Paul Gooley

Prof. Paul Gooley

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Research Focus & Metrics

Academic Career Length

43Years (1984-Present)

(Calculated once Scilit publication data is synced: current year − year of first publication + 1)

Representative Publications

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1 November 2008 in Chemistry & Biology
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Journal Article
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John ScottJohn Scott
John Scott
BDBryce J.W. van Denderen
Bryce J.W. van Denderen
SJSebastian B. Jorgensen
Sebastian B. Jorgensen
JHJane E. Honeyman
Jane E. Honeyman
GSGregory R. Steinberg
Gregory R. Steinberg
BKBruce E. Kemp
Bruce E. Kemp

8 April 2015 in The Plant Journal
Verified
Journal Article
Closed access
PDF file
SEShane Emanuelle
Shane Emanuelle
MHMohammed Iqbal Hossain
Mohammed Iqbal Hossain
IMIsabel E. Moller
Isabel E. Moller
HPHenriette L. Pedersen
Henriette L. Pedersen
AMAllison M. L. van de Meene
Allison M. L. van de Meene
DSDavid I. Stapleton
David I. Stapleton

18 December 2007 in Journal of Biomolecular NMR
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Journal Article
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EDEdward J. D’auvergne
Edward J. D’auvergne
PGPaul Gooley
Paul Gooley
The key to obtaining the model-free description of the dynamics of a macromolecule is the optimisation of the model-free and Brownian rotational diffusion parameters using the collected R 1, R 2 and steady-state NOE relaxation data. The problem of optimising the chi-squared value is often assumed to be trivial, however, the long chain of dependencies required for its calculation complicates the model-free chi-squared space. Convolutions are induced by the Lorentzian form of the spectral density functions, the linear recombinations of certain spectral density values to obtain the relaxation rates, the calculation of the NOE using the ratio of two of these rates, and finally the quadratic form of the chi-squared equation itself. Two major topological features of the model-free space complicate optimisation. The first is a long, shallow valley which commences at infinite correlation times and gradually approaches the minimum. The most severe convolution occurs for motions on two timescales in which the minimum is often located at the end of a long, deep, curved tunnel or multidimensional valley through the space. A large number of optimisation algorithms will be investigated and their performance compared to determine which techniques are suitable for use in model-free analysis. Local optimisation algorithms will be shown to be sufficient for minimisation not only within the model-free space but also for the minimisation of the Brownian rotational diffusion tensor. In addition the performance of the programs Modelfree and Dasha are investigated. A number of model-free optimisation failures were identified: the inability to slide along the limits, the singular matrix failure of the Levenberg–Marquardt minimisation algorithm, the low precision of both programs, and a bug in Modelfree. Significantly, the singular matrix failure of the Levenberg–Marquardt algorithm occurs when internal correlation times are undefined and is greatly amplified in model-free analysis by both the grid search and constraint algorithms. The program relax (http://www.nmr-relax.com) is also presented as a new software package designed for the analysis of macromolecular dynamics through the use of NMR relaxation data and which alleviates all of the problems inherent within model-free analysis.

1 April 2016 in Trends in Plant Science
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Journal Article
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SEShane Emanuelle
Shane Emanuelle
MDMonika S. Doblin
Monika S. Doblin
DSDavid I. Stapleton
David I. Stapleton
ABAntony Bacic
Antony Bacic
PGPaul Gooley
Paul Gooley

28 January 2011 in The FEBS Journal
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AKAnn H. Kwan
Ann H. Kwan
MMMehdi Mobli
Mehdi Mobli
PGPaul Gooley
Paul Gooley
Glenn KingGlenn King
Glenn King
JMJoel P. Mackay
Joel P. Mackay

18 December 2007 in Journal of Biomolecular NMR
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Journal Article
Open access
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EDEdward J D'Auvergne
Edward J D'Auvergne
PGPaul Gooley
Paul Gooley
Finding the dynamics of an entire macromolecule is a complex problem as the model-free parameter values are intricately linked to the Brownian rotational diffusion of the molecule, mathematically through the autocorrelation function of the motion and statistically through model selection. The solution to this problem was formulated using set theory as an element of the universal set \({\mathfrak{U}}\)—the union of all model-free spaces (d’Auvergne EJ and Gooley PR (2007) Mol BioSyst 3(7), 483–494). The current procedure commonly used to find the universal solution is to initially estimate the diffusion tensor parameters, to optimise the model-free parameters of numerous models, and then to choose the best model via model selection. The global model is then optimised and the procedure repeated until convergence. In this paper a new methodology is presented which takes a different approach to this diffusion seeded model-free paradigm. Rather than starting with the diffusion tensor this iterative protocol begins by optimising the model-free parameters in the absence of any global model parameters, selecting between all the model-free models, and finally optimising the diffusion tensor. The new model-free optimisation protocol will be validated using synthetic data from Schurr JM et al. (1994) J Magn Reson B 105(3), 211–224 and the relaxation data of the bacteriorhodopsin (1–36)BR fragment from Orekhov VY (1999) J Biomol NMR 14(4), 345–356. To demonstrate the importance of this new procedure the NMR relaxation data of the Olfactory Marker Protein (OMP) of Gitti R et al. (2005) Biochem 44(28), 9673–9679 is reanalysed. The result is that the dynamics for certain secondary structural elements is very different from those originally reported.