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Biomedical subjects

B C Wilson

Publications and source records attributed to B C Wilson.

At least 73 records · Page 4Linked to original sources
PubMed1994

Effects of exogenous relaxin on oxytocin and vasopressin release and the intramammary pressure response to central hyperosmotic challenge.

Experiments were done to study the effects of porcine relaxin on osmotically evoked changes in intramammary pressure and the release of oxytocin and vasopressin in anaesthetized rats. Injections (1 microliter) of hypertonic (0.75 M) NaCl into the left lateral cerebral ventricle were used to induce consistent rises in intramammary pressure and the release of oxytocin and vasopressin. Plasma hormone concentration was determined by radioimmunoassay. Relaxin (5 micrograms i.v.) significantly (P < 0.05) suppressed the intramammary pressure response to osmotic challenge 5 and 10 min after treatment. However, pretreatment with a specific vasopressin V1 receptor antagonist completely negated the effect of relaxin on intramammary pressure. Baseline levels of oxytocin and vasopressin in unstimulated rats were 41 +/- 1.6 and 36 +/- 1.1 pmol/l respectively. Osmotic challenge induced significant (P < 0.05) rises in plasma levels of both hormones (62.8 +/- 1.1 and 67.9 +/- 1.2 pmol/l respectively) which were further augmented by relaxin (81.3 +/- 1.8 and 117.1 +/- 2.4 pmol/l respectively; P < 0.05). The data confirm that central osmotic challenge provokes the release of oxytocin and vasopressin but the effects of oxytocin at the level of the mammary gland may be obscured by the action of vasopressin affecting blood flow to the gland.

Animals↗
PubMed1993

Mitochondrial alterations in photodynamic therapy-resistant cells.

The characterization of radiation-induced fibrosarcoma cells (RIF-8A) which have been selected for resistance to Photofrin-mediated photodynamic therapy (PDT) is detailed in this report. Morphological and functional assessment of mitochondria in both the resistant RIF-8A and parental RIF-1 cells show distinct differences. Electron micrographs show that the mitochondria in the RIF-8A cells are relatively smaller; stain more densely, and display a higher cristae density than RIF-1 cells. P. A. Andrews et al. (Cancer Res., 52: 1895-1901, 1992) reported similar mitochondrial differences between a human ovarian carcinoma cell line, 2008, and its cisplatin-resistant counterpart (C13*). Dose-response curves demonstrate that these cisplatin-resistant C13* cells show cross-resistance to Photofrin-mediated PDT. Functionally, the RIF-8A cells produce more ATP and demonstrate higher succinate dehydrogenase activity than do the RIF-1 cells, but the rates of oxygen consumption do not differ between the two cell types. The PDT-sensitive RIF-1 cells demonstrate a significantly higher susceptibility to inhibition of glycolytic activity as determined by 2-deoxy-d-glucose survival curves. These findings suggest differences in the efficacy and/or mode(s) of energy production in the RIF-1 and RIF-8A cells. Since mitochondria are sensitive targets for porphyrin-mediated PDT, the observed changes in mitochondrial structure and/or function may be involved in the PDT resistance seen in RIF-8A cells.

Adenosine Triphosphate↗
PubMed1993

Comparison of magnetic resonance images and the histopathological findings of lesions induced by interstitial laser photocoagulation in the brain.

Interest has developed in using magnetic resonance (MR) imaging to monitor the volume of tissue destroyed by interstitial laser photocoagulation (ILP). In these experiments, ILP was induced in the normal brains of 9 anesthetized cats by delivering 1.5 W of continuous-wave Nd:YAG laser energy (1,064 nm) from a single 400-microns core optical fiber for 1,000 s. The irradiations were monitored using proton spin-echo MR imaging during and immediately after ILP and at postirradiation survival times of 2, 5, and 14 days. At 2 days postirradiation, the necrotic thermal lesion consisted of a central cavity surrounded by 2 concentric zones of coagulative necrosis, one dense and the other dispersed. The lesion shrank and the zonal appearance became less obvious over the 14 day survival period. An enhancing halo on contrast-enhanced T1-weighted images acquired immediately postirradiation best approximated the total lesion diameter at 2 days. These images also indicated that the volume of tissue destroyed during ILP corresponded better to the necrotic volume determined at 2 days than at 5 days and 14 days postirradiation. T2-weighted images acquired during and immediately after ILP consistently underestimated the total lesion diameter at 2 days.

Animals↗
PubMed1993

Miniature isotropic optical fibre probes for quantitative light dosimetry in tissue.

