Chaotic based Pteropus algorithm for solving optimal reactive power problemIJAAS Team
In this work, a Chaotic based Pteropus algorithm (CPA) has been proposed for solving optimal reactive power problem. Pteropus algorithm imitates deeds of the Pteropus. Normally Pteropus while flying it avoid obstacles by using sonar echoes, particularly utilize time delay. To the original Pteropus algorithm chaotic disturbance has been applied and the optimal capability of the algorithm has been improved in search of global solution. In order to augment the population diversity and prevent early convergence, adaptively chaotic disturbance is added at the time of stagnation. Furthermore, exploration and exploitation capability of the proposed algorithm has been improved. Proposed CPA technique has been tested in standard IEEE 14,300 bus systems & real power loss has been considerably reduced.
Investigation of Parameter Behaviors in Stationarity of Autoregressive and Mo...BRNSS Publication Hub
The most important assumption about time series and econometrics data is stationarity. Therefore, this study focuses on behaviors of some parameters in stationarity of autoregressive (AR) and moving average (MA) models. Simulation studies were conducted using R statistical software to investigate the parameter values at different orders (p) of AR and (q) of MA models, and different sample sizes. The stationary status of the p and q are, respectively, determined, parameters such as mean, variance, autocorrelation function (ACF), and partial autocorrelation function (PACF) were determined. The study concluded that the absolute values of ACF and PACF of AR and MA models increase as the parameter values increase but decrease with increase of their orders which as a result, tends to zero at higher lag orders. This is clearly observed in large sample size (n = 300). However, their values decline as sample size increases when compared by orders across the sample sizes. Furthermore, it was observed that the means values of the AR and MA models of first order increased with increased in parameter but decreased when sample sizes were decreased, which tend to zero at large sample sizes, so also the variances
Gaining Confidence in Signalling and Regulatory NetworksMichael Stumpf
Mathematical models of signalling and gene regulatory systems are abstractions of much more complicated processes. Even as more and larger data sets are becoming available we are not be able to dispense entirely with mechanistic models of real-world processes; nor should we. However, trying to develop informative and realistic models of such systems typically involves suitable statistical inference methods, domain expertise and a modicum of luck. Except
for cases where physical principles provide sucient guidance it will also be generally possible to come up with a large number of potential models that are compatible with a given biological system and any finite amount of data generated from experiments on that system.
Here I will discuss how we can systematically evaluate
potentially vast sets of mechanistic candidate models in light
of experimental and prior knowledge about biological systems. This enables us to evaluate quantitatively
the dependence of model inferences and predictions on the assumed model structures. Failure to consider the impact of structural uncertainty introduces biases into the analysis and potentially gives rise to misleading conclusions.
ESTIMATE OF THE HEAD PRODUCED BY ELECTRICAL SUBMERSIBLE PUMPS ON GASEOUS PETR...ijaia
This paper reports successful development of an exact and an efficient radial basis function network (RBFN) model to estimate the head of gaseous petroleum fluids (GPFs) in electrical submersible pumps (ESPs). Head of GPFs in ESPs is now often estimated using empirical models. Overfitting and its consequent lack of model generality data is a potentially serious issue. In addition, available data series is fairly small, including the results of 110 experiments. All these limits were considered in RBFN design process, and highly accurate RBFNs were developed and cross validated.
Chaotic based Pteropus algorithm for solving optimal reactive power problemIJAAS Team
In this work, a Chaotic based Pteropus algorithm (CPA) has been proposed for solving optimal reactive power problem. Pteropus algorithm imitates deeds of the Pteropus. Normally Pteropus while flying it avoid obstacles by using sonar echoes, particularly utilize time delay. To the original Pteropus algorithm chaotic disturbance has been applied and the optimal capability of the algorithm has been improved in search of global solution. In order to augment the population diversity and prevent early convergence, adaptively chaotic disturbance is added at the time of stagnation. Furthermore, exploration and exploitation capability of the proposed algorithm has been improved. Proposed CPA technique has been tested in standard IEEE 14,300 bus systems & real power loss has been considerably reduced.
