Dale A. C.
Brownson
and
Craig E.
Banks
*
Faculty of Science and Engineering, School of Chemistry and the Environment, Division of Chemistry and Environmental Science, Manchester Metropolitan University, Chester Street, Manchester, M1 5GD, Lancs, UK. E-mail: c.banks@mmu.ac.uk; Fax: +(0)1612476831; Tel: +(0)1612471196
First published on 2nd November 2010
We explore for the first time the relationship between the drug content of blood and its corresponding physical property, viscosity, and examine whether this effect can lead to the miss-interpretation of the Bloodstain Pattern Analysis (BPA) of drug contaminated bloodstains found at crime scenes. The viscosity of amphetamine spiked blood was measured using a capillary tube viscometer with amphetamine concentrations explored over the range 3.0 × 10−7 to 4.1 × 10−3 mol dm−3 equating to therapeutic and potentially fatal levels respectively, which are commonly found in Crime Scene Investigation and were found to result in a viscosity change; the range of 0.5–11.0% respectively. Based on these observations the estimation of variances within BPA was calculated by introducing the variability of the viscosity into previously derived equations. We find with increasing amphetamine concentrations an increase in the percentage change (corresponding to a decrease in dynamic viscosity) of blood viscosity occurred; this variation theoretically induces a 0.61 mm diameter alteration (2.9%) of resultant bloodstains. The effect of drug contaminated bloodstains on BPA is currently an under explored area within the field of forensic science which requires further investigation due to BPA's inclusion in legal proceedings.
Research conducted by Herbert Leon MacDonell1 stated that bloodstains produced as a result of an intoxicated individual were not significantly different or altered as a result of their blood alcohol level.1 This claim was based upon the fact that the alcohol concentration required to significantly alter the viscosity of blood, leading to an alteration in BPA, was within a range of concentrations up to 1%, which is two times the recognised fatal level. Therefore, the consumption of a dose significant enough to affect analysis would be deadly, and it is highly likely this would never be practically encountered. Additionally, this assumption was not scientifically supported. Research conducted in 1983, prior to MacDonell, studied the effects of alcohol on thrombotic disease5 conducting in vitro and in vivo experiments focusing upon the relationship between alcohol and blood viscosity. It was found that the in vitro addition of alcohol did not significantly change the viscosity of blood at concentrations of 0.1, 0.2, and 0.3% (w/v). However at 0.4% it was found that the viscosity was depressed by 1.2%. Results for the in vivo addition of alcohol showed that on average, a 7.4% increase in blood viscosity occurred after an average of 64 g (1.12 g kg−1 body weight) alcohol consumption. While research involving alcohol in relation to blood is not unknown;5 never before has the effect of drugs on BPA been explored.
Owing to their stimulating mildly hallucinogenic and aphrodisiac properties, amphetamines are extremely popular in certain social settings. The toxic effects of drug use, such as hallucinations and drug induced psychosis, can lead to all forms of aggressive antisocial behaviour, including violence, and therefore this research is enormously relevant within modern-day Forensic Science, and with the misuse of drugs on the rise and the ever-presence of blood at violent crime scenes, with time this study will no doubt become more significant.6 Based on the above insights, we explore for the first time the effects of amphetamine on blood viscosity and estimate the variance caused upon the BPA of drug contaminated stains, concluding whether or not the Forensic use of BPA needs to be reconsidered.
Viscosity measurements were carried out using a capillary tube viscometer (U-Tube Viscometer, Type BS/U, nominal overall length 283 mm, sample volume 13.5 mL, Size C, nominal constant 0.03). The viscometer was filled in a vertical position with the fluid sample and the free flow time of blood from an upper reservoir line to a lower reservoir line measured in seconds. Afterwards, the experimentally determined viscometer constant was used to convert the free flow times into values of dynamic viscosity (mPa.s). All measurements were performed at 37 °C to simulate body temperature. For the purpose of accurate temperature control, the capillary tube viscometer was secured within a transparent glass enclosed bath system, in which the viscometer stood in the same position throughout all tests. A thermostated bath system with a peristaltic pump (Lauda water circulator) was used to maintain a constant temperature but was momentarily turned off during viscosity measurements to eliminate water fluctuations disturbing the viscometer in the form of shaking. Additionally the viscometer was kept away from exposure to direct sunlight or airflow as recommended in previous literature.7 After each successive analysis the viscometer was washed through with hot water, deionised water, and finally acetone before being allowed to air dry.
