Immunomodulation by shark cartilage extracts

The immune system is composed of innate and adaptive mechanisms. Innate immune responses are significantly modulated by immunomodulatory factors that act through the induction of specific patterns of cytokine production in responding cells. Human leukocytes have been shown to respond to substance(s) present in acid extracts of commercial shark cartilage (SC). Shark cartilage is a food supplement taken by consumers as a prophylaxis and for the treatment of conditions ranging from arthritis to cancer. No reliable scientific evidence in the literature supports the alleged usefulness of shark cartilage supplements, but their use remains popular. Cartilage extracts exhibit immunomodulatory properties by inducing various inflammatory, Th1-type cytokines and potent chemokines in human peripheral blood leukocytes (HPBL) in vitro. The objectives of the study were to (1) to determine the nature of the active component(s), (2) to define the scope of cellular response to SC extract, and (3) to elucidate the molecular mechanisms underlying bioactivity. Results showed that there are at least two cytokine-inducing components which are acid stable. One anionic component has been identified as a small (14-21 kDa) glycoprotein with at least 40% carbohydrate content. Shark cartilage stimulated HPBL to produce cytokines resembling an inflammatory, Th1 polarized response. Leukocyte-specific responses consist of both initial cytokine responses to SC directly (i.e., TNF-α) and secondary responses such as the IFN-γ response by lymphocytes following initial SC stimulation. Response of RAW cells, a murine macrophage cell line, indicated that TNF-á could be induced in macrophages of another mammalian species in the absence of other cell types. The results suggest that the human monocyte/macrophage is most likely to be the initial responding cell to SC stimulation. Stimulation of cells appears to engage at least one ligand-receptor interaction with TLR 4, although the role of TLR 2 cannot be ruled out. Initial activation is likely followed by the activation of the JNK and p38 MAPK signal transduction pathways resulting in activation, release, and translocation of transcription factor nuclear factor κB (Nf-κB). This dissertation research study represents the first in-depth study into characterizing the bioactive component(s) of commercial shark cartilage responsible for its immunomodulating properties and defining cellular responses at the molecular level.

Weak electron scattering for the 3He-3H transition and the weak nuclear form factors

We calculate the differential cross section for weak electron scattering reaction, e + 3He-' 3H + ve, for energies from 100 MeV to 6 GeV as a function of outgoing nucleus angle from 0 to n/2 radians. We find that the differential cross section at low [q2] increases with electron energy from 0.1 GeV to 6.0 GeV, such that the peak value at 6.0 GeV is approximately 3.2 x 10-40 cm 2 / ster, a factor of 10 larger than the peak value at 0.1 GeV. We also find that the width of the peak falls very rapidly with increasing electron energy. At high [q2] we find that the differential cross section falls by approximately three orders of magnitude making experimental observation at this time unlikely. The contributions of the individual form factors are obtained for electron energies of 0.5GeV and 2.0 GeV. It is found that at low [q2] the form factors, FA(q2) and Fv(q2), make contributions of similar size to the differential cross section and might be simultaneously determined , but for the case of FM(q2) we find that the contribution is too small to determine. It is also found that at large [q2] values, the contribution of FM(q2) is substantially enhanced , but that the cross section is probably too small to enable a direct determination of FM(q2).

Proton Form Factor Puzzle and the CEBAF Large Acceptance Spectrometer(CLAS) Two-Photon Exchange Experiment

The electromagnetic form factors are the most fundamental observables that encode information about the internal structure of the nucleon. The electric ($G_{E}$) and the magnetic ($G_{M}$) form factors contain information about the spatial distribution of the charge and magnetization inside the nucleon. A significant discrepancy exists between the Rosenbluth and the polarization transfer measurements of the electromagnetic form factors of the proton. One possible explanation for the discrepancy is the contributions of two-photon exchange (TPE) effects. Theoretical calculations estimating the magnitude of the TPE effect are highly model dependent, and limited experimental evidence for such effects exists. Experimentally, the TPE effect can be measured by comparing the ratio of positron-proton elastic scattering cross section to that of the electron-proton $\large(R = \frac{\sigma (e^{+}p)}{\sigma (e^{-}p)}\large)$. The ratio $R$ was measured over a wide range of kinematics, utilizing a 5.6 GeV primary electron beam produced by the Continuous Electron Beam Accelerator Facility (CEBAF) at Jefferson Lab. This dissertation explored dependence of $R$ on kinematic variables such as squared four-momentum transfer ($Q^{2}$) and the virtual photon polarization parameter ($\varepsilon$). A mixed electron-positron beam was produced from the primary electron beam in experimental Hall B. The mixed beam was scattered from a liquid hydrogen (LH$_{2}$) target. Both the scattered lepton and the recoil proton were detected by the CEBAF Large Acceptance Spectrometer (CLAS). The elastic events were then identified by using elastic scattering kinematics. This work extracted the $Q^{2}$ dependence of $R$ at high $\varepsilon$ ($\varepsilon > $ 0.8) and the $\varepsilon$ dependence of $R$ at $\langle Q^{2} \rangle \approx 0.85$ GeV$^{2}$. In these kinematics, our data confirm the validity of the hadronic calculations of the TPE effect by Blunden, Melnitchouk, and Tjon. This hadronic TPE effect, with additional corrections contributed by higher excitations of the intermediate state nucleon, largely reconciles the Rosenbluth and the polarization transfer measurements of the electromagnetic form factors.