A Tactile Automated Passive-Finger Stimulator (TAPS)

Introduction

The Tactile Automated Passive-Finger Stimulator (TAPS) is a computer-controlled system that presses structured surfaces against the skin in order to assess a person's tactile spatial acuity. We designed and constructed the device in Duquesne University, and modified it to its current form in McMaster University. Here, we provide an overview of the function of TAPS. We then describe the components of the device, in order to facilitate its reproduction by other researchers. Finally, we show how TAPS is used to conduct a psychophysical experiment.

1. Device Overview

TAPS uses gravity to press a stimulus surface against the skin (Fig. 1). The subject's arm rests comfortably in prone position on a tabletop. The fingertip (or other skin area to be tested) lies over a tunnel in the table. Beneath the table, a stepper motor rotates a disk that holds up to 40 stimulus pieces, positioning one of the pieces under the tunnel. Gravity exerts a downward force on a mass hanging from one end of a rotatable rod. A crossbar extending from the carriage of a linear actuator prevents the rod from moving. As the actuator motors forward, the rod pivots under the influence of gravity, pressing a stimulus piece upward through the tunnel and onto the skin. Simple physics relates the speed of the actuator to the speed with which the stimulus surface rises to contact the skin, and the weight of the hanging mass to the static force of the tactile stimulus. As the actuator reverses direction to return the rod to its starting position, the stimulus piece drops. Thus, the device applies tactile stimuli with controlled force, velocity, contact duration, and inter-stimulus interval. The subject selects a button with the non-tested hand to register a response. TAPS detects the response and proceeds to deliver the next stimulus.

Figure 1. The Physics of TAPS. TAPS controls both the onset velocity and the steady-state force of the stimulus.

Onset velocity: As the crossbar from the linear actuator (red) moves to the right with velocity V₁, the left end of the rotating rod drops under the influence of gravity; the right end of the rod therefore presses a stimulus piece upwards towards the finger with velocity V₂ = V₁ (L₂ / L₃). Since V₁ is under computer control, V₂ may be set to any value desired by the investigator.

Force: Gravity exerts a downward force, F₁ = Mg, on the mass M (where g = 9.8 m/s²). This causes the stimulus piece to press against the finger with an upward force, F₂. For a massless rod, F₂ = F₁ ( L₁ / L₂). Since the rod is not in fact massless, F₂ is determined empirically, by measurement with a force sensor. To make fine adjustments to F₂, the investigator can change the position of M along the rod. F₂ increases slightly as M is moved to the left (increasing L₁), and decreases slightly as M is moved to the right (decreasing L₁). To make larger adjustments to F₂, the mass can be changed.

2. Components and Details of Device Function

i. Moving Parts

TAPS uses two stepper motors, one to drive the carriage of the linear actuator, and another to rotate the disk containing the stimulus pieces. These two motors control all of TAPS' moving parts. These parts lie on a lower table that is mechanically uncoupled from the upper table on which the subject's arm rests. Because the two tables are uncoupled, vibrations caused by the motors do not transfer to the skin. The tables are carefully aligned so that the tunnel through the upper table lies directly above the stimulus piece contacted by the rotating rod.

We machined 40 square slots around the circumference of the rotating disk, to accommodate the stimulus pieces. We constructed stimulus pieces from round plastic rods, machining the rods to have square shafts that fit into the slots of the disk. This ensures that the pieces do not rotate within their slots as the disk spins. We cut the stimulus surfaces into the round faces of the pieces.

When the actuator carriage motors forward, the end of the rotating rod opposite the hanging mass rises to contact the bottom of the selected stimulus piece. Because the rod describes an arc as it swings upwards, it is fit with a lightweight plastic bearing wheel to eliminate friction with the bottom of the stimulus piece. This plastic wheel rotates slightly as it pushes the stimulus piece upward; without the plastic wheel, the end of the rod would pull the base of the piece slightly laterally (towards the left in Fig. 1), causing the piece to jam within the tunnel through the upper table. To further ensure a smooth upward trajectory of the piece, the tunnel is fit with a plastic collar that is beveled to direct the piece towards the center of the tunnel as the piece rises.

ii. Sensors

TAPS makes use of six sensors to ensure proper functioning: two home sensors, three limit sensors, and a force sensor.

The actuator and disk home sensors signal to the computer that the actuator carriage and the disk are in their desired initial positions at the start of an experiment. The actuator home sensor is a Hall-effect sensor; the disk home sensor is a U-shaped photoelectric sensor, activated when a piece of stiff paper glued to the disk rim breaks the infrared sensor beam. When the disk is in home position, a particular slot is aligned directly under the tunnel in the upper table. All subsequent disk movement calculations are made relative to this known starting position.