Investigation of Parameter Behaviors in Stationarity of Autoregressive and Mo...BRNSS Publication Hub
The most important assumption about time series and econometrics data is stationarity. Therefore, this study focuses on behaviors of some parameters in stationarity of autoregressive (AR) and moving average (MA) models. Simulation studies were conducted using R statistical software to investigate the parameter values at different orders (p) of AR and (q) of MA models, and different sample sizes. The stationary status of the p and q are, respectively, determined, parameters such as mean, variance, autocorrelation function (ACF), and partial autocorrelation function (PACF) were determined. The study concluded that the absolute values of ACF and PACF of AR and MA models increase as the parameter values increase but decrease with increase of their orders which as a result, tends to zero at higher lag orders. This is clearly observed in large sample size (n = 300). However, their values decline as sample size increases when compared by orders across the sample sizes. Furthermore, it was observed that the means values of the AR and MA models of first order increased with increased in parameter but decreased when sample sizes were decreased, which tend to zero at large sample sizes, so also the variances
Gaining Confidence in Signalling and Regulatory NetworksMichael Stumpf
Mathematical models of signalling and gene regulatory systems are abstractions of much more complicated processes. Even as more and larger data sets are becoming available we are not be able to dispense entirely with mechanistic models of real-world processes; nor should we. However, trying to develop informative and realistic models of such systems typically involves suitable statistical inference methods, domain expertise and a modicum of luck. Except
for cases where physical principles provide sucient guidance it will also be generally possible to come up with a large number of potential models that are compatible with a given biological system and any finite amount of data generated from experiments on that system.
Here I will discuss how we can systematically evaluate
potentially vast sets of mechanistic candidate models in light
of experimental and prior knowledge about biological systems. This enables us to evaluate quantitatively
the dependence of model inferences and predictions on the assumed model structures. Failure to consider the impact of structural uncertainty introduces biases into the analysis and potentially gives rise to misleading conclusions.
ESTIMATE OF THE HEAD PRODUCED BY ELECTRICAL SUBMERSIBLE PUMPS ON GASEOUS PETR...ijaia
This paper reports successful development of an exact and an efficient radial basis function network (RBFN) model to estimate the head of gaseous petroleum fluids (GPFs) in electrical submersible pumps (ESPs). Head of GPFs in ESPs is now often estimated using empirical models. Overfitting and its consequent lack of model generality data is a potentially serious issue. In addition, available data series is fairly small, including the results of 110 experiments. All these limits were considered in RBFN design process, and highly accurate RBFNs were developed and cross validated.
"Hyperpolarization - Description, Overview, & Methods" ISMRM Annual Meeting, Educational Presentation, April 26, 2017
Basic introduction of Hyperpolarization via DNP, as well as PHIP and optical pumping
Imaging strategies and analysis methods for Hyperpolarized MRI (emphasis on carbon-13 metabolic imaging)
https://youtu.be/NLT8E-CLF6o
UCSF Hyperpolarized MR Seminar
Summer 2019, Lecture #8-2
"Integration into Biomedical Research - Neurological"
Lecturer: Lydia Le Page
Sponsored by the NIH/NIBIB-supported UCSF Hyperpolarized MRI Technology Resource Center (P41EB013598)
https://radiology.ucsf.edu/research/labs/hyperpolarized-mri-tech
UCSF Hyperpolarized MR Seminar
Summer 2019, Lecture #6 part 1
"Hyperpolarized MR in the Heart"
Lecturer: Peder Larson
Sponsored by the NIH/NIBIB-supported UCSF Hyperpolarized MRI Technology Resource Center (P41EB013598)
https://radiology.ucsf.edu/research/labs/hyperpolarized-mri-tech
UCSF Hyperpolarized MR #4: Acquisition and RF Coils (2019)Peder Larson
UCSF Hyperpolarized MR Seminar
Summer 2019, Lecture #4
"Hyperpolarized MR Acquisition and RF Coils"
Lecturer: Jeremy Gordon
Sponsored by the NIH/NIBIB-supported UCSF Hyperpolarized MRI Technology Resource Center (P41EB013598)
https://radiology.ucsf.edu/research/labs/hyperpolarized-mri-tech
UCSF Hyperpolarized MR #2: DNP Physics and Hardware (2019Peder Larson
UCSF Hyperpolarized MR Seminar
Summer 2019, Lecture #2
"DNP Physics and Hardware"
Lecturer: Jeremy Gordon
Sponsored by the NIH/NIBIB-supported UCSF Hyperpolarized MRI Technology Resource Center (P41EB013598)
https://radiology.ucsf.edu/research/labs/hyperpolarized-mri-tech
Richard's entangled aventures in wonderlandRichard Gill