The viscometer was calibrated using the calibration standard so that the raw data obtained from the tests (free flow time (seconds)) could be accurately converted into dynamic viscosity (mPa.s). The calibration fluid was consequentially run through the viscometer at varying temperatures corresponding to the known viscosity values of the fluid and a calibration plot of ‘run time (seconds)’ verses ‘dynamic viscosity, ‘V’, (mPa.s)’ plotted; producing a highly linear response (seconds = 41.385 [seconds/mPa.s] + 16.515 s; R2 = 0.999). This allows the calibration constant, ‘C’ of the viscometer to be deduced from the following equation:
![]() | (1) |
The blood samples were consequentially spiked with amphetamines and the dynamic viscosities measured. The observed results are depicted in Table 1 and for convenience Fig. 1 presents a graphical representation where it can be readily observed that the presence of amphetamine significantly alters the dynamic viscosity value of defibrinated horse blood. A negative correlation is apparent, suggesting that with increasing amphetamine concentrations a decrease in the viscosity value of blood is observed within the range of 0.5–11.0% (±0.001%: N = 3), which represents a change in dynamic viscosity of between 0.02–0.36 mPa.s respectively. Fig. 2 is a diagrammatical representation that can be summarised to depict that an increase in amphetamine concentration results in an increase in the percentage change of viscosity, resulting in an overall decrease in the dynamic viscosity value of the sample in question.
Amphetamine Concentration/M | Defibrinated Horse Blood | Laked Horse Blood | Corresponding Dose Level | ||
---|---|---|---|---|---|
Dynamic Viscosity/mPa.s | Δ Viscosity Observed/% | Dynamic Viscosity/mPa.s | Δ Viscosity Observed/% | ||
0 | 3.29 | 0.0 | 2.74 | 0.0 | Unadulterated |
3.0 × 10−7 | 3.27 | 0.5 | 2.72 | 0.6 | Therapeutic |
4.1 × 10−6 | 3.15 | 4.1 | 2.70 | 1.5 | Average Dose |
4.1 × 10−5 | 3.12 | 5.1 | 2.67 | 2.4 | Within Fatal Range |
4.1 × 10−4 | 3.09 | 5.7 | 2.66 | 2.8 | Within Fatal Range |
4.1 × 10−3 | 2.93 | 11.0 | 2.65 | 3.4 | Above Fatal Range |
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Fig. 1 Relationship between: log10 amphetamine concentration and log10 viscosity of defibrinated horse blood (square); and laked horse blood (circle). |
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Fig. 2 A diagrammatic representation of the observed increase in percentage change that is apparent with an increase in the concentration of amphetamine within the blood sample. |
Upon detailed analysis of the results shown in Table 1, it is apparent that the addition of an average dose of amphetamine (4.1 × 10−6 mol dm−3)10 to defibrinated horse blood resulted in a decrease in dynamic viscosity of 4.1% representing an alteration from 3.29 to 3.15 mPa.s. Considering the average standard deviation of ±0.001% (N = 3) it can be stated that the decrease in viscosity observed is significant and most probably due to the addition of amphetamine to the defibrinated horse blood rather than experimental deviation. Furthermore, the largest alteration observed within the range tested was a viscosity change of 11.0%, when tests were performed at an amphetamine concentration of 4.1 × 10−3 mol dm−3 (above the believed fatal range),9 however, it must be born in mind that with amphetamine (as well as other narcotics) desensitisation occurs with prolonged use, and therefore doses much higher than those examined here may be encountered, thus the effects within these specific individuals may be higher still.
As expected defibrinated and laked horse blood display similar trends (both exhibit negative correlations), however, these trends are not to the same extent; with the addition of amphetamine laked horse blood exhibits a percentage change corresponding to a decrease in viscosity within the range of 0.6–3.4%, of which is dramatically less than the alterations observed with defibrinated blood (0.5–11.0%). This may likely reflect the extensive pre-treatment of the blood by the manufacturer. We have demonstrated that the addition of amphetamine to horse blood causes a decrease in its dynamic viscosity, thus we now turn our attention to determining whether this variation results in a significant alteration when performing BPA.
When calculating the variances within BPA we understand that the flight characteristics and resultant stain characteristics of blood are a function of its physical properties, viscosity being one of the three most important contributing factors. Due to the properties of blood it is possible to determine the height from which a blood drop has fallen, the direction it was travelling upon impact with a surface, its velocity and the angle at which it impacted.1,14,8 The following equation8 depicts the length and width (or the diameter – which is used to estimate the height or impact velocity) of a vertical impact as a subject of viscosity:
![]() | (2) |
![]() | (3) |
Using eqn (2) we now introduce variable viscosity values (as appropriate to the viscosity change of blood due to the addition of amphetamine) and determine the discrepancy this brings with regards to whether this change is sufficient to mislead BPA experts. The results of this analysis are depicted in Table 2 for determining the final stain diameter, DS which is essential for calculating the drop height and impact velocity of the bloodstain. As identified above, only the results for defibrinated horse blood are considered although similar trends were apparent within the data set of laked horse blood.
