Outdoor Lighting and Crime - Amper
Outdoor Lighting and Crime - Amper
Outdoor Lighting and Crime - Amper
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5.2.3.4 UCR crime rate data <strong>and</strong> light energy loss per person<br />
Figure 9 is also a plot of the UCR crime rate, but this time the abscissa represents upward<br />
light energy loss per person (from Table 6), corrected as described to no-snow conditions.<br />
The regression line is positive <strong>and</strong> its slope is reliably different from zero (r 2 = 0.459, t =<br />
2.953, 19 df, p < 0.01). Without the snow correction, the regression line slope is smaller but<br />
still positive <strong>and</strong> statistically significant (r 2 = 0.338, t = 2.708, 19 df, p < 0.05). The changes<br />
introduced by the corrections to no-snow conditions are relatively insensitive to the<br />
assumptions made in deriving the corrections. As before, the actual results for the whole year<br />
would be intermediate between the original <strong>and</strong> no-snow values.<br />
Of the 21 USA cities, those with higher values of UCR crime rate have reliably more upward<br />
light energy loss per person. This supports the existence of coupled growth of lighting <strong>and</strong><br />
crime <strong>and</strong> the lighting, commerce <strong>and</strong> crime hypothesis devised to explain it, but, by itself,<br />
does not allow assignment of causality. Regardless, the regression equation shown on Figure<br />
9 appears to have a useful amount of predictive power in determining the effect of a US city<br />
lighting change on the UCR index crime rate. Within the data set examined, the equation<br />
accounts for 46% of the variance in the crime data.<br />
The data in Tables 5 <strong>and</strong> 6 were used to make a graph (not shown here) of UCR index crime<br />
rate against population. Logarithmic transformation was used to deal with the gap between<br />
the population of New York City <strong>and</strong> other cities. Despite the common belief that bigger<br />
cities have more crime, the slope in this case was slightly negative. No reliable connection<br />
exists between UCR crime <strong>and</strong> log10 population for the 21 cities: r 2 = 0.039 <strong>and</strong> t = 0.876, 19<br />
df, ns. This helps in interpretation of the findings for light <strong>and</strong> crime.<br />
5.2.3.5 Morgan Quitno crime data plots<br />
As mentioned in Section 3.2.6, the Morgan Quitno scores are based on UCR crime rate data<br />
weighted by the posed threat for various crimes, determined by survey. Cities <strong>and</strong><br />
metropolitan areas in the USA with populations of more than 75 000 are included. A score is<br />
expressed as a positive real number when the weighted UCR value is greater than the mean<br />
weighted crime rate for all of the cities. A score of 0 means the place is representative of the<br />
mean, while a negative value means less dangerous than the mean. The Morgan Quitno crime<br />
scores for 1997 were available but were missing those cities mentioned above as missing from<br />
the 1997 UCR data. The Morgan Quitno (2000) crime scores for 1998 <strong>and</strong> their ranking are<br />
used instead in this paper, <strong>and</strong> are both listed in Table 5 for the 21 cities.<br />
The Morgan Quitno crime scores were plotted (not shown here) against light energy loss per<br />
square kilometre. The regression line had a reliably positive slope (7.225) using the<br />
uncorrected light loss data (r 2 = 0.292, t = 2.356, 19 df, p < 0.05) <strong>and</strong> a statistically nonsignificant<br />
lesser positive slope (6.585) when the light measures were corrected as described<br />
to no-snow conditions (r 2 = 0.127, t = 1.551, 19 df). The statistical significance of the<br />
combined result would depend on the duration of snow cover over the year for each of the<br />
five cities observed with snow cover.<br />
The Morgan Quitno crime scores were then plotted against light energy loss per person. The<br />
regression line had a reliably positive slope of 1.886 using the light loss data corrected to nosnow<br />
conditions (r 2 = 0.537, t = 3.194, 19 df, p < 0.01) (Figure 10) <strong>and</strong> a lesser but still<br />
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