Since the loophole-free Bell experiments of 2020 and the Nobel prizes in physics of 2022, critics of Bell's work have retreated to the fortress of super-determinism. Now, super-determinism is a derogatory word - it just means "determinism". Palmer, Hance and Hossenfelder argue that quantum mechanics and determinism are not incompatible, using a sophisticated mathematical construction based on a subtle thinning of allowed states and measurements in quantum mechanics, such that what is left appears to make Bell's argument fail, without altering the empirical predictions of quantum mechanics. I think however that it is a smoke screen, and the slogan "lost in math" comes to my mind. I will discuss some other recent disproofs of Bell's theorem using the language of causality based on causal graphs. Causal thinking is also central to law and justice. I will mention surprising connections to my work on serial killer nurse cases, in particular the Dutch case of Lucia de Berk and the current UK case of Lucy Letby.
Deep Behavioral Phenotyping in Systems Neuroscience for Functional Atlasing a...Ana Luísa Pinho
Functional Magnetic Resonance Imaging (fMRI) provides means to characterize brain activations in response to behavior. However, cognitive neuroscience has been limited to group-level effects referring to the performance of specific tasks. To obtain the functional profile of elementary cognitive mechanisms, the combination of brain responses to many tasks is required. Yet, to date, both structural atlases and parcellation-based activations do not fully account for cognitive function and still present several limitations. Further, they do not adapt overall to individual characteristics. In this talk, I will give an account of deep-behavioral phenotyping strategies, namely data-driven methods in large task-fMRI datasets, to optimize functional brain-data collection and improve inference of effects-of-interest related to mental processes. Key to this approach is the employment of fast multi-functional paradigms rich on features that can be well parametrized and, consequently, facilitate the creation of psycho-physiological constructs to be modelled with imaging data. Particular emphasis will be given to music stimuli when studying high-order cognitive mechanisms, due to their ecological nature and quality to enable complex behavior compounded by discrete entities. I will also discuss how deep-behavioral phenotyping and individualized models applied to neuroimaging data can better account for the subject-specific organization of domain-general cognitive systems in the human brain. Finally, the accumulation of functional brain signatures brings the possibility to clarify relationships among tasks and create a univocal link between brain systems and mental functions through: (1) the development of ontologies proposing an organization of cognitive processes; and (2) brain-network taxonomies describing functional specialization. To this end, tools to improve commensurability in cognitive science are necessary, such as public repositories, ontology-based platforms and automated meta-analysis tools. I will thus discuss some brain-atlasing resources currently under development, and their applicability in cognitive as well as clinical neuroscience.
Earliest Galaxies in the JADES Origins Field: Luminosity Function and Cosmic ...Sérgio Sacani
We characterize the earliest galaxy population in the JADES Origins Field (JOF), the deepest
imaging field observed with JWST. We make use of the ancillary Hubble optical images (5 filters
spanning 0.4−0.9µm) and novel JWST images with 14 filters spanning 0.8−5µm, including 7 mediumband filters, and reaching total exposure times of up to 46 hours per filter. We combine all our data
at > 2.3µm to construct an ultradeep image, reaching as deep as ≈ 31.4 AB mag in the stack and
30.3-31.0 AB mag (5σ, r = 0.1” circular aperture) in individual filters. We measure photometric
redshifts and use robust selection criteria to identify a sample of eight galaxy candidates at redshifts
z = 11.5 − 15. These objects show compact half-light radii of R1/2 ∼ 50 − 200pc, stellar masses of
M⋆ ∼ 107−108M⊙, and star-formation rates of SFR ∼ 0.1−1 M⊙ yr−1
. Our search finds no candidates
at 15 < z < 20, placing upper limits at these redshifts. We develop a forward modeling approach to
infer the properties of the evolving luminosity function without binning in redshift or luminosity that
marginalizes over the photometric redshift uncertainty of our candidate galaxies and incorporates the
impact of non-detections. We find a z = 12 luminosity function in good agreement with prior results,
and that the luminosity function normalization and UV luminosity density decline by a factor of ∼ 2.5
from z = 12 to z = 14. We discuss the possible implications of our results in the context of theoretical
models for evolution of the dark matter halo mass function.
