Real-time phase-contrast x-ray imaging: a new technique for the study of animal form and function
© Socha et al; licensee BioMed Central Ltd. 2007
Received: 28 January 2007
Accepted: 01 March 2007
Published: 01 March 2007
Despite advances in imaging techniques, real-time visualization of the structure and dynamics of tissues and organs inside small living animals has remained elusive. Recently, we have been using synchrotron x-rays to visualize the internal anatomy of millimeter-sized opaque, living animals. This technique takes advantage of partially-coherent x-rays and diffraction to enable clear visualization of internal soft tissue not viewable via conventional absorption radiography. However, because higher quality images require greater x-ray fluxes, there exists an inherent tradeoff between image quality and tissue damage.
We evaluated the tradeoff between image quality and harm to the animal by determining the impact of targeted synchrotron x-rays on insect physiology, behavior and survival. Using 25 keV x-rays at a flux density of 80 μW/mm-2, high quality video-rate images can be obtained without major detrimental effects on the insects for multiple minutes, a duration sufficient for many physiological studies. At this setting, insects do not heat up. Additionally, we demonstrate the range of uses of synchrotron phase-contrast imaging by showing high-resolution images of internal anatomy and observations of labeled food movement during ingestion and digestion.
Synchrotron x-ray phase contrast imaging has the potential to revolutionize the study of physiology and internal biomechanics in small animals. This is the only generally applicable technique that has the necessary spatial and temporal resolutions, penetrating power, and sensitivity to soft tissue that is required to visualize the internal physiology of living animals on the scale from millimeters to microns.
The ability to visualize the internal anatomy of living animals is fundamental to our understanding of biology and medicine. Although imaging systems for respiratory, circulatory and musculoskeletal systems are available for large animals, real-time visualization of the internal processes of small animals has been limited by scaling factors and imaging technology. In order to visualize internal physiological mechanisms of millimeter-sized animals in real-time, a probe must have the following features: (1) ability to penetrate the opaque exterior, (2) spatial resolution in the 1–10 μm range, (2) temporal resolution below 100 ms, and (4) sensitivity to soft tissue. Visible light microscopy (conventional or confocal) is not broadly applicable for intact, live animals due to animal opacity and size limitations. Near-infrared (NIR) microscopy has been tried, but with limited success due to poor spatial resolution . Magnetic resonance imaging (MRI) has been used to image insects , but the best resolution obtained so far is about 50 μm, and images must be averaged over seconds to minutes. For sufficient penetration, spatial resolution of ultrasound imaging is wavelength-limited  to about 100 μm. Conventional x-ray imaging relies on absorption as the contrast mechanism, which is ineffective at visualizing soft tissue. For example, at 25 keV, the maximum absorption contrast of a 100-μm diameter air-filled trachea in water is only 0.3%, smaller than the Poisson noise for a high-end 16-bit CCD camera (0.4%).
Additional File 1: Rhythmic compressive movements in the tracheal system in the carabid beetle Platynus decentis, demonstrating the utility of phase-contrast synchrotron imaging for studies of respiratory dynamics in small animals. View (1.3 × 1.0 mm) is a dorsoventral projection through prothorax of a beetle (mass ~ 45 mg) using monochromatic x-rays (25 keV). The midline of the beetle lies on the right side of the video between the two coxae (large circular structures, bottom right). Collapse and reinflation of the air-filled tracheal tubes can be seen in the majority of the tubes in view. The smallest tracheal tubes that can be seen are about 10 μm in diameter; tracheoles (<1 μm diameter) are too small to be resolved. The circle and dark opaque spots the upper right are an air bubble and particles in the esophagus, respectively; note that they move anteriorly and posteriorly during the compression of the tracheal tubes. The white and dark spots that do not move with the beetle movement are artifacts due to the incident beam and detector system. (MOV 3 MB)
Additional file 2: Passage of food bolus through the esophagus of the butterfly Pieris rapae. View (1.3 × 1.0 mm) is a lateral projection through the thorax of the butterfly (mass ~50 mg), with food moving from anterior (upper right) to posterior (lower left). The butterfly was feeding on a mixture of sugar water and iodine compound (Isovue). X-ray energy (33.2 keV) was tuned just above the K-edge for iodine, making the food bolus appear dark. This clip demonstrates how synchrotron imaging can be used to visualize internal food transport during feeding in small animals. Note that the esophagus is collapsed until the bolus passes through; the light structure running along the same diagonal axis is a tracheal tube. From this clip, it can be seen that the bolus is tapered at both ends and is transported at a speed of ~1.5 mm/s. (MOV 860 KB)