The three limit sensors serve as safety features in case of malfunction. To prevent runaway movement of the actuator carriage in the unlikely event of a control malfunction, the actuator is fit with forward and reverse limit sensors (Hall-effect sensors). If activated, these cut power to the actuator. To prevent disk movement in the event that a stimulus piece becomes stuck in the tunnel, an infrared retro-reflective sensor is attached to the underside surface of the upper table. A piece that is elevated sufficiently to enter the tunnel breaks the infrared beam cast by this sensor, and blocks command voltages from reaching the disk stepper motor.

The sixth and final sensor is a force sensor that rests gently on the subject's fingernail (Fig. 2). This sensor detects downward (into the tunnel), backward or forward finger movement. The program discards trials in which movement occurred. Because the sensor is attached to a rigid arm, it additionally prevents the finger from moving passively upwards upon contact with the rising piece. Since we use TAPS to test passive (finger stationary) tactile spatial acuity, the force sensor is a crucial element. As a final precaution against finger movement, we place plastic barriers gently against the sides of the finger to prevent lateral movements.

Figure 2. Force Sensor to detect finger movement. A. The force sensor presses at 90-deg to the surface of the fingernail, near the cuticle, with a force between 50 and 80 grams. B. Example force sensor trace showing one second preceding contact of the stimulus piece with the finger, followed by one second of maintained contact with the stationary finger. Note that, upon contact (time = 0), the force of the stimulus piece from below pushes the finger more firmly up against the sensor (rising slope in force trace). C. If the subject attempts to move the finger downward to better feel the stimulus surface, then the force between the fingernail and the sensor diminishes (arrow). The sensor also registers force fluctuations if the subject moves the finger backwards or forwards. TAPS is programmed to discard any trials in which the force of contact between the sensor and the fingernail fluctuates by more than a threshold amount (e.g., 20 grams) while the skin is in contact with the stimulus surface. Using a computer-generated voice, TAPS can optionally warn the subject that movement was detected.

iii. Vibration and Sound Damping

TAPS' stepper motors produce vibration, and this in turn causes sound. Both vibration and sound are undesirable. Vibration, if transmitted to the skin, could interfere with the subject's ability to perform the tactile task. Over time, vibration could also cause mechanical instability in TAPS' components. Sound could distract the subject. For these reasons, we have taken measures to reduce both vibration and sound, and to prevent any vibration from reaching the subject.

Most importantly, the lower and upper tables do not contact one another. They are connected only in the sense that they both contact the floor. Hence, vibration from the motors, which rest on the lower table, is not transmitted to the subject's arm, which rests on the upper table. Additionally, vibration and sound are reduced as follows: a fiberglass curtain enclosing the lower table muffles device sound; PVC/fiber reinforced anti-vibration pads sandwiched between the actuator and its base absorb some of the actuator-produced vibration; the actuator base sits on four rubber cylindrical sandwich mounts that serve to further dampen vibration; the disk stepper motor base also sits on rubber mounts (syringe plunger rubber); and silicone O-rings surround the shafts of the stimulus pieces, reducing clatter as the disk turns.

iv. Stimulus Pieces

TAPS uses modified half-inch diameter rods to press spatially structured surfaces against the skin (Fig. 3). The rods are machined to have square shafts. The round faces of the rods contain the stimulus surfaces; the square shafts of the rods fit into the 40 square slots around the circumference of the rotating disk, ensuring that the stimulus surfaces maintain their proper orientations as the disk spins.

Any stimulus surfaces may be machined into the rod faces. We have used TAPS mainly to apply square wave gratings (i.e., parallel ridges and grooves). To create these, we started with 0.5" diameter Delrin plastic cylindrical rods, 3" long. Using a Sherline milling machine, we cut the rods to 2.75" long, with 2" long square-cross-section shafts (8.7 x 8.7 mm), and a 0.75"-long, 12.74 mm diameter round cylindrical head. We then milled grooves in the round face to create the stimulus surfaces. Each stimulus surface has equal ridge and groove widths. We made pieces with groove widths ranging from 0.25 to 3.10 mm in 0.15 mm increments. We made two identical stimulus pieces for each of these 20 groove widths, resulting in 40 pieces total. We then inserted the pieces into the square slots of the disk such that each groove width was represented in both the vertical (parallel to long axis of the finger) and horizontal (transverse to the long axis of the finger) orientation.

Figure 3. Stimulus piece. Each stimulus surface is milled into the face of a 0.5-inch diameter Delrin rod. The base of the rod is cut to have a square cross section, allowing it to fit into the square cutouts in the rotating disk. The surface of the piece shown is a square-wave grating, with parallel grooves and ridges of equal width.

v. Computer Control

TAPS is a fully automated, computer-controlled system. Many computer hardware and software configurations could be used to control the device. We currently use a Macintosh G3 running LabVIEW 6.1 (National Instruments). The computer communicates via a motor controller board with a stepper motor driver to command the actuator and disk motors, and to read the home sensors and limit switches. A PCI data acquisition board reads the force sensor and subject response buttons.

vi. Force and Timing Limitations

Force range: We have used TAPS to deliver stimuli with forces ranging from 10 to 50 grams. We suspect that friction in the components would impede the delivery of stimuli at forces under about 5 grams, and that some mechanical instability would arise for forces in excess of about 100 grams.