Richard's aventures in two entangled wonderlandsRichard Gill
Since the loophole-free Bell experiments of 2020 and the Nobel prizes in physics of 2022, critics of Bell's work have retreated to the fortress of super-determinism. Now, super-determinism is a derogatory word - it just means "determinism". Palmer, Hance and Hossenfelder argue that quantum mechanics and determinism are not incompatible, using a sophisticated mathematical construction based on a subtle thinning of allowed states and measurements in quantum mechanics, such that what is left appears to make Bell's argument fail, without altering the empirical predictions of quantum mechanics. I think however that it is a smoke screen, and the slogan "lost in math" comes to my mind. I will discuss some other recent disproofs of Bell's theorem using the language of causality based on causal graphs. Causal thinking is also central to law and justice. I will mention surprising connections to my work on serial killer nurse cases, in particular the Dutch case of Lucia de Berk and the current UK case of Lucy Letby.
Multi-source connectivity as the driver of solar wind variability in the heli...Sérgio Sacani
The ambient solar wind that flls the heliosphere originates from multiple
sources in the solar corona and is highly structured. It is often described
as high-speed, relatively homogeneous, plasma streams from coronal
holes and slow-speed, highly variable, streams whose source regions are
under debate. A key goal of ESA/NASA’s Solar Orbiter mission is to identify
solar wind sources and understand what drives the complexity seen in the
heliosphere. By combining magnetic feld modelling and spectroscopic
techniques with high-resolution observations and measurements, we show
that the solar wind variability detected in situ by Solar Orbiter in March
2022 is driven by spatio-temporal changes in the magnetic connectivity to
multiple sources in the solar atmosphere. The magnetic feld footpoints
connected to the spacecraft moved from the boundaries of a coronal hole
to one active region (12961) and then across to another region (12957). This
is refected in the in situ measurements, which show the transition from fast
to highly Alfvénic then to slow solar wind that is disrupted by the arrival of
a coronal mass ejection. Our results describe solar wind variability at 0.5 au
but are applicable to near-Earth observatories.
Slide 1: Title Slide
Extrachromosomal Inheritance
Slide 2: Introduction to Extrachromosomal Inheritance
Definition: Extrachromosomal inheritance refers to the transmission of genetic material that is not found within the nucleus.
Key Components: Involves genes located in mitochondria, chloroplasts, and plasmids.
Slide 3: Mitochondrial Inheritance
Mitochondria: Organelles responsible for energy production.
Mitochondrial DNA (mtDNA): Circular DNA molecule found in mitochondria.
Inheritance Pattern: Maternally inherited, meaning it is passed from mothers to all their offspring.
Diseases: Examples include Leber’s hereditary optic neuropathy (LHON) and mitochondrial myopathy.
Slide 4: Chloroplast Inheritance
Chloroplasts: Organelles responsible for photosynthesis in plants.
Chloroplast DNA (cpDNA): Circular DNA molecule found in chloroplasts.
Inheritance Pattern: Often maternally inherited in most plants, but can vary in some species.
Examples: Variegation in plants, where leaf color patterns are determined by chloroplast DNA.
Slide 5: Plasmid Inheritance
Plasmids: Small, circular DNA molecules found in bacteria and some eukaryotes.
Features: Can carry antibiotic resistance genes and can be transferred between cells through processes like conjugation.
