Since it is practically convenient, so-called resistance method by Veraguth has been used commonly in the investigation of the galvanic skin reflex (GSR). However, this method has some difficulties in the quantitative measurements of reflex curves, as they are influenced by the basal resistance or the strength of electric currents through the skins of the objects.
In our study, it was purposed to study the effects of variable strength of the currents upon reflex curves. The experiments were conducted on 8 female adults during the period from June to September at the room temperature of 24.0° to 31.5°C. Two reflex curves were recorded from both palms and forearms simultaneously by means of a pair of so-called simple circuits which consist of battery cells, vibrator-F (5 × 10
-1A, 35c/s, 60Ω), microammeter and two Zn-ZnSO
4 kaolin electrodes.
It is remarkable that by means of this method the reflex curve can be recorded accurately, both in time and in shape. In our experiments, the strength of the currents of one side (left side) were increased from 50 μA upto 100μA, step by step, while that of the other side (right side) were kept constant at 100μA, to be the control side. It is a characteristics in our device to compare the corresponding reflex curves of both palms, instead of statistical observation of the reflex curves at different times, as it is the customary used method of measurements.
Our results were as follows:
1) At 100μA, the mean latent time out of 60 to 90 reflexes of each subject was 1.22 to 2.40 seconds and the mean top time (reaction time) was 0.97 to 2.25 seconds, showing normal distributions.
2) The reflex appeared out to one correspondence at both palms, and if the skin temperature and the strength of the current applied were kept constant during each series of experiments, latent time, toptime and amplitudes of reflex curves showed almost the same value in both sides. If the amplitudes of reflex curves increased, latent time showed the tendency of decrease and reaction time became longer.
3) If the strength of the current was increased from 50μA, step by step, upto 300μA, the latent time became gradually short, the reaction time became long and the amplitude measured by μA increased gradually.
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