simulate the experiment by numerical integration of the model equations (3) and (4) using CVODE^{29}. The dynamical system is converted to four firstorder differential equations, characterized by two resonant frequencies: ω_{0,b}= and ω_{0,t}=. When the adaptive timestep integrator becomes rather slow. We chose , which is at least one order of magnitude smaller than experiments, but still large enough to simulate the dynamics qualitatively so that we can explore the parameter space of the model in a reasonable time (each simulation takes 200 s on an Intel Core i7, 3.50 GHz PC). We simulated with normalized values where (length)=1.42 Å, (mass)=4.78 × 10^{−25} kg and (time)=4.46 × 10^{−13} s. The parameters are given in Tables 1 and 2. To simulate different interaction strengths, we vary the surface potential U_{0} and dissipation of the tip γ as in Table 2. Our choice of simulation parameters means that the simulated frequency of surfaceinduced force pulses on the tip is about an order of magnitude smaller than in the experiment. Nevertheless, our simulation is able to capture the qualitative shape of the force quadrature curves at high velocity and high interaction strength. However, with these simulation parameters we are not able to reproduce the experiment at low velocity and low interaction.
Data and code availability
The data, analysis and simulation code that support the findings of this study are available from the corresponding author PAT upon reasonable request.
Additional information
How to cite this article: Thorén P.A. et al. Imaging highspeed friction at the nanometer scale. Nat. Commun. 7, 13836 doi: 10.1038/ncomms13836 (2016).
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Acknowledgements
We gratefully acknowledge financial support from the Swedish Research Council (VR), the Knut and Alice Wallenberg Foundation and the Olle Engkvist Foundation. We also acknowledgement the use of methods and analysis code originally developed by Daniel Platz, as well as fruitful discussions with Mark Rutland and Roland Bennewitz.
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All authors contributed to discussion and interpretation of the experimental data, model and simulations. P.A.T. did the measurements and data analysis, performed the simulations and generated all figures. A.S.d.W. contributed with model development and simulation code. R.B. and D.F. contributed to the experiments and simulation code. D.B.H., A.S.d.W. and P.A.T. contributed to the writing of the manuscript.
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D.B.H. and D.F. are part owners of the company Intermodulation Products AB, which manufactures and sells the multifrequency AFM addon system used in this work.
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Thorén, PA., de Wijn, A., Borgani, R. et al. Imaging highspeed friction at the nanometer scale. Nat Commun 7, 13836 (2016). https://doi.org/10.1038/ncomms13836
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