Significance: Important in biotechnology for gene cloning and genetic engineering.
Slide 6: Mechanisms of Extrachromosomal Inheritance
Non-Mendelian Patterns: Do not follow Mendel’s laws of inheritance.
Cytoplasmic Segregation: During cell division, organelles like mitochondria and chloroplasts are randomly distributed to daughter cells.
Heteroplasmy: Presence of more than one type of organellar genome within a cell, leading to variation in expression.
Slide 7: Examples of Extrachromosomal Inheritance
Four O’clock Plant (Mirabilis jalapa): Shows variegated leaves due to different cpDNA in leaf cells.
Petite Mutants in Yeast: Result from mutations in mitochondrial DNA affecting respiration.
Slide 8: Importance of Extrachromosomal Inheritance
Evolution: Provides insight into the evolution of eukaryotic cells.
Medicine: Understanding mitochondrial inheritance helps in diagnosing and treating mitochondrial diseases.
Agriculture: Chloroplast inheritance can be used in plant breeding and genetic modification.
Slide 9: Recent Research and Advances
Gene Editing: Techniques like CRISPR-Cas9 are being used to edit mitochondrial and chloroplast DNA.
Therapies: Development of mitochondrial replacement therapy (MRT) for preventing mitochondrial diseases.
Slide 10: Conclusion
Summary: Extrachromosomal inheritance involves the transmission of genetic material outside the nucleus and plays a crucial role in genetics, medicine, and biotechnology.
Future Directions: Continued research and technological advancements hold promise for new treatments and applications.
Slide 11: Questions and Discussion
Invite Audience: Open the floor for any questions or further discussion on the topic.
Professional air quality monitoring systems provide immediate, on-site data for analysis, compliance, and decision-making.
Monitor common gases, weather parameters, particulates.
THE IMPORTANCE OF MARTIAN ATMOSPHERE SAMPLE RETURN.Sérgio Sacani
The return of a sample of near-surface atmosphere from Mars would facilitate answers to several first-order science questions surrounding the formation and evolution of the planet. One of the important aspects of terrestrial planet formation in general is the role that primary atmospheres played in influencing the chemistry and structure of the planets and their antecedents. Studies of the martian atmosphere can be used to investigate the role of a primary atmosphere in its history. Atmosphere samples would also inform our understanding of the near-surface chemistry of the planet, and ultimately the prospects for life. High-precision isotopic analyses of constituent gases are needed to address these questions, requiring that the analyses are made on returned samples rather than in situ.
Observation of Io’s Resurfacing via Plume Deposition Using Ground-based Adapt...Sérgio Sacani
Since volcanic activity was first discovered on Io from Voyager images in 1979, changes
on Io’s surface have been monitored from both spacecraft and ground-based telescopes.
Here, we present the highest spatial resolution images of Io ever obtained from a groundbased telescope. These images, acquired by the SHARK-VIS instrument on the Large
Binocular Telescope, show evidence of a major resurfacing event on Io’s trailing hemisphere. When compared to the most recent spacecraft images, the SHARK-VIS images
show that a plume deposit from a powerful eruption at Pillan Patera has covered part
of the long-lived Pele plume deposit. Although this type of resurfacing event may be common on Io, few have been detected due to the rarity of spacecraft visits and the previously low spatial resolution available from Earth-based telescopes. The SHARK-VIS instrument ushers in a new era of high resolution imaging of Io’s surface using adaptive
optics at visible wavelengths.
Introduction:
RNA interference (RNAi) or Post-Transcriptional Gene Silencing (PTGS) is an important biological process for modulating eukaryotic gene expression.
It is highly conserved process of posttranscriptional gene silencing by which double stranded RNA (dsRNA) causes sequence-specific degradation of mRNA sequences.
dsRNA-induced gene silencing (RNAi) is reported in a wide range of eukaryotes ranging from worms, insects, mammals and plants.
This process mediates resistance to both endogenous parasitic and exogenous pathogenic nucleic acids, and regulates the expression of protein-coding genes.
