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1.
Repeated warm laser stimuli produce a progressive increase of the sensation of warmth and heat and eventually that of a burning pain. The pain resulting from repetitive warm stimuli is mediated by summated C fibre responses. To shed more light on the cortical changes associated with pain during repeated subnoxious warm stimulation, we analysed magnetoencephalographic (MEG) evoked fields in eleven subjects during application of repetitive warm laser stimuli to the dorsum of the right hand. One set of stimuli encompassed 10 laser pulses occurring at 2.5 s intervals. Parameters of laser stimulation were optimised to elicit a pleasant warm sensation upon a single stimulus with a rise of skin temperature after repeated stimulation not exceeding the threshold of C mechano-heat fibres. Subjects reported a progressive increase of the intensity of heat and burning pain during repeated laser stimulation in spite of only mild (4.8°C) increase of skin temperature from the first stimulus to the tenth stimulus. The mean reaction time, evaluated in six subjects, was 1.33 s, confirming involvement of C fibres. The neuromagnetic fields were modelled by five equivalent source dipoles located in the occipital cortex, cerebellum, posterior cingulate cortex, and left and right operculo-insular cortex. The only component showing statistically significant changes during repetitive laser stimulation was the late component of the contralateral operculo-insular source peaking at 1.05 s after stimulus onset. The amplitude increases of the late component of the contralateral operculo-insular source dipole correlated with the subjects' numerical ratings of warmth and pain. Results point to a pivotal role of the contralateral operculo-insular region in processing of C-fibre mediated pain during repeated subnoxious laser stimulation.  相似文献   

2.
Diverging observations on secondary hyperalgesia to heat stimuli have been reported in the literature. No studies have investigated the importance of heat stimulus intensity and duration for the assessment of secondary heat hyperalgesia. The present study was designed to investigate systematically (1) if pain sensitivity to radiant heat stimuli (focused Xenon light) is altered in the area of secondary punctuate hyperalgesia induced by intradermal injection of capsaicin and (2) if heat stimulus duration and intensity had an influence on the ability to detect secondary heat hyperalgesia.Pain ratings to radiant heat stimuli from a focused xenon lamp were assessed within the area of secondary punctuate hyperalgesia in fifteen volunteers before and after intradermal injection of capsaicin. The stimulus conditions were systematically varied between three intensity levels (0.8, 1.0 and 1.2 x heat pain threshold (PT)) and four duration steps (200, 350, 500 and 750 ms). The present study shows that long duration (350-750 ms) and low intensity (0.8 and 1.0 x PT) radiant heat stimuli were adequate to detect secondary heat hyperalgesia.  相似文献   

3.
Summary Although cutaneous type I and type II mechanoreceptors in the cat respond at progressively higher frequencies to increasingly rapid skin indentations of suprathreshold intensity, their thresholds are not lowered when these more rapid stimuli are applied. Since these receptors do not selectively detect rapid stimuli of small amplitude, even though they respond much more vigorously to a suprathreshold stimulus that is rapid, different parameters of the stimulus are signalled depending on whether it is near threshold or clearly suprathreshold.This work was supported by grant GB42643 from the National Science Foundation and by grants NS08769, NS07938 and NS05244 from the U.S. Public Health ServiceThe authors thank John Fisher, Gary Frederickson, Tom O'Leary, Robert Perry, and Jane Burgess for their valuable help.  相似文献   

4.
Diverging observations on secondary hyperalgesia to heat stimuli have been reported in the literature. No studies have investigated the importance of heat stimulus intensity and duration for the assessment of secondary heat hyperalgesia. The present study was designed to investigate systematically (1) if pain sensitivity to radiant heat stimuli (focused Xenon light) is altered in the area of secondary punctuate hyperalgesia induced by intradermal injection of capsaicin and (2) if heat stimulus duration and intensity had an influence on the ability to detect secondary heat hyperalgesia.

Pain ratings to radiant heat stimuli from a focused xenon lamp were assessed within the area of secondary punctuate hyperalgesia in fifteen volunteers before and after intradermal injection of capsaicin. The stimulus conditions were systematically varied between three intensity levels (0.8, 1.0 and 1.2?×?heat pain threshold (PT)) and four duration steps (200, 350, 500 and 750?ms). The present study shows that long duration (350–750?ms) and low intensity (0.8 and 1.0 ×?PT) radiant heat stimuli were adequate to detect secondary heat hyperalgesia.  相似文献   

