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A two-state model of simple reaction time

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- 92 -<br />

meet rather complex situation, where we must investigate many<br />

situations, each <strong>of</strong> which corresponds to each combination <strong>of</strong><br />

the ranges <strong>of</strong> values <strong>of</strong> the parameters, TO' 6;, t and 1\., <strong>of</strong> the<br />

functions, D(x) and R(x). The forms <strong>of</strong> D(x) and R(x) are<br />

natural approximations to the real ones. Densities <strong>of</strong> D(x) and<br />

R(x) are concentrated on rather restricted ranges, which are s-ome<br />

distant from the origin O. The forms <strong>of</strong> D(x) and R(x) are<br />

very <strong>simple</strong>, so the programming and calculation by computer<br />

<strong>of</strong> these functions is very easy.<br />

But, computer calculations leave some dissatisfaction.<br />

We can see only the narrow range <strong>of</strong> the behaviors <strong>of</strong> the <strong>model</strong><br />

which were simulated& The other part <strong>of</strong> the range <strong>of</strong> the behaviors<br />

which have not yet simulated is unknown until it is calculatedo<br />

In the following part <strong>of</strong> this chapter, in order to analyze<br />

the <strong>model</strong> mathematically, we make the forms <strong>of</strong> D(x) and R(x)<br />

mathematically analyzable ones.<br />

Assumption 3-2.<br />

-J.x.<br />

D(x, 6 ) ::: 1 - e<br />

where d is a decreasing function, g(T O )' <strong>of</strong> TO·

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