What are small ncRNAs?
micro RNA (miRNA)
short interfering RNA (siRNA)
Properties of small non-coding RNA:
Involved in silencing mRNA transcripts.
Called “small” because they are usually only about 21-24 nucleotides long.
Synthesized by first cutting up longer precursor sequences (like the 61nt one that Lee discovered).
Silence an mRNA by base pairing with some sequence on the mRNA.
Discovery of siRNA?
The first small RNA:
In 1993 Rosalind Lee (Victor Ambros lab) was studying a non- coding gene in C. elegans, lin-4, that was involved in silencing of another gene, lin-14, at the appropriate time in the
development of the worm C. elegans.
Two small transcripts of lin-4 (22nt and 61nt) were found to be complementary to a sequence in the 3' UTR of lin-14.
Because lin-4 encoded no protein, she deduced that it must be these transcripts that are causing the silencing by RNA-RNA interactions.
Types of RNAi ( non coding RNA)
MiRNA
Length (23-25 nt)
Trans acting
Binds with target MRNA in mismatch
Translation inhibition
Si RNA
Length 21 nt.
Cis acting
Bind with target Mrna in perfect complementary sequence
Piwi-RNA
Length ; 25 to 36 nt.
Expressed in Germ Cells
Regulates trnasposomes activity
MECHANISM OF RNAI:
First the double-stranded RNA teams up with a protein complex named Dicer, which cuts the long RNA into short pieces.
Then another protein complex called RISC (RNA-induced silencing complex) discards one of the two RNA strands.
The RISC-docked, single-stranded RNA then pairs with the homologous mRNA and destroys it.
THE RISC COMPLEX:
RISC is large(>500kD) RNA multi- protein Binding complex which triggers MRNA degradation in response to MRNA
Unwinding of double stranded Si RNA by ATP independent Helicase
Active component of RISC is Ago proteins( ENDONUCLEASE) which cleave target MRNA.
DICER: endonuclease (RNase Family III)
Argonaute: Central Component of the RNA-Induced Silencing Complex (RISC)
One strand of the dsRNA produced by Dicer is retained in the RISC complex in association with Argonaute
ARGONAUTE PROTEIN :
1.PAZ(PIWI/Argonaute/ Zwille)- Recognition of target MRNA
2.PIWI (p-element induced wimpy Testis)- breaks Phosphodiester bond of mRNA.)RNAse H activity.
MiRNA:
The Double-stranded RNAs are naturally produced in eukaryotic cells during development, and they have a key role in regulating gene expression .
Astronomy Update- Curiosity’s exploration of Mars _ Local Briefs _ leadertele...
UCSF Hyperpolarized MR #7-1: Analysis (2019)
1. Analysis of Hyperpolarized 13C MRI
BioE 297: Hyperpolarized MR Seminar
August 16, 2019
Peder Larson, Ph.D.
Associate Professor, Department of Radiology and Biomedical Imaging, University
of California, San Francisco, CA, United States
peder.larson@ucsf.edu
https://radiology.ucsf.edu/research/labs/larson
@pezlarson
2. What do we do with HP 13C MR data?
Parametrizations: Kinetic Modeling vs. alternatives (e.g. Area-under-curve)
Choice of model
Fitting algorithms
Considerations
• Robustness of fitting
• Assumptions
• Limitations
August 16, 20192
Pyr Lac
T1 T1
kPLkTRANS
Imaging Voxel
AIF(t)
Pyr
Vessels
3. Parametrizations: Kinetic Modeling vs. alternatives
Numerous options
Kinetic modeling (e.g. kPL)
Unidirectional vs bidirectional
Fixed vs free parameters
Lactate/pyruvate
Area-under-curve (AUCratio, Hill, et
al. PLoS One (2013).)