5.
Psychophysical measurements were made of the sensory effects of l-menthol applied topically to the forearm under controlled thermal conditions. In the first experiment, subjects judged the intensity and quality of sensations produced by warming or cooling the skin in the presence of menthol or the vehicle. During cooling, menthol intensified cutaneous sensations and increased reports of burning. During warming, menthol intensified sensations transiently at low temperatures and weakened them lastingly at higher temperatures; the frequency of reports of burning varied with intensity. A second experiment tested the hypothesis that menthol would lower the threshold for warmth and raise the threshold for heat pain. No change in either threshold was observed. The primary sensory effects of l-menthol on hairy skin are therefore to heighten the perception of cooling and to attenuate the perception of moderate warming. In contrast with other common chemical irritants, menthol's pungent qualities appear to be enhanced by cooling and suppressed by warming; this suggests that its sensory irritancy may be attributable to the stimulation of a population of high-threshold cold fibers or cold-sensitive nociceptors.  相似文献   

6.
Negative phonotaxis is elicited in flying Australian field crickets, Teleogryllus oceanicus, by ultrasonic stimuli. Using upright tethered flying crickets, we quantitatively examined several kinematic and aerodynamic factors which accompany ultrasound-induced negative phonotactic behavior. These factors included three kinematic effects (hindwing wingbeat frequency, hindwing elevation and depression, and forewing tilt) and two aerodynamic effects (pitch and roll). 1. Within two cycles following a 20 dB suprathreshold ultrasonic stimulus, the hindwing wingbeat frequency increases by 3-4 Hz and outlasts the duration of the stimulus. Moreover, the relationship between the maximum increase in wingbeat frequency and stimulus intensity is a two-stage response. At lower suprathreshold intensities the maximum wingbeat frequency increases by approximately 1 Hz; but, at higher intensities, the maximum increase is 3-4 Hz. 2. The maximum hindwing elevation angle increases on the side ipsilateral to the stimulus, while there was no change in upstroke elevation on the side contralateral to the stimulus. 3. An ultrasonic stimulus affects forewing tilt such that the forewings bank into the turn. The forewing ipsilateral to the stimulus tilts upward while the contralateral forewing tilts downward. Both the ipsilateral and contralateral forewing tilt change linearly with stimulus intensity. 4. Flying crickets pitch downward when presented with a laterally located ultrasonic stimulus. Amputation experiments indicate that both the fore and hindwings contribute to changes in pitch but the pitch response in an intact cricket exceeds the simple addition of fore and hindwing contributions. With the speaker placed above or below the flying cricket, the change is downward or upward, respectively.(ABSTRACT TRUNCATED AT 250 WORDS)  相似文献   

7.
Intensity Characteristics of the Noctuid Acoustic Receptor   总被引:1,自引:0,他引:1       下载免费PDF全文
Spiking activity of the more sensitive acoustic receptor is described as a function of stimulus intensity. The form of the intensity characteristic depends strongly on stimulus duration. For very brief stimuli, the integral of stimulus power over stimulus duration determines the effectiveness. No response saturation is observed. With longer stimuli (50 msec), a steady firing rate is elicited. The response extends from the spontaneous rate of 20–40 spikes/sec to a saturated firing rate of nearly 700 spikes/sec. The characteristic is monotonic over more than 50 db in stimulus intensity. With very long stimuli (10 sec), the characteristics are nonmonotonic. Firing rates late in the stimulus decrease in response to an increase in stimulus intensity. The non-monotonic characteristics are attributed to intensity-related changes in response adaptation.  相似文献   

8.
The temporal parameters of the perception of radially moving sound sources partly masked with broadband internalized noise at an intensity of 40, 46, or 52 dB above the hearing threshold have been studied. The threshold of sound duration necessary for identifying the direction of movement of the sound source (75% correct answers) increases from 135 ms in silence to 285 ms at all intensities of continuous noise studied. The minimum duration of the stimulus beginning with which a subsequent increase in duration does not increase the number of correct responses is the same (385 ms) under all conditions of stimulus presentation. Broadband noise of any intensity increases the time of response to stimuli in the range of durations studied. At a noise of 52 dB, which is close to the threshold of full masking, the reaction time is not increased significantly compared to its estimation at a noise of 46 dB. The minimum duration of the stimulus has proved to be the stablest temporal parameter of the perception of movement of a sound source. Changes in the temporal parameters of sound perception at noise levels close to the threshold of full masking are discussed.  相似文献   