Additional file 3: Movements of the foregut and gut contents of the carabid beetle Pterostichus stygicus. View (3.3 × 2.5 mm) is a dorsoventral projection through the pterothorax, posterior to the mesocoxae (circular structures seen at top of image). The beetle (mass ~210 mg) was fed macerated larva sprinkled with cadmium powder to increase x-ray (25 keV) absorption contrast; the gut boundaries and food movement can only be seen in places with cadmium powder. In this sequence, the crop (bag-like structure, center left) is squeezed anteriorly and then slowly settles back into its initial orientation. Mixing movements and peristalsis of the proventriculus (cylindrical structure, right side) can also be seen. Note that the proventriculus is closed, preventing food from moving posteriorly into the midgut. Dark bands on the left side of the video are artifacts from the incident beam. (MOV 9 MB)
The basis of the x-ray phase-contrast imaging described here is Fresnel diffraction. For samples with minimal absorption, true for insects at the x-ray energies used here, the intensity of an image at a distance d downstream of the sample can be approximated by Equation 1 (see also ):
I(x, y) = I inc (1 + 1.3 × 10-6 × d × λ 2 × ∇2 [∫ ρ(x, y, z)dz]) * R(x, y) (1)
A major concern in using synchrotron x-rays to study physiological processes in small animals is the effect of the x-rays on the animal. Radiation causes molecular damage, including protein and lipid oxidation and gene transmutation; however, the effects depend on dose . Previous studies show that fruit flies (Drosophila melanogaster)  and wasps (Habrobracon and Bracon hebetor) [11, 12] temporarily lose motor control after a dose of about 1–2 kGy, but recover to normal behavior within minutes  or hours . At exposures greater than 2.5 kGy, insects do not recover, although it is unclear when death actually occurs . Feeding patterns are affected after 600 (D. melanogaster)  to 1000 Gy (Bracon hebetor Say) . In one study of D. melanogaster receiving doses of 600 Gy, metabolic rates were unaffected one day after irradiation . In summary, the literature suggests that there are no observable physiological effects at doses less than 500 Gy, a temporary loss of motor control is observed after ~1.5 kGy, and a more permanent loss of motor control occurs at doses greater than 2.5 kGy. However, in most prior studies of radiation effects on insects (concerned primarily with insect control  and ageing ), animals have been subjected to full body irradiation; the few studies that examined localized x-rays have used low levels of radiation [16–19]. Thus it is unknown how insects are affected by intense, targeted radiation – such as in a synchrotron x-ray beam – on specific parts of the body. Furthermore, previous studies focused primarily on effects that occur on a relatively long time scale, usually days after irradiation, and few studies have examined immediate radiation effects. This study strives to answer two questions: what combination of x-ray beam parameters optimizes image quality while minimizing damage to the animal? And under these conditions, how much time is available before the insect is negatively impacted? We varied x-ray parameters and used both CO2 emission patterns and motor behaviors as proxy indicators to assess physiological damage in four insect species. In addition, we demonstrate the range of studies that can be addressed using this technique by showing examples of high-resolution still imagery and real-time movement of food during ingestion and digestion.
There is a trade-off between image quality and survivorship: higher quality images require greater exposures to radiation, which result in greater harm to the animal. With our video camera and beamline configurations, we found a satisfactory comprise between image quality and survivorship by using 25 keV x-rays at 80 μW/mm2 flux density (2 × 1010 ph/s/mm2) and 1 m sample-detector distance (hereafter referred as 'nominal' settings). With these settings, insects exhibited no negative behavioral effects for a period of about 5 minutes. X-rays on the insect's head or thorax caused major changes to the respiratory pattern by about 17 minutes (2.4 kGy). With the beam on the abdomen, no significant changes were observed on the respiratory pattern throughout the full 2-hr trials (17.3 kGy), or even in two trials that were extended to 4 hrs (34.5 kGy). No thermal effects of the x-rays were observed. Food transport and gut structures could be clearly seen using labeled food (Figure 1e–l). In cases where tracking food transport was more important than maximizing the clarity of internal anatomy, 33.2 keV x-rays were successfully used to visualize iodine-laced food. Although not explicitly tested, the shorter wavelength of the x-rays at this setting results in lower absorption and therefore lower impact on the animals. We observed insect feeding under irradiation for more than 30 minutes, depending on species and location of the x-rays on the insect.