A small detector to measure light fluence rates in turbid media and biological tissue, based on an optical fibre with a fluorescent dye-doped tip, is presented. The measured optical power of the fluorescent light transmitted through the fibre is directly proportional to the local fluence rate of the treatment or excitation light at the tip. The detector has been built as small as 170 microns outer diameter, while retaining good mechanical properties for insertion into soft tissue. The detector response is linear with fluence rate over a wide range and isotropic for all angles less than 160 degrees from the forward direction. Hence, the detector can measure accurately the fluence rate in turbid media and biological tissue. This fluorescent tip design has no fundamental restrictions in size and shows comparable isotropy, but is less sensitive than, fluence rate detectors based on optical fibres with light-scattering tips.

Fiber Optic Technology↗
PubMed1992

Magnetic resonance imaging of interstitial laser photocoagulation in brain.

Magnetic resonance (MR) imaging can be used to monitor the development of thermal lesions induced in tissue using interstitial laser photocoagulation (ILP). A potential application for ILP is the treatment of surgically inaccessible brain tumors. For the successful clinical application of MR-monitored ILP, it is necessary to relate MR images of ILP lesions to the actual induced lesions. In this preliminary study we performed ILP in the normal brains of anesthetized cats by delivering interstitially 1.0, 1.5, and 2.0 W of continuous-wave Nd:YAG laser energy (1,064 nm) for 1,000 s via a plane-cut 400 microns core optical fiber. At 48 h post-irradiation the lesions consisted of four sharply demarcated concentric zones of thermal damage. Lesion diameter increased linearly with delivered power. T2-weighted proton spin-echo images acquired during ILP showed a region of complete or near signal loss that underestimated the actual lesion at 48 h. Gadolinium-enhanced T1-weighted spin-echo images acquired immediately post-irradiation showed the actual lesion precisely.

Animals↗
PubMed1992

Optical properties of Intralipid: a phantom medium for light propagation studies.

Intralipid is an intravenous nutrient consisting of an emulsion of phospholipid micelles and water. Because Intralipid is turbid and has no strong absorption bands in the visible region of the electromagnetic spectrum, and is readily available and relatively inexpensive, it is often used as a tissue simulating phantom medium in light dosimetry experiments. In order to assist investigators requiring a controllable medium that over a finite range of wavelengths is optically equivalent to tissue, we have compiled previously published values of the optical interaction coefficients of Intralipid, most of which were measured at a wavelength of 633 nm. We have extended the measurements of the absorption and reduced scattering coefficients from 460 to 690 nm and the total attenuation coefficient from 500 to 890 nm. These measurements show that, for stock 10% Intralipid, the absorption coefficient varies from 0.015 to 0.001 cm-1 between 460 and 690 nm, the reduced scattering coefficient varies from 92 to 50 cm-1 between 460 and 690 nm, the total attenuation coefficient varies from 575 to 150 cm-1 between 500 and 890 nm, and the average cosine of scatter varies from 0.87 to 0.82 between 460 and 690 nm. With these data, we discuss the design of an optically tissue-equivalent phantom consisting of Intralipid and black India ink.

Absorption↗
PubMed1992

Interstitial laser photocoagulation: Nd:YAG 1064 nm optical fiber source compared to point heat source.

Interstitial laser photocoagulation (ILP) was performed in vitro in lean bovine and chicken muscle by delivering 1.6 W of continuous-wave Nd:YAG laser energy (1064 nm) from a 400-microns core optical fiber for 300s. The resulting thermal coagulation lesion was consistently larger when the delivered energy was deposited into a small steel sphere than when it was delivered freely into the tissue. Mathematical modelling confirms this result. This preliminary study suggests that a point heat source produces a larger volume of thermal coagulation than a point optical source (1064 nm) delivering the same power.

Animals↗
PubMed1992

Determination of optical properties of turbid media using pulsed photothermal radiometry.

Pulsed photothermal radiometry (PPTR) measures blackbody radiation emitted by a sample after absorption of an optical pulse. Three techniques for obtaining the absorption coefficient of absorbing-only, semi-infinite samples are examined and shown to give comparable results. An analytic theory for the time dependence of the PPTR signal in semi-infinite scattering and absorbing media has been derived and tested in a series of controlled gel phantoms. This theory, based on the diffusion approximation of the radiative transport equation, is shown to model the time course of the detected signal accurately. Furthermore, when the incident fluence is known, the theory can be used in a non-linear, two-parameter fitting algorithm to determine the absorption and reduced scattering coefficients of a turbid sample with an accuracy of 10-15% for transport albedos ranging from 0.42-0.88.

Algorithms↗
PubMed1992

Sonographic changes during hepatic interstitial laser photocoagulation. An investigation of three optical fiber tips.