9.
目的:研究1.06μm激光所致人手背皮肤的痛觉效应。方法:以输出波长为1.06μm的脉冲Nd:YAG激光照射人手背皮肤,记录每次刺激激光的能量以及受试者的反应。采用加权概率单位算法计算诱发痛觉概率为50%时对应的激光剂量ED50,即为痛觉阈值。改变光斑大小和脉冲宽度,测定三种不同刺激条件下的痛觉阈值,并探索温度对激光所致痛觉效应的影响。结果:当皮肤温度约为30℃,分别使用光斑直径1.20mm、脉冲宽度85μs,光斑直径1.20mm、脉冲宽度20ns和光斑直径2.56mm、脉冲宽度20ns的激光刺激时,痛觉阈值分别为394mJ/mm^2、36.4mJ/mm^2和8.92mJ/mm^2。在第一种刺激条件下,当皮肤温度为25℃时,剂量为383mJ/mm^2的激光诱发痛觉的概率为16.7%;当皮肤温度为39℃时,剂量为361mJ/mm^2的激光诱发痛觉的概率为56.7%。结论:1.06“m激光所致痛觉的阈值随脉冲宽度的减小、光斑面积的增大和皮肤表面温度的增加而减小。  相似文献   

10.
Psychophysical visual analog scaling can be used to reveal critical determinants of the neural processing underlying non-painful and painful heat sensations produced by radiant and contact heat stimulation. This study determined the stimulus-response (S-R) functions of cutaneous non-painful and painful heat stimuli delivered by an infra-red CO2 laser or by a contact thermode in a series of experiments in healthy volunteers. In experiment 1 ( n = 12), with the rating scale anchored at pain threshold, the S-R curve for brief (60 ms) laser pulse stimulation with a beam diameter of 10 mm was a negatively accelerating function. Transformation of laser stimulus intensity (W) into temperatures ( C) did not change the form of the S-R curve. In experiment 2 ( n=9), using the same laser stimulus parameters as in experiment 1, but without an anchored rating scale, the form of the S-R relationship did not change. In experiment 3 ( n =9), increases of the laser pulse duration up to 5 s and the beam diameter up to 18 mm produced linear S-R curves. In contrast, in experiment 4 ( n =21), the S-R curve for cutaneous contact heat stimuli applied for 5 s with an 18 mm diameter probe was best described by a positively accelerating power function with an exponent greater than 2.0. These experiments have (1) characterized the S-R functions for different parameters of infra-red laser stimulation of the skin, and (2) have shown that the form of the S-R function for innocuous and noxious heat sensation is influenced strongly by the physical conditions of heat stimulus application, including mechanical contact with the skin.  相似文献   

11.
The relationship between thermal detection threshold and rate of temperature change of the thermal stimulus when slow (<1 degrees C s(-1)) rates of change are employed was investigated. Using both the reaction time (RT) inclusive Method of Limits and RT exclusive Method of Levels healthy volunteers had warming (WDT) and cooling detection thresholds (CDT) measured at four different rates of temperature change (0.3, 0.5, 0.7 and 1.0 degrees C s(-1)) from the thenar and/or mental regions using a contact thermode. With the Method of Limits, CDT increased linearly with rate of temperature change suggesting increments were due to RT artefacts. This was further supported by threshold assessment with the Method of Levels which showed CDT were unaffected by the rate of change in the RT exclusive method (P > 0.1). In contrast, WDT did not increase linearly with rate of stimulus temperature change when the Method of Limits was used and threshold assessment with the Method of Levels showed WDT assessed using a 0.3 degrees C s(-1) ramp rate were significantly higher than those measured with a 1 degrees C s(-1) rate of change (P < 0.05). This study indicates that adaptation to a warming stimulus can occur at faster rates of stimulus change than previously anticipated and identifies differences in warming and cooling pathways in sensitivity to adaptation.  相似文献   

12.
Responses of 75 single units in the goldfish olfactory bulb were analyzed in detail for their relationship to the time-course of the change in odor concentration during each odor stimulus. Odor stimuli were controlled for rise time, duration, and peak concentration by an apparatus developed for the purpose. This apparatus enabled aqueous odor stimuli to be interposed into a constant water stream without changes in flow rate. The time-course of the concentration change within the olfactory sac was inferred from conductivity measurements at the incurrent and excurrent nostrils. Temporal patterns of firing rate elicited by stimuli with relatively slow rising and falling phases could be quite complex combinations of excitation and suppression. Different temporal patterns were produced by different substances at a single concentration in most units. Statistical measures of the temporal pattern of response for a small number of cells at a given concentration were more characteristic of the stimulus substance than any of three measures of magnitude of response. The temporal patterns change when the peak concentration, duration, and rise time of the stimuli are varied. The nature of these changes suggests that the different patterns are due primarily to the combined influence of two factors: (a) a stimulus whose concentration varies over time and (b) a relationship between concentration and impulse frequency which varies from unit to unit. Some units produce patterns suggestive of influence by neural events of long time constant. The importance of temporal patterns in odor quality and odor intensity coding is discussed.  相似文献   