Time-to-peak
…
August 16, 2019
Daniels et al, NMR Biomed 2016, doi: 10.1002/nbm.3468
3
4. L/P ratio (single time-point)
AUC L/P ratio (dynamics)
Kinetic modeling
• Assumptions
• Input functions
• Perfused voxel model
August 16, 20194
5. Ratiometric methods: Lactate/pyruvate (single time-
point)
Simple approach – acquire single time-point lactate and pyruvate data, then
measure ratio
Major limitation – variability with experiment timing (injection start, duration,
acquisition start time)
August 16, 20195
6. Area-under-curve methods
Ratio of areas under curve (AUC) proportional to
kPL:
• Derived with Laplace transforms
• Assumes entire dynamics are captured and
constant-in-time flip angles
• No assumption on shape of input function (Pin)
• Assuming negligible “back-reaction”, kLP, and
consistent lactate relaxation rates, then
AUCratio is directly proportional to kPL
Hill, et al. PLoS One 8, 9 (2013), e71996.
August 16, 20196
7. AUCratio applicability
Works best with
• Acquire data before injection OR
consistent bolus and acquisition
timing
• Constant-in-time flip angles
Breaks down when
• Variations in lactate T1
• Acquisition starts when there is
already magnetization
• Variable flip angles and variations in
bolus timing and shape
August 16, 20197
AUCratio simulation with
metabolite-specific
(θpyruvate < θlactate),
constant-in-time flip angles
8. Is T1 consistent for HP agents?
Largely
uninvestigated in vivo
Extrapolated results
from in vitro (yeast)
show significantly
shorter intracellular
T1s for carboxylic
acids
August 16, 20198
Carboxylic acid T1,int T1,AC Relative T1,AC Predicted T1,int
Butyric acid 8.1±0.6 8.5 0.85 7.7
Keto‐isocaproic
acid
10.4 11 1.1 9.9
Acetic acid 9.0±1.0 10 1.0 9.0
Pyruvic acid 12.7 15 1.5 13.5
Lactic acid NA 5 0.5 4.5
9. Simulation Framework for
Evaluation of Analysis Methods
Generate simulated data based on model
with typical parameter ranges and
experimental parameters (flip angles, TR,
start/end times)
Measure AUCratio on ideal, noiseless data
Repeat simulation with varying random
noise, and measure AUCratio to analyze
expected parameter accuracy
Repeat simulation for various parameter
ranges to analyze sensitivity to
experimental and physiologic variations
August 16, 20199
Larson et al. NMR in Biomed 2018. DOI: 10.1002/nbm.3997
10. Simulation Evaluation
of AUCratio
Constant 10º flip angle, 8x
phase encodes, TR = 5 s
Most significant bias due to
R1L = 1/T1,lactate
Small bias due to missing
start of acquisition
August 16, 2019
RelativeParameterAccuracy
Tarrive
Tbolus
Using gamma-
variate function
for input function,
u(t)
10
11. Simulation Evaluation
of AUCratio
Metabolite-specific
10º(pyr)/20º(lac) flip angles,
8x phase encodes, TR = 5 s
Bias due to R1L substantially
reduced
Accuracy (dashed lines)
similar otherwise
(Metabolite-specific flip angle
not helping!)
August 16, 2019
RelativeParameterAccuracy
11
12. Simulation Evaluation
of AUCratio
Metabolite-specific variable flip
angles, 8x phase encodes, TR = 2 s
Accuracy (dashed lines) improved,
BUT
Large bias with differences in input
function differences and relaxation
rates
August 16, 2019
RelativeParameterAccuracy
Tarrive
Tbolus
12
13. 2D Dynamic Analysis
From Phase I clinical trial
3 good patient datasets
• Patient 1 – 10º flip
• Others –
10º(pyr)/20º(lac)
August 16, 201913
kPLAUCratio
Patient 1 Patient 3 Patient 4
Polarization Dissolution,
QC, and
delivery
Injection
Duration
Voxel
Size
Prostate Vasculature
max
Pyr
SNR
max
Pyr
time
max
Lac
SNR
max
Lac
time
max
Pyr
SNR
max
Pyr
time
max
Lac
SNR
max
Lac
time
Patient 1* 19.6% 50 s 14 s 3.5 cc 36.0 25 s 7.0 30 s 63.1 25 s 5.7 40 s
Patient 3# 18.7% 47 s 16 s 2 cc 134.9 15 s 16.7 25 s 339.9 15 s 13.6 20 s
Patient 4# 18.7% 64 s 15 s 1.2 cc 24.9 15 s 8.6 25 s 31.0 15 s 7.9 20 s
0.029 0.045 0.045
14. 3D Dynamic Prostate Cancer Analysis
Multiband, variable flip angle
strategy
AUCratio inconsistent compared
to kPL model
Bottom plots show this is due to
bolus delivery variations under
variable flip angle acquisitions
August 16, 201914
15. AUCratio Summary
Best when capturing entire dynamic curves
Major assumption – lactate T1 is consistent
Usable with variable flip angle strategies provided there is reproducible bolus
delivery
Probably easier to use in preclinical studies, where there is less difference in
bolus characteristics due to rapid circulation times, and more physiologic
consistency in animal models compared to human studies
Similarly, single time-point lactate:pyruvate ratio is fine if there is consistency in
the experiment timing (bolus delivery, vascular delivery, and acquisition time)
Can create simulation-based calibration curves to convert to kPL
August 16, 201915
16. Kinetic modeling
Kinetics assumed to fit to a model, which
can be expressed by a set of differential
equations:
Fit data to model, with inclusion of solution
for differential equations
Simple two-site model shown here
August 16, 2019
Pyr Lac
T1 T1
kPL
Imaging Voxel
u(t)
16
17. Additional considerations: RF Flip Angle compensation
Solution: Hybrid continuous-discrete model
• Continuous evolution of z-magnetization
between RF pulses
• Discrete change in magnetization with RF
pulses
August 16, 2019
Bahrami et al. Quant Imaging Med Surg 2014. Maidens et al. IEEE-TMI 2016.
17
Continuous
Model
Discrete
Model
18. Example: Box-car input, two-site
kinetic model
u(t) = “box-car” shape, i.e. constant for
a limited period of time
Solve differential equations:
Challenge: must fit or estimate
multiple parameters of input (rateinj,
tarrival, tend)
Typical Assumptions: neglect back-
reaction, kLP = 0. Often fix T1 values
Can be adapted for other input
shapes, such as gamma-variate
Zierhut et al, JMR 2010.
August 16, 201918
Pyr Lac
T1 T1
kPL
Imaging Voxel
u(t)
19. Example: Fitted input, two-site
kinetic model
u(t) = Input, estimated from vascular
voxels in slice
Estimate perfusion of pyruvate and
kPL
Typical Assumptions: neglect back-
reaction, kLP = 0. Often fix T1 values
Maidens, Gordon, Arcak, Larson. IEEE-TMI 2016 DOI: 10.1109/TMI.2016.2574240 August 16, 201919
Pyr Lac
T1 T1
kPL
Imaging Voxel
u(t)
20. Fitting Methods: Mechanics of model fitting
Approach: code up model and a minimization/optimization routine in your
favorite programming language
• MATLAB: lsqnonlin(), fmincon() …
Test!
Constrained fitting: add upper and lower bounds based on prior
results/expectations (e.g. T1,invivo < T1,solution limits on bolus duration)
Our models typically create non-convex problems, which means the result can
depend a lot on initial guesses
• Potential solution: generate estimates from a simplified model, or based on
some other measurement source (e.g. linear fit to later data for T1 guess,
AUCratio for kPL guess, adjacent voxels fit values)
August 16, 201920
21. Robust Fitting
Idea: separate out more complex models into sub-models
Potentially easier to solve, less confusion and local minima than trying to fit
whole model
August 16, 201921
Perfusion
sub-model
Conversion
sub-model
Maidens, Gordon, Arcak, Larson. IEEE-TMI 2016 DOI: 10.1109/TMI.2016.2574240
22. “Input-less” Fitting as a Robust Model
Actual pyruvate signal as input, change in lactate
as output
No assumptions or fitting of pyruvate signal or
input function u(t)
Pros: Reduced number of parameters to fit,
insensitive to fitting errors in pyruvate (e.g.
incorrect bolus shape), works with any sampling
strategy
Cons: No estimate of perfusion, using input
shape could help constrain fit results, errors in
pyruvate can propogