Those who can, teach. 'A teacher affects eternity; she can never tell where her influence stops'

Teachers can have a profound effect on us all, both good and bad. In this paper the effect two individual midwives had on my evolution as a midwife will be examined. They were very different: one was formal and the other informal. The classroom was the setting for one, the clinical area for the other. Each had her own unique style and way of looking at the world. One was very different from the other in manner and in approach. However they each shared a philosophy of women centred, normal birth which they espoused in all aspects of their working lives.

Experimental detection of sudden stiffness change in a structural system employing Laser Doppler Vibrometry

Sudden changes in the stiffness of a structure are often indicators of structural damage. Detection of such sudden stiffness change from the vibrations of structures is important for Structural Health Monitoring (SHM) and damage detection. Non-contact measurement of these vibrations is a quick and efficient way for successful detection of sudden stiffness change of a structure. In this paper, we demonstrate the capability of Laser Doppler Vibrometry to detect sudden stiffness change in a Single Degree Of Freedom (SDOF) oscillator within a laboratory environment. The dynamic response of the SDOF system was measured using a Polytec RSV-150 Remote Sensing Vibrometer. This instrument employs Laser Doppler Vibrometry for measuring dynamic response. Additionally, the vibration response of the SDOF system was measured through a MicroStrain G-Link Wireless Accelerometer mounted on the SDOF system. The stiffness of the SDOF system was experimentally determined through calibrated linear springs. The sudden change of stiffness was simulated by introducing the failure of a spring at a certain instant in time during a given period of forced vibration. The forced vibration on the SDOF system was in the form of a white noise input. The sudden change in stiffness was successfully detected through the measurements using Laser Doppler Vibrometry. This detection from optically obtained data was compared with a detection using data obtained from the wireless accelerometer. The potential of this technique is deemed important for a wide range of applications. The method is observed to be particularly suitable for rapid damage detection and health monitoring of structures under a model-free condition or where information related to the structure is not sufficient.

Inter-ELM evolution of the edge current density profile on the ASDEX upgrade tokamak

The sudden decrease of plasma stored energy and subsequent power deposition on the first wall of a tokamak due to edge localised modes (ELMs) is potentially detrimental to the success of a future fusion reactor. Understanding and control of ELMs is critical for the longevity of these devices and also to maximise their performance. The commonly accepted picture of ELMs posits a critical pressure gradient and current density in the plasma edge, above which coupled magnetohy drodynamic peeling-ballooning modes become unstable. Much analysis has been presented in recent years on the spatial and temporal evolution of the edge pressure gradient. However, the edge current density has typically been overlooked due to the difficulties in measuring this quantity. In this thesis, a novel method of current density recovery is presented, using the equilibrium solver CLISTE to reconstruct a high resolution equilibrium utilising both external magnetic and internal edge kinetic data measured on the ASDEX Upgrade tokamak. The evolution of the edge current density relative to an ELM crash is presented, showing that a resistive delay in the buildup of the current density is unlikely. An uncertainty analysis shows that the edge current density can be determined with an accuracy consistent with that of the kinetic data used. A comparison with neoclassical theory demonstrates excellent agreement be- tween the current density determined by CLISTE and the calculated profiles. Three ELM mitigation regimes are investigated: Type-II ELMs, ELMs sup- pressed by external magnetic perturbations, and Nitrogen seeded ELMs. In the first two cases, the current density is found to decrease as mitigation on- sets, indicating a more ballooning-like plasma behaviour. In the latter case, the flux surface averaged current density can decrease while the local current density increases, providing a mechanism to suppress both the peeling and ballooning modes.

X-ray and optical studies of soft x-ray transients in M31

Soft X-ray transients (SXTs) are a subgroup of low-mass X-ray binaries consisting of a neutron star or a black hole and a companion low-mass star. SXTs exhibit a sudden outburst by increasing the luminosity from ∼ 1033 to ∼ 1036−38ergs1. After spending a few months in outburst, SXTs switch back to quiescence. Optical study of the binary system during the quiescence state of SXTs provides an opportunity to discriminate between BH binaries and neutron star binaries. The first part ot this research is composed of result of 10 years joint project between Hubble space telescope and Chandra, to study SXTs in M31. The other part of this thesis focused on the light curve of bright SXTs in M31. Disc irradiation is thought to be capable of explaining the global behaviour of the light curves of SXTs. Depending on the strength of the central X-ray emission in irradiating the disc, the light curve may exhibit an exponential or a linear decay. The model predicts that in brighter transients a transition from exponential decline to a linear one may be detectable. In this study, having excluded super-soft sources and hard X-ray transients, a sample of bright SXTs in M31 (Lpeak > 1038ergs1) has been studied. The expected change in the shape of the decay function is only observed in two of the light curves from the six light curves in the sample. Also, a systematic correlation between the shape of the light curve and the X-ray luminosity has not been seen.

A novel activation mechanism for Clostridial bacteriophage endolysins

Bacteriophage-encoded endolysins are produced at the end of the phage lytic cycle for the degradation of the host bacterial cell. Endolysins offer the potential as alternatives to antibiotics as biocontrol agents or therapeutics. The lytic mechanisms of three bacteriophage endolysins that target Clostridium species living under different conditions were investigated. For these endolysins a trigger and release mechanism is proposed for their activation. During host lysis, holin lesion formation suddenly permeabilises the membrane which exposes the cytosol-sequestered endolysins to a sudden environmental shock. This shock is suggested to trigger a conformational switch of the endolysins between two distinct dimer states. The switch between dimer states is proposed to activate a novel autocleavage mechanism that cleaves the linker connecting the N-terminal catalytic domain and the C-terminal domain to release the catalytic domain for more efficient digestion of the bacterial cell wall. Crystal structures of cleaved fragments of CD27L and CTP1L were previously obtained. In these structures cleavage occurs at the stem of the linker connected to the C-terminal domain. Despite a sequence identity of only 22% between 81 residues of the C-terminal domains of CD27L and CTP1L, they represent a novel fold that is identified in a number of different lysins. Within the crystal structures the two distinct dimerization modes are represented: the elongated head‐on dimer and the side-by‐side dimer. Introducing mutations that inhibit either of the dimerization states caused a decrease in the efficiency of both the autocleavage mechanism and the lytic activity of the endolysins. The two dimer states were validated for the full-length endolysins in solution by using right angle light scattering, small angle X‐ray scattering and cross-linking experiments. Overall, the data represents a new type of regulation governed by the C-terminal domains that is used to activate these endolysins once they enter the bacterial cell wall.