13.
A new multimodal pain assessment model was developed integrating electrical, mechanical, cold, and warmth stimuli into the same device. The device, with a bag and electrodes for electrical stimulation, was positioned in the lower part of the esophagus in 11 healthy subjects. Mechanical stimuli were delivered with an impedance planimetric system. Thermal stimuli were performed by circulating water of different temperatures (5-50 degrees C) inside the bag. All subjects reported both nonpainful and painful local and referred sensations to all stimuli. Temporal summation to repeated electrical stimuli could be studied. For all stimuli, there was a relationship between stimulus intensity and pain intensity. The referred pain area increased with increasing intensity of the electrical and mechanical stimuli. There were several differences between the sensations evoked by the four stimulus modalities, indicating activation of different visceral nerve pathways. This model offers the possibility for controlled multimodal stimuli activating the superficial and deeper layers of the human gut and should be used in basic, clinical, and pharmacological pain studies.  相似文献   

14.
Perception of cutaneous heating and cooling depends strongly on stimulus size. Although this dependence has been attributed solely to spatial summation, topographical variations in temperature sensitivity may also play a role. These variations, which differentially affect perception of small stimuli, may have led to overestimation of spatial summation. This possibility was investigated by measuring detection thresholds and perceived intensity for heating and cooling on the volar surface of the forearm using a multiple-thermode stimulus array. By keeping the array in place throughout each testing session we were able to measure threshold sensitivity and suprathreshold responsiveness at eight individual sites and for combinations of these sites having total stimulus areas of 0.64-5.12 cm2. When spatial summation was calculated in the traditional way by averaging the data for all stimuli of each size, the results agreed closely with previous estimates of summation for warmth and cold. When calculations were based instead on the most sensitive test site for each stimulus size, estimates of summation were reduced by about two-thirds. This outcome indicates that the spatial heterogeneity of thermal sensitivity likely contributed to estimates of spatial summation reported in earlier psychophysical studies. A schematic model of cutaneous thermoreception is presented that shows how neural summation and the density of innervation may combine to produce the psychophysical effects of increasing stimulus size (spatial enhancement).  相似文献   

15.
Perception of cutaneous heating and cooling depends strongly on stimulus size. Although this dependence has been attributed solely to spatial summation, topographical variations in temperature sensitivity may also play a role. These variations, which differentially affect perception of small stimuli, may have led to overestimation of spatial summation. This possibility was investigated by measuring detection thresholds and perceived intensity for heating and cooling on the volar surface of the forearm using a multiple-thermode stimulus array. By keeping the array in place throughout each testing session we were able to measure threshold sensitivity and suprathreshold responsiveness at eight individual sites and for combinations of these sites having total stimulus areas of 0.64-5.12 cm2. When spatial summation was calculated in the traditional way by averaging the data for all stimuli of each size, the results agreed closely with previous estimates of summation for warmth and cold. When calculations were based instead on the most sensitive test site for each stimulus size, estimates of summation were reduced by about two-thirds. This outcome indicates that the spatial heterogeneity of thermal sensitivity likely contributed to estimates of spatial summation reported in earlier psychophysical studies. A schematic model of cutaneous thermoreception is presented that shows how neural summation and the density of innervation may combine to produce the psychophysical effects of increasing stimulus size (spatial enhancement).  相似文献   

16.
We determined the temporal changes in effectiveness of inspiratory-shortening expiratory-prolonging stimulus trains delivered in the region of the nucleus parabrachialis medialis and compared the responses to those observed during trains delivered to the vagus in the same animals (pentobarbital, sodium-anesthetized paralyzed cats). The inspiratory inhibitory effect of the pontine stimulus was assessed from the effect the stimulus has on threshold for terminating inspiration. Stimulus effect increased gradually, reached a peak at 0.2-0.4 s, and declined thereafter. The time of occurrence of peak effect was different from that observed in the course of vagal stimulus trains. With long stimulus trains (19-40 s), the initial effect on inspiratory duration (TI) (i.e., shortening) rapidly subsided and, in six of eight animals, was replaced by TI prolongation. The initial effect on expiratory duration (TE) (i.e., prolongation) also gradually declined with time but TE remained above control throughout. The time constant of adaptation was very similar with vagal and pontine stimulus trains (12.2 and 11.0 s, respectively), but the gain of the adapting response was much more pronounced with pontine stimuli, resulting in a paradoxical effect while stimulation continued. We conclude that the response to pontine stimuli, as with vagal stimuli, displays both integrative and adaptive characteristics. The similarity of the time constants for vagal and pontine adaptation responses suggests that these two inputs share common processing pathways.  相似文献   