RATIONALE AND OBJECTIVES: Interstitial laser photocoagulation (ILP) destroys tumors thermally, using laser energy delivered from implanted optical fibers. The objectives of the study are to identify a fiber tip/delivered energy combination which produces lesions of useful size, visible on ultrasound (US) during ILP, and to compare ILP lesions and their US images. METHODS: Hepatic ILP was performed at laparotomy in six pigs, using three different fiber tips (cylindrical diffusing, spherical diffusing, plane-cut). US images were obtained during ILP, immediately after ("early" images), and before the animals were killed (2-2.5 hours, "late" images). Actual lesions were assessed histopathologically. RESULTS: Few US changes were seen around cylindrical diffusing and spherical diffusing tips until tip destruction. Plane-cut tips, at 1.5 to 2.0 W, produced prominent US images of the 1- to 2-cm thermal lesions. Early images tended to overestimate necrosis. Late images approximated necrosis. CONCLUSION: For US-controlled ILP, plane-cut tips are better than currently available cylindrical diffusing or spherical diffusing tips. Lesion image growth periods might enable control of lesion size. Further studies are needed to determine the consistency of the described relationship between lesion images and actual lesions.

Animals↗
PubMed1992

Effects of light beam size on fluence distribution and depth of necrosis in superficially applied photodynamic therapy of normal rat brain.

The light fluence distributions of 632.8 nm light incident on the exposed surface of normal rat brain in vivo have been measured using an interstitial, stereotactically-mounted optical fiber detector with isotropic response. The dependence of the relative fluence rate on depth and the spatial distribution of fluence were compared for incident beam diameters of 3 and 5 mm. The fluence rate at depth of 1-6 mm along the optical axis within the brain tissue was approximately 70% greater for a 5 mm diameter beam than for a 3 mm beam, at the same incident fluence rate, although the plots of the relative fluence rate vs depth were parallel over the depth range 1-6 mm. The depths of necrosis resulting from photodynamic treatment of brain tissue using the photosensitizer Photofrin and irradiation by 632 nm light with 3 and 5 mm incident beams were also measured. The observed difference in necrosis depths was consistent with the measured difference in fluence. The importance of beam size in photodynamic treatment with small diameter incident light fields is discussed.

Animals↗
PubMed1992

The effect of light fluence rate in photodynamic therapy of normal rat brain.

This paper reports the effect of incident light fluence rate on the depth to which necrotic lesions are produced by photodynamic therapy (PDT) in the brains of normal Fisher rats. The rats were injected intraperitoneally with Photofrin (12.5 mg kg-1) 48 h prior to PDT with a fixed incident fluence of 35 J cm-2. The treatment was performed at 10, 50, 100, and 200 mW cm-2 and also in a periodic manner (30 s "on" at 100 mW cm-2, 30 s "off"). The depth to which necrosis occurred was determined 24 h after treatment by microscopic examination of tissue sections. No differences were found in the depth to which necrosis was produced by any of the five irradiation schedules. This finding is discussed in the context of other published dose-rate experiments.

Animals↗
PubMed1991

Use of photodynamic therapy in the palliation of massive advanced rectal cancer. Phase I/II study.

Photodynamic therapy (PDT) is a relatively new form of cancer therapy utilizing a photosensitizer such as hematoporphyrin derivative. We conducted a pilot study to determine the efficacy of its use in palliating advanced rectal cancer, to determine toxicity, and to establish objective outcome criteria. Six patients with very advanced, usually recurrent rectal cancer were treated with PDT after being photosensitized with Photofrin II. A protocol was established to measure clinical and radiologic response to therapy. A new intraluminal delivery system was incorporated. Five patients had both clinical and radiologic responses to therapy. In two patients we observed such significant responses that they cannot be accounted for on a photobiologic basis alone. One patient developed a significant sunburn after discharge. There was no major toxicity of bleeding or sepsis even at maximum doses (200 J/cm2). We are confident that PDT has a role to play in rectal cancer and speculate as to future applications.

Adenocarcinoma↗
PubMed1991

A control method for a nonlinear multivariable system: application to interstitial laser hyperthermia.

An original adaptive control method is presented for controlling a nonlinear multivariable system. The method, which could be described as a modified quasi-linear approach, involves dividing the source excitation into a series of pulsing rounds and is implemented as a control algorithm on a computer. The theory underlying the method is developed with reference to an application involving temperature control in interstitial laser hyperthermia. In this application, the method is both successful and necessary to achieve optimally uniform elevated temperatures in a ground beef phantom. Apart from variable and parameter definitions, the method is otherwise general and might be useful for controlling a nonlinear system in which no prior exact characterization of the system is possible. Simulations were conducted to assess the effectiveness of the method in systems for which the unit excitation response changes by factors ranging from zero to three over the total period of excitation. In each case the method has proven stable.

Algorithms↗