Inter-stimulus interval (ISI): The distance between the stimulus surfaces and the finger, and the stable speeds of the linear actuator and disk stepper motor, together set a lower limit on the ISI that the device can achieve. We estimate this limit at about 1.5 seconds. Thus, the device is not appropriate for applications such as masking experiments, which require sub-second ISI.

3. Conducting an Experiment

Here we describe one protocol for which TAPS can be used: a two-interval forced-choice (2-IFC) grating orientation task (GOT) with Bayesian adaptive tracking. TAPS can be programmed for many other psychophysical protocols as well. We have used it previously to conduct 2-IFC experiments with staircase tracking^1,2 and with the method of constant stimuli. Of course, it is able to conduct yes/no procedures as well as 2-IFC.

For the 2-IFC GOT task, we use square wave gratings that contact the distal pad of the finger with 4 cm/sec onset velocity, 50 gm contact force, and 1 sec contact duration. Each trial consists of two sequential stimulus presentations (ISI: 2 sec) with gratings of identical groove width, but differing 90-deg in orientation. In one presentation, the grooves are aligned vertically (parallel), and in the other, horizontally (transverse), to the long axis of the finger. Stimulus order is chosen randomly by the computer program. The subject indicates whether the horizontal orientation occurred in the first or second interval, by pressing one of two buttons with the non-tested hand. A Bayesian adaptive method adjusts groove width from trial to trial.

We programmed TAPS with a modified version of the psi (Ψ) method, a Bayesian adaptive algorithm³. This method has several advantages over conventional adaptive methods, such as staircase methods. First, the psi method estimates not just a single point on the psychometric function (e.g., the 71% threshold estimated by a 2-down 1-up staircase), but the entire psychometric function. Second, the method yields Bayesian posterior probability distributions (and thereby confidence intervals) for the parameters of the psychometric function. Finally, the method is efficient. It holds in memory many thousands of possible psychometric function shapes, and updates the posterior probability of each function after each response. It then uses an expected entropy minimization procedure to choose the next stimulus; that is, it chooses the stimulus on each trial that is expected to maximize the information gain.

Following Kontsevich and Tyler³, we modeled d-prime as a power function of stimulus level, and each subject's psychometric function – P_c(x), the probability of a correct response as a function of stimulus level, x – as a mixture of a cumulative normal (probit) function and a lapse rate term:


Here, a is the threshold (stimulus level corresponding to 76% correct response probability, d-prime = 1), and b is the slope, of the subject's psychometric function.

We modified the Ψ algorithm by treating the lapse rate (delta) as a parameter of unknown value, and by calculating a "guessing Bayes factor" after each trial:


This Bayes factor is a likelihood ratio that compares the probability of the data under hypothesis 1, that the subject is guessing, to the probability of the data under hypothesis 2, that the subject has a psychometric function. The numerator is the probability of the subject's data, D (correct and incorrect responses at each of the groove widths presented) given that the subject is simply guessing (50% probability correct) on all trials up to and including the current trial. The denominator is the probability of the data given the algorithm's best estimate of the subject's psychometric function. In our experience, for most young subjects the Bayes factor rapidly approaches zero as the testing block progresses, indicating that the subject's performance conforms to a psychometric function. For some older subjects, the Bayes factor rises above one, indicating that the subject is unable to perform the task. TAPS can be programmed to terminate the testing block if the guessing Bayes factor has exceeded a threshold value after a specified number of trials.

4. Results

Figure 4 shows an experimental block consisting of 40 trials from a 2-IFC GOT experiment. This 40-trial block consisted of 80 stimuli to the subject's right middle finger, with 1-second contact duration and 2-second ISI between contacts in a single trial. The subject's 76% correct threshold was 1.7 mm, as indicated by the mode of the posterior probability density function (PDF) for the threshold parameter (panel C). The 95% confidence interval for the subject's threshold parameter, indicated by the width of the posterior PDF, was 1.3 – 1.9 mm.

Figure 4. Results from a 2-interval forced-choice grating orientation task. A. An experimental block, consisting of 40 trials applied in this case to the right middle finger. The subject's correct (plus symbols) and incorrect (open circles) responses at different groove widths are plotted against trial number. A Bayesian adaptive method (see text) determined the sequence of groove widths to apply, based on the subject's performance. B. The best-fit psychometric function for this subject. C. Posterior probability density function for the subject's 76% correct groove width (psychometric function a-parameter, corresponding to d-prime = 1).