17.
The aim was to study spatial summation within and between ipsi- and contralateral dermatomes at different painful temperatures. For heat stimulation we used a computer controlled thermofoil based thermode. The thermode area could be varied in five discrete steps from 3.14 to 15.70 cm2. When we applied the stimuli within a dermatome, the mean heat pain threshold decreased significantly from 45.6 to 43.5 C as the area was increased from minimum (3.14 cm2) to maximum (15.70 cm2). When the areas were increased involving different dermatomes (both ipsi- or contralateral), we found similar decreases in pain threshold. Spatial summation was also found within and between dermatomes at supra-threshold temperatures (46, 48, 50 C).The study shows that spatial summation of pain is most likely a mechanism acting across segments and is existing from pain threshold to tolerance.  相似文献   

18.
Natural visual scenes are rich in information, and any neural system analysing them must piece together the many messages from large arrays of diverse feature detectors. It is known how threshold detection of compound visual stimuli (sinusoidal gratings) is determined by their components' thresholds. We investigate whether similar combination rules apply to the perception of the complex and suprathreshold visual elements in naturalistic visual images. Observers gave magnitude estimations (ratings) of the perceived differences between pairs of images made from photographs of natural scenes. Images in some pairs differed along one stimulus dimension such as object colour, location, size or blur. But, for other image pairs, there were composite differences along two dimensions (e.g. both colour and object-location might change). We examined whether the ratings for such composite pairs could be predicted from the two ratings for the respective pairs in which only one stimulus dimension had changed. We found a pooling relationship similar to that proposed for simple stimuli: Minkowski summation with exponent 2.84 yielded the best predictive power (r=0.96), an exponent similar to that generally reported for compound grating detection. This suggests that theories based on detecting simple stimuli can encompass visual processing of complex, suprathreshold stimuli.  相似文献   

19.
How do humans perceive the passage of time and the duration of events without a dedicated sensory system for timing? Previous studies have demonstrated that when a stimulus changes over time, its duration is subjectively dilated, indicating that duration judgments are based on the number of changes within an interval. In this study, we tested predictions derived from three different accounts describing the relation between a changing stimulus and its subjective duration as either based on (1) the objective rate of changes of the stimulus, (2) the perceived saliency of the changes, or (3) the neural energy expended in processing the stimulus. We used visual stimuli flickering at different frequencies (4–166 Hz) to study how the number of changes affects subjective duration. To this end, we assessed the subjective duration of these stimuli and measured participants'' behavioral flicker fusion threshold (the highest frequency perceived as flicker), as well as their threshold for a frequency-specific neural response to the flicker using EEG. We found that only consciously perceived flicker dilated perceived duration, such that a 2 s long stimulus flickering at 4 Hz was perceived as lasting as long as a 2.7 s steady stimulus. This effect was most pronounced at the slowest flicker frequencies, at which participants reported the most consistent flicker perception. Flicker frequencies higher than the flicker fusion threshold did not affect perceived duration at all, even if they evoked a significant frequency-specific neural response. In sum, our findings indicate that time perception in the peri-second range is driven by the subjective saliency of the stimulus'' temporal features rather than the objective rate of stimulus changes or the neural response to the changes.  相似文献   

20.
Computations show that cathodal rheobase increases with temperature from 0 degrees C to 30 degrees C. Anodal rheobase (stimulation at the end of an indefinitely long anodal pulse) also increases with temperature, but goes to infinity at a critical temperature 17.13 degrees C, above which such excitation is impossible. For a stimulus consisting of any step change of current from I0 to I1, a threshold curve of I1 is plotted against I0. As the temperature increases, this curve rises. Its intersection with the horizontal axis, which determines the anodal rheobase, goes to infinity at the critical temperature. This phenomenon is caused by the saturation of the variables m, h, n for strongly hyperpolarized potentials, combined with the relative speeding up of the inhibitory process with increasing temperature. The threshold charge Q in an instantaneous anodal current pulse (of zero duration) goes to infinity at the same temperature, with a similar explanation in terms of threshold curves in the I1 vs. Q plane. The fact that the critical temperature for both cases is the same is generalized by the conjecture that for any anodal current waveform whatever, as its amplitude approaches infinity, the trajectory in the phase space following its cessation approaches the same limiting trajectory. This limiting trajectory changes from suprathreshold to subthreshold at the critical temperature.  相似文献   

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