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Statistical Methods in Medical Research 4ed

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where Vd ˆ var(d ), Cdb ˆ cov(d, b) andVbˆvar(b). These variances and the<br />

covariance should be obta<strong>in</strong>able from the computer output. Approximate<br />

100…1 a)% confidence limits for log r are then<br />

p<br />

M za var…M† ,<br />

where za is the usual standardized normal deviate. Limits for r are obta<strong>in</strong>ed by<br />

tak<strong>in</strong>g antilogs.<br />

By analogy with (20.8), Fieller's theorem can be used to give more reliable<br />

approximations. From (5.13) the limits for log r then become<br />

M gCdb<br />

Vb<br />

za<br />

b Vd 2MCdb ‡ M 2 Vb g Vd<br />

,<br />

1 g<br />

where g ˆ za 2Vb=b2 .<br />

Approximate x2 tests for (i) parallelism and (ii) l<strong>in</strong>earity may be obta<strong>in</strong>ed by<br />

the analysis of deviance, by tak<strong>in</strong>g: (i) the difference between the deviances of the<br />

fitted model and a model with separate slopes for S and T; and (ii) the deviance<br />

of the latter model.<br />

An alternative approach to the analysis of quantal-response data, probit<br />

analysis, is widely used. This method, which is fully described by F<strong>in</strong>ney (1971),<br />

provides the maximum likelihood solution for the probit or normal equivalent<br />

deviate (NED) transformation (§14.1) rather than for the logit. Here P is the<br />

distribution function for a standard normal deviate Y (a constant 5 be<strong>in</strong>g added<br />

to the NED to give the probit). This transformation thus implies that the tolerance<br />

distribution for the log dose is normal, and the slope parameter b <strong>in</strong> (20.20) is the<br />

reciprocal of the standard deviation. There is no evidence to suggest that either<br />

model is more consistent with real data than the other, and curves fitted by the two<br />

methods are <strong>in</strong>variably very similar.<br />

Before the advent of computer programs for the efficient analysis of quantalresponse<br />

data, a number of simple methods were <strong>in</strong> common use. These ma<strong>in</strong>ly<br />

aimed to estimate the location of the tolerance distribution as summarized by its<br />

median. This is the dose at which P ˆ 0 5, and is called the median effective dose<br />

(ED50). In the comparison of two response curves, the ED50 for T and S are <strong>in</strong> the<br />

ratio 1 : r. If they are estimated by X0T and X0S, the ratio X0S=X0T will provide an<br />

estimate of r. The ED50 is sometimes given slightly different names accord<strong>in</strong>g to<br />

the type of response: e.g. LD50 or median lethal dose if the response is lethal. A full<br />

account of these short-cut methods is given by F<strong>in</strong>ney (1978, §§18.6±18.8).<br />

The up-and-down (or staircase) method<br />

20.4 Quantal-response assays 729<br />

In experiments or assays <strong>in</strong> which the ma<strong>in</strong> purpose is to estimate the ED50, the<br />

choice of dose levels is important. Doses yield<strong>in</strong>g very low or very high values of<br />

C 2 db<br />

Vb<br />

1<br />

2

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