Corresponding Dose Level | Dynamic Viscosity of Blood Sample/mPa.s | Final Stain Diameter, DS Calculated/mm | Variation in Calculated Stain Diameter/% |
---|---|---|---|
Unadulterated | 3.29 | 20.94 | 0.0 |
Therapeutic | 3.27 | 20.96 | 0.1 |
Average Dose | 3.15 | 21.17 | 1.0 |
Within Fatal Range | 3.12 | 21.22 | 1.3 |
Within Fatal Range | 3.09 | 21.26 | 1.5 |
Above Fatal Range | 2.93 | 21.55 | 2.9 |
The data presented in Table 2 represents the bloodstain diameters calculated when the alterations within the dynamic viscosity of blood due to the addition of amphetamine are incorporated into eqn (2); these values are also compared to unadulterated blood, based upon the assumption that all other values remain constant. When considering the effects of the average dose (4.1 × 10−6 mol dm−3),10 and the extreme alteration that occurs when an amphetamine concentration of above the fatal range is incorporated (4.1 × 10−3 mol dm−3)9 it is apparent that at these concentrations, amphetamine causes a diameter alteration of 0.23 mm (1.0%) and 0.61 mm (2.9%) respectively, both of which are equivalent to a drop height of ∼6 ft.1 Considering this, upon first appearances one would assume that an alteration of 2.9% is highly significant, however, when taking into consideration that both of the raw data values obtained are equivalent to a drop height of ∼6 ft,1 it would appear that the alteration is not highly significant.
Let us now ‘theoretically’ consider the effect that a change in the viscosity value of blood has upon the stain pattern produced when a single drop impacts upon a solid/smooth angled surface. If we assume that two small droplets of blood are falling through the air under identical conditions such as the same volume, and velocity, except that one of the droplets contains amphetamine, and as shown above has a slightly decreased viscosity, then we can presume that the droplets travel through the air in the same Newtonian motion. The differences between these two spherical blood drops only become apparent when each drop impacts upon the surface.15 As the blood impacts the surface it proceeds to flow in the direction that it was travelling upon impact. The extent to how far the blood flows in a particular direction is dependent upon its angle of impact, velocity and other factors (viscosity). However, upon ceasing momentum, the resultant bloodstain is routinely examined using trigonometry; which incorporates the length and width of the stain to determine the angle ‘θ’ of impact via the following equation:1
![]() | (4) |
Consequentially it would be fair to state that if both of the above blood droplets impacted upon a surface at an identical angle, they would then proceed to exhibit different lengths because of their differences in viscosity. The blood containing amphetamine would have a reduced viscosity and resultantly ‘flow’ a longer distance along the surface before coming to a halt and alternatively the ‘normal’ blood drop would exhibit a slightly more viscous texture and hence cease momentum quicker – resulting in differential stain lengths orientating from the same angle of impact. This concept is diagrammatically represented in Fig. 3 where it is shown that a difference in viscosity will result in an alteration to the length of a stain and as a consequence a different angle of impact will be calculated based upon the calculation in eqn (4). Previous literature has shown viscosity to be an important variable affecting the impact process of fluids upon hard surfaces.15 The theoretical perspective highlighted above is in excellent agreement with Mao et al.,15 who considered the effect of a range of parameters on the spread and rebound of liquid droplets impacting flat surfaces. The authors15 considered (among many) the effect of viscosity upon the impacting process and demonstrated that as the impact droplets reach their maximum spread, the rate of spread reduces and viscosity starts to become significant.15 Additionally a droplet with a high viscosity produces a smaller maximum spread (travel) and consequently has less energy for recoil/rebound than the less viscous blood droplet.15
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Fig. 3 A diagrammatic representation of how the length of a bloodstain is dependent upon the viscosity of the blood in question. |
Considering the data (and theoretical argument) represented above, it is apparent that a change in blood viscosity causes alterations resulting in changes to the calculated angles (theoretically), heights and impact velocities of resultant bloodstains when using BPA to construe these values, and perhaps in light of this revelation one must suggest that this data is highly significant and that the deduced alterations are also significant, meaning they must be accounted for when undertaking BPA interpretation. However, questions must also be asked whether it is plausible that an alteration by such a small scale (for an average concentration: 0.23 mm) could cause such an immense and inconceivable misinterpretation of evidence, and it is with this that we suggest more research be needed within this field before any audacious claims are made.
Last it is illuminating to consider the possible effect of surface tension when undertaking BPA analysis. The Weber number, We is given by:8
![]() | (5) |
![]() | (6) |
N = 0.76We0.5sin3θ | (7) |
This journal is © The Royal Society of Chemistry 2010 |