Figure 3 demonstrates the advantage of phase-contrast imaging over conventional absorption-based imaging. At d = 5 cm, where the phase effects are minimal, image contrast is poor for all energies, consistent with the fact that the absorption is small. For d = 5 cm and E = 15 keV, although some differences due to absorption can be seen, it is the small phase-contrast edge enhancements that make the features easily discernible. At a fixed energy, increasing d clearly increases the image contrast, as predicted by Equation 1. A careful comparison of the image at d = 100 cm with d = 5 or 50 cm shows that the spatial resolution of the d = 100 cm image is poorer: the line widths at the edges of the air sacs are broader in the d = 100 cm image.
Thermal effects due to x-ray irradiation
Measured no-beam metabolic rates and absorbed powers under x-ray irradiation (25 keV, 80 μW/mm2) for the four species studied.
Measured metabolic rate (no-beam, μW)
Measured absorbed power (μW)
2772 ± 248 (N = 2, 1250.0 ± 2.8 mg)
83.5 (head, N = 1, 1258.8 mg)
230 ± 65 (N = 1, 64.3 mg)
26.0 (head, N = 1, 75.1 mg)
441 ± 184 (N = 20, 46.6 ± 9.2 mg)
13.0 (head, N = 2, 40.1 mg)
127 ± 62 (N = 59, 21.4 ± 8.3 mg)
11.7 (head, N = 2, 19.2 ± 5.0 mg)
15.0 (thorax, N = 2, 19.2 ± 5.0 mg)
33.8 (abdomen, N = 2, 19.2 ± 5.0 mg)
31 ± 9 (N = 28, 1.4 ± 0.3 mg)
1.3 (head, N = 2)
X-ray irradiation effects on CO2emission patterns
Time to respiratory signal (TTRS) varied strongly with incident beam power density (Figure 4a); higher power densities resulted in lower TTRS for all species. The one exception was grasshoppers at the highest power density, which showed a higher TTRS than the other species. Figure 4b shows still images taken from the video corresponding to the different incident power densities. Together, Figures 4a and 4b provide a guide for an experimenter to gauge the compromise between image quality and physiological impact.
TTRS dependence on insect mass
Measurements at the nominal beam intensity showed no mass dependence on the TTRS for grasshoppers (N = 9, 13.3–1473.5 mg, Spearman ρ = 0.23, p = 0.51) and ants (N = 14, 8.4–53.7 mg, Spearman ρ = -0.24, p = 0.38). One possible explanation for this lack of pattern is that, in all cases, major portions of the brain were irradiated.
TTRS dependence on x-ray beam location on the insect body
X-ray irradiation effects on motor function
Using simple behavioral assays, we tested for the presence/absence of righting behavior, defensive behavior, and locomotor ability after a fixed duration of x-ray exposure on the head using nominal beam settings (Table 2). No changes in behavior were observed within the first 5 minutes of exposure. During 6–25 minutes of x-ray exposure, ants, beetles and flies progressively lost motor abilities, starting with leg twitches and ranging to full immobility. By contrast, after 2 hrs of exposure, the grasshoppers could still right themselves, hop, feed and fly (and were later observed to mate and lay eggs). One major difference between the grasshoppers and all other insects studied is that, because of their large size, only a part of the grasshopper's head was irradiated as opposed to the entire head in the other taxa. We note that, consistent with other studies [11, 12, 23], the loss of locomotor abilities observed in the insects at lower dosages was temporary, indicating radiation-induced lethargy. In many individuals, we observed recovery minutes to hours later, suggesting that radiation damage was at least partially repairable.
Our measurements show that a major change in CO2 emission pattern, probably indicating major damage to the central nervous system, occurred after about 2.4 kGy when the insect was exposed on the head or thorax. No change in CO2 emission was observed if the x-ray beam was incident on the abdomen. The TTRS was independent of mass and species. In ants, beetles and juvenile grasshoppers whose entire heads were irradiated, a cyclic or discontinuous gas exchange (DGC) CO2 emission pattern  occurred after the RS. Ants have also been shown to exhibit DGC after they are physically decapitated [25, 26], supporting the hypothesis that the x-ray treatment caused major brain damage. In cases where the RS was observed in this study, it is likely that the very high, acute dose of radiation caused profound tissue damage, causing such problems as potassium leakage [27, 28] and leading to effects akin to the 'central nervous system syndrome' known from mammals . One puzzling result is that although grasshoppers were no different in TTRS at some power densities, they showed a surprising degree of behavioral control after long periods of irradiation, suggesting a greater tolerance of x-rays to the head. For these animals, whose heads were larger than the size of the x-ray beam, the positioning of the x-ray beam may have missed or only partially damaged parts of the central nervous system, including the major ganglia controlling respiratory and motor function. In particular, partial control of motor behaviors such as walking occur in ganglia in the thorax [30–32]. Many of the smaller insects received incidental radiation on the thorax due to geometry during nominal 'head only' trials and exhibited motor loss, lending further weight to this hypothesis.
Due to the many factors that contribute to the question of image quality versus survivorship, there is no single set of x-ray parameters that provide an optimal setting. Generally, one would like a very small source size to minimize image blur, and an efficient detector system so that a less intense x-ray beam can be used to maximize survivorship. In practice, for insect physiology, the first question is whether the particular internal dynamic or morphology can be visualized by this technique. Given the particular source and detector that is available, one usually starts with parameters that give superior image quality. Based on our experience with insects, this is usually with an x-ray energy of 10–20 keV and a sample-detector distance of 10–100 cm. After the desired feature is visualized, the experimenter can optimize the system based on the relative importance of image contrast, spatial resolution, and survivorship.
With our commercially available standard NTSC interlaced video camera (30 fps, Cohu 4920) and nominal incident fluxes of 2 × 1010 ph/s/mm2 at 25 keV, a 16.6 ms (1/60 s) exposure time is sufficient to produce a quality image and record many physiological functions. For body functions that require shorter exposure times (e.g., flight), higher incident beam fluxes are necessary (and are available), in which case insect survivorship will be correspondingly reduced. However, in many cases the total time needed to record such rapid phenomena will be lower. Nonetheless, because the current overall detection efficiency is still very low (< 10%) , there is ample room for technological improvement with the development of better detectors. In fact, during the course of this manuscript preparation, we acquired a new video camera with the same pixel numbers and sizes, but with twice the sensitivity; thus, we can now obtain high-quality images with only 1 × 1010 ph/s/mm2 incident beam flux (Figure 4b). This improvement should double the working time (from 5 to 10 minutes) before any x-ray related effect is observed.
Finally, although this study was targeted specifically at insects, these species were chosen primarily as exemplars to introduce the technique to the biological community. Synchrotron x-ray phase contrast imaging is broadly applicable to any organism with features on the micron scale and above. However, we urge caution when exploring new systems with this technique; it is crucial to understand the effects of the radiation on the organism when making biological interpretations.
Synchrotron x-ray phase contrast imaging shows great promise as a powerful new tool for internal visualization in biological and medical research. This is the only generally applicable technique that has the necessary spatial and temporal resolutions, penetrating power, and sensitivity to soft tissue that is required to visualize the internal physiology of small living animals on a scale from millimeters to microns. The impact of this technique is just beginning to be seen as it is applied to some of the more easily arranged experiments such as those on the respiratory systems of insects, where it has already had a major impact. The discovery of rhythmic tracheal compressive movements in taxa in which it was previously unknown  has opened whole new areas of research, for example those aimed at determining morphological mechanisms of compression and the role of associated convection in insect physiology and evolution. Another exciting possibility is the visualization of previously unknown, complex circulatory patterns within insects that have only been inferred before from changes in body surface temperature .
Current uses of the technique include the analysis of the rapidly moving internal mouthparts of biting insects and the visualization of fluid motion in the pumping organs of fluid feeding insects such as flies and butterflies. The ability to see inside the animal, including the internal workings of jaws, legs, and wing hinges, may be of significant utility in the exploration of functional diversity. Although more challenging due to lower density differences, this approach has also yielded impressive x-ray video of insect digestive (Figure 1e–l; see also Additional files 2 and 3) and circulatory system function, including the pumping of the tiny pulsatile organs that maintain the internal pressure of the antennae of ants. The first synchrotron research on living vertebrate musculoskeletal systems has recently begun with successful video of the interior bones of the pharynx and skull during fish respiratory pumping. The potential for investigation of model systems in genetics and medicine such as fly, zebrafish, and mouse is considerable, as the natural and normal mechanisms of heart, circulatory, digestive, and locomotor systems can be analyzed in new ways and compared to mutants or disease models that may be used to study human health concerns. Ultimately, the ability to clearly visualize internal functions in small animals will have a large impact in both biology and medicine.
Synchrotron x-ray phase-contrast imaging
Experiments were performed at the XOR-1ID and XOR-32ID undulator beamlines at the Advanced Photon Source (Figure 2). Synchrotron x-rays are produced here by a source with full-width half maximum dimensions of 35 μm (vertical) by 560 μm (horizontal) and source-to-sample distances of 60 m and 40 m, respectively. A Si (111) double crystal monochromator was used to select the x-ray wavelength. The incident beam flux (photons/s/mm2) was changed by varying the undulator magnetic gap and was monitored with an upstream ion chamber. Insects were mounted on top of a remotely controlled stage that enabled precise positioning in the x-ray beam. After passing through the insect, the x-rays were converted to visible light via a cerium doped yttrium aluminum garnet scintillator. The sample-to-scintillator distance was approximately 1 m; a distance of this magnitude is necessary for obtaining the phase-contrast effect. The visible light created by the scintillator was imaged onto a video camera (Cohu 4920 or Cohu 2700, Cohu, San Diego, CA, USA) or higher resolution CCD camera (SensiCam QE, Cooke, Romulus, MI, USA) using a 2× or 5× microscope objective. The field of view was 2.4 mm × 3.2 mm and 1.0 mm × 1.3 mm for the 2× and 5× objectives, respectively. Unlike most prior studies, the size of the x-ray beam was comparable to the size of the insect, and we only exposed parts of the insect to radiation.
We conducted the majority of our experiments on carpenter ant workers (Camponotus pennsylvanicus, n = 59), but also explored taxonomic diversity by examining beetles (Platynus decentis, n = 20), fruit flies (Drosophila virilis, n = 28), and grasshoppers (Schistocerca gregaria, n = 19). Ants and fruit flies were purchased from Carolina Biological Supply Company (NC, USA). Beetles were collected in the woods at Argonne National Laboratory, and grasshoppers were reared at one of the author's laboratory (JH). Insects were housed with free access to food and water prior to experimentation.
Survivorship and behavior
To determine the length of time that insects could withstand radiation on a particular part of the body (head, thorax, or abdomen), insects were monitored for CO2 release using flow-through respirometry while being observed with x-rays (Figure 2b). Insects were cold anaesthetized and placed individually in custom plexiglass respirometry chambers (volumes: 0.03, 0.25, 1.0, and 9.5 ml) with Kapton (Dupont, DE, USA) windows for x-ray transmission (Figure 2c). Because some insects actively moved away from the beam upon contact, cotton was used to fill in gaps within the chamber to constrain the insect within the field of view. The chambers were oriented such that the long axis of the body lay perpendicular to the beam path, providing either lateral or dorsoventral views.
CO2 emission was monitored by a flow-through respirometry system from Sable Systems International (SSI, Las Vegas, NV, USA). Room air was scrubbed of CO2 and H2O using a Drierite/Ascarite/Drierite column and pushed through the system using a pump (TR-SS3, SSI). Flow rate (100 ml/min for all species except D. virilis, 50 ml/min) was maintained via a mass flow controller (SSI MFC-2 using a Sierra Instruments mass flow control valve). CO2 exiting the insect chamber was measured by a gas analyzer (LI-7000, Li-Cor, Lincoln, NE, USA). Chamber washout times were on the order of 6–12 s. CO2 data were output to a computer via UI-2 (SSI) and recorded using ExpeData software (SSI). Pre-beam CO2 emission was typically recorded for 5–10 minutes before opening the x-ray shutter. For survivorship trials, insects were exposed to x-rays on the head, thorax, or abdomen until they clearly showed a respiratory signature that we infer to be respiratory function damage; otherwise, trials were ended after 2 hrs. CO2 emission was also monitored post-beam for up to 30 minutes. For behavioral trials, the insects were exposed for a fixed amount of time, then removed from the chamber and tested for the presence/absence of righting behavior, defensive behavior, and locomotor ability. All trials were conducted at room temperature (21–22°C). Data were analyzed using ExpeData and LabAnalyst X (Mark Chappell, University of California Riverside, CA, USA) software packages.
To demonstrate the use of x-rays to visualize internal food movement during ingestion and digestion, beetles (Platynus decentis) were fed macerated insects mixed with fine particles of CdWO4, and butterflies (Pieris rapae) were fed sugar solutions laced with an iodine contrast agent (Isovue, Bracco Diagnostics, NJ, USA). Animals were held in place by securing the body to a microscope cover slip (beetles) or by a mounted clamp attached to the wings (butterflies). These examples illustrate the use of contrast agents to visualize internal food transport. The fine particles of CdWO4 had a significantly higher absorption over the entire x-ray energy range used in this study and appeared darker than the surrounding soft tissue. In the case of the iodine solution, differences in x-ray absorption at the nominal setting (25 keV) were minimal. To maximize contrast between the iodine and the surrounding anatomy, we used an energy just above the K-absorption edge (33.2 keV for iodine), where absorption increased dramatically. Because in general the use of higher energy x-rays results in an overall lower contrast for soft tissue (Figure 3), this technique is most applicable for cases where it is more important to track internal movements of food than to visualize clearly the surrounding insect anatomy. The use of simultaneous x-ray images above and below the K-edge to improve visualization of the contrast agent is possible, but would require a more complicated set of x-ray optics. Furthermore, it would imply a doubling of the x-ray dose to the animal.
For contrast agents, iodine is more suitable for fluids whereas CdWO4 is more suitable for solids. Although we have not investigated the toxicity of iodine versus CdWO4 in insects, we speculate that iodine is less harmful because Isovue is used for human medical diagnosis, and it is well known that cadmium is toxic . We chose a cadmium compound for its convenience, but other high electron density materials in powder form (such as silica or lead) can be used to provide radio-opacity with lower toxicity.
Possible change in temperature in the insect due to the absorption of x-rays was measured separately with two methods. First, an implanted 0.01 mm copper-constantan thermocouple and thermocouple thermometer (0.1 K resolution, Physitemp Instruments, Inc., NY, USA) were used to measure internal abdominal temperature in an adult grasshopper (Schistocerca gregaria) while it was irradiated for up to 10 minutes on the thorax. To test if local heating occurred at the site of irradiation, an infrared camera (Inframetrics 760, 0.1 K resolution, American Infrared, NY, USA) was used to visualize temperature change in the head of three beetles (Platynus decentis) and one grasshopper (Schistocerca gregaria).
We used two metrics to quantify the effect of the x-rays on the CO2 emission patterns. To assess immediate effects of the beam, we compared CO2 emission rates in the 2 minutes before 'beam on' to those 2 minutes after 'beam on' (Equation 2). We defined the ratio (R 2 min ) as:
where 〈E pre-beam 〉2 min and 〈E beam-on 〉2 min are, respectively, the CO2 emission rates (μl/hr) averaged over the 2 minutes immediately prior and after the x-rays (25 keV) were turned on. Second, to assess the duration required for damage to occur due to x-rays, we identified a major change in the CO2 emission pattern within each species, which we refer to as the respiratory signature (RS; Figure 6). The RS was chosen for its repeatability; by the time of the RS, major (and likely irreversible) damage has occurred. This time interval, between when the beam first hit the insect and the RS, is the time to respiratory signature (TTRS).
Image quality and the corresponding photon fluxes and average power densities for 25 keV x-rays used in this study are shown in Figure 4. The incident photon fluxes were chosen for an approximate factor of two change in intensity between each setting. At 25 keV, a 1-mm thick water sample (over the entire beam area) would absorb about 3% of the incident beam energy . Absorbed power for a volume of insect that is irradiated can thus be estimated by Equation 3:
Absorbed power = 0.03 × D × V (3)
Effect of duration of x-ray exposure to head on motor control abilities. m/n denotes m animals behaving normally out of n animal trials. Asterisks denote partially limited response (e.g., slow response).
Exposure time (min) with 25 keV x-rays, 80 μW/mm 2
Metabolic rate calculations were based on averages of all available prebeam CO2 recordings for each of the four species. Conversion from CO2 output to metabolic rate assumed respiratory quotients (RQ) of 1.0, 0.8, 0.7, and 1.0 and energy equivalences of 20.1, 24.5, 27.6 and 21.2 J/ml of CO2 for grasshoppers , beetles , ants , and fruit flies , respectively.
discontinuous gas exchange
incident beam power density
- Iinc :
incident beam intensity
- R(x, y):
effective detector resolution
time to respiratory signal
We thank Kamel Fezzaa and Aaron Rice with help in collecting data, John Lighton, Barbara Joos, and Robbin Turner of Sable Systems International (SSI) for assistance with respirometry equipment, Kendra Greenlee for help with the thermocouple thermometry, and Jim Liebherr for help with identification of beetle internal anatomy. Use of the Advanced Photon Source was supported by the U. S. Department of Energy, Office of Science, Office of Basic Energy Sciences, under Contract No. W-31-109-ENG-38. Harrison's work at ANL was supported by NSF IBN-9985857 and IBN 0419704.
- Ridgway C, Chambers J: Detection of insects inside wheat kernels by NIR imaging. J Near Infrared Spectroscopy. 1998, 6: 115-119.View ArticleGoogle Scholar
- Hart AG, Bowtell RW, Kockenberger W, Wenseleers T, Ratnieks FLW: Magnetic resonance imaging in entomology: a critical review. J Insect Sci. 2003, 3: 5-PubMed CentralView ArticlePubMedGoogle Scholar
- Harris RA, Follett DH, Halliwell M, Wells PNT: Ultimate limits in ultrasonic imaging resolution. Ultrasound Med Biol. 1991, 17: 547-558. 10.1016/0301-5629(91)90025-R.View ArticlePubMedGoogle Scholar
- Cloetens P, Barrett R, Baruchel J, Guigay JP, Schlenker M: Phase objects in synchrotron radiation hard x-ray imaging. J Phys D: App Phys. 1996, 29: 133-146. 10.1088/0022-3727/29/1/023.View ArticleGoogle Scholar
- Snigirev A, Snigireva I, Kohn V, Kuznetsov S, Schelokov I: On the possibilities of x-ray phase contrast microimaging by coherent high-energy synchrotron radiation. Rev Sci Inst. 1995, 66: 5486-5492. 10.1063/1.1146073.View ArticleGoogle Scholar
- Westneat MW, Betz O, Blob RW, Fezzaa K, Cooper WJ, Lee WK: Tracheal respiration in insects visualized with synchrotron x-ray imaging. Science. 2003, 299: 558-560. 10.1126/science.1078008.View ArticlePubMedGoogle Scholar
- Herford GM: Tracheal pulsation in the flea. J Exp Biol. 1938, 15: 327-338.Google Scholar
- Cowley JM: Diffraction Physics. 1995, Amsterdam: Elsevier, ThirdGoogle Scholar
- Grosch DS: Entomological aspects of radiation as related to genetics and physiology. Ann Rev Entomol. 1962, 7: 81-106. 10.1146/annurev.en.07.010162.000501.View ArticleGoogle Scholar
- Megumi T, Gamo S, Ohonishi T, Tanaka Y: Induction of leg-shaking, knock-down and killing responses by gamma-ray irradiation in Shaker mutants of Drosophila melanogaster. J Rad Res. 1995, 36: 134-142.View ArticleGoogle Scholar
- Grosch DS: Induced lethargy and the radiation control of insects. J Econ Entomol. 1956, 49: 629-631.View ArticleGoogle Scholar
- Heidenthal G: The occurrence of x-ray induced dominant lethal mutations in Habrobracon. Genetics. 1945, 30: 197-205.PubMed CentralPubMedGoogle Scholar
- King RC, Wilson LP: Studies of the radiation syndrome in Drosophila melanogaster. Rad Res. 1955, 2: 544-555. 10.2307/3570358.View ArticleGoogle Scholar
- Bakri A, Heather N, Hendrichs J, Ferris I: Fifty years of radiation biology in entomology: Lessons learned from IDIDAS. Ann Entomol Soc Am. 2005, 98: 1-12. 10.1603/0013-8746(2005)098[0001:FYORBI]2.0.CO;2.View ArticleGoogle Scholar
- Allen RG, Sohal RS: Life-lengthening effects of gamma radiation on the adult housefly, Musca domestica. Mech Age Dev. 1982, 20: 369-375. 10.1016/0047-6374(82)90104-X.View ArticleGoogle Scholar
- Baldwin WF, Salthouse TN: Latent radiation damage and synchronous cell division in the epidermis of an insect. I. Nonreversible effects leading to local radiation burns. Rad Res. 1959, 10: 387-396. 10.2307/3570829.View ArticleGoogle Scholar
- Baldwin WF, Sutherland JB: Extreme sensitivity to low-level X-rays in the eye of the cockroach Blaberus. Rad Res. 1965, 24: 513-518. 10.2307/3571642.View ArticleGoogle Scholar
- Lee WR: Partial body radiation of queen honeybee. J Apic Res. 1964, 3: 113-116.Google Scholar
- Pijnacker LP: Effects of X-rays on different meiotic stages of oocytes in the parthenogenetic stick insect Carausius morosus Br. Mut Res. 1971, 13: 251-262.View ArticleGoogle Scholar
- Lighton JRB, Turner RJ: Thermolimit respirometry: an objective assessment of critical thermal maxima in two sympatric desert harvester ants, Pogonomyrmex rugosus and P. californicus. J Exp Biol. 2004, 207: 1903-1913. 10.1242/jeb.00970.View ArticlePubMedGoogle Scholar
- Lighton JRB: Discontinuous gas exchange in insects. Ann Rev Entomol. 1996, 41: 309-324. 10.1146/annurev.en.41.010196.001521.View ArticleGoogle Scholar
- Miller PL: The regulation of breathing in insects. Advances in Insect Physiology. Edited by: Beament JWL, Treherne JE, Wigglesworth VB. 1966, London and New York: Academic Press, 3: 279-354.Google Scholar
- Cheng CC, Ducoff HS: High-dose mode of death in Tribolium. Entomol Exp App. 1989, 51: 189-197. 10.1007/BF00186737.View ArticleGoogle Scholar
- Marais E, Klok CJ, Terblanche JS, Chown SL: Insect gas exchange patterns: a phylogenetic perspective. J Exp Biol. 2005, 208: 4495-4507. 10.1242/jeb.01928.View ArticlePubMedGoogle Scholar
- Lighton JRB: Direct measurement of mass loss during discontinuous ventilation in two species of ants. J Exp Biol. 1992, 173: 289-293.Google Scholar
- Lighton JRB, Fukushi T, Wehner R: Ventilation in Cataglyphis bicolor : regulation of carbon dioxide release from the thoracic and abdominal spiracles. J Insect Phys. 1993, 39: 687-699. 10.1016/0022-1910(93)90074-2.View ArticleGoogle Scholar
- Ducoff HS: Causes of death in irradiated adult insects. Biol Rev Cam Phil Soc. 1972, 47: 211-240.View ArticleGoogle Scholar
- Pribush A, Agam G, Yermiahu T, Dvilansky A, Meyerstein D, Meyerstein N: Radiation damage to the erythrocyte membrane – the effects of medium and cell concentrations. Free Rad Res. 1994, 21: 135-146.View ArticleGoogle Scholar
- Edwards AA, Lloyd DC: Risks from ionising radiation: deterministic effects. J Rad Protn. 1998, 18: 175-183. 10.1088/0952-4746/18/3/004.View ArticleGoogle Scholar
- Gal R, Libersat F: New vistas on the initiation and maintenance of insect motor behaviors revealed by specific lesions of the head ganglia. J Comp Phys A: Neur Sens Neur Behav Phys. 2006, 192: 1003-1020. 10.1007/s00359-006-0135-4.View ArticleGoogle Scholar
- Ridgel AL, Ritzmann RE: Effects of neck and circumoesophageal connective lesions on posture and locomotion in the cockroach. J Comp Phys A: Neur Sens Neur Behav Phys. 2005, 191: 559-573. 10.1007/s00359-005-0621-0.View ArticleGoogle Scholar
- Burrows M: The Neurobiology of an Insect Brain. 1996, New York: Oxford University PressView ArticleGoogle Scholar
- Gruner SM, Tate MW, Eikenberry EF: Charge-coupled device area x-ray detectors. Rev Sci Inst. 2002, 73: 2815-2842. 10.1063/1.1488674.View ArticleGoogle Scholar
- Wasserthal LT: Interaction of circulation and tracheal ventilation in holometabolous insects. Advances in Insect Physiology. Edited by: Evans PD. 1996, San Diego: Academic Press, 298-351.Google Scholar
- Occupational Safety and Health Administration. 1996, [http://www.osha.gov/]
- Hubbel JH, Seltzer SM: Tables of X-ray Mass Attenuation Coefficients and Mass Energy-Absorption Coefficients 1 keV to 20 MeV for Elements Z = 1 to 92 and 48 Additional Substances of Dosimetric Interest. Nat Inst Stand. 1995, NISTIR 5632.Google Scholar
- Greenlee KJ, Harrison JF: Development of respiratory function in the American locust Schistocerca americana I. Across-instar effects. J Exp Biol. 2004, 207: 497-508. 10.1242/jeb.00767.View ArticlePubMedGoogle Scholar
- Schmidt-Nielsen K: Animal Physiology: Adaptation and Environment. 1980, Cambridge: Cambridge University Press, 2Google Scholar
- Lighton JRB, Wehner R: Ventilation and respiratory metabolism in the thermophilic desert ant, Cataglyphis bicolor (Hymenoptera, Formicidae). J Comp Phys B: Biochem Syst Env Phys. 1993, 163: 11-17.View ArticleGoogle Scholar
- Van Voorhies WA, Khazaeli AA, Curtsinger JW: Long-lived Drosophila melanogaster lines exhibit normal metabolic rates. J App Phys. 2003, 95: 2605-2613.View ArticleGoogle Scholar
- Yahiro K: A comparative morphology of the alimentary canal in adults of ground-beetles (Coleoptera) I. Classification into the types. Esakia. 1990, 1: 35-44.Google Scholar
This article is published under license to BioMed Central Ltd. This is an Open Access article distributed under the terms of the Creative Commons Attribution License (http://creativecommons.org/licenses/by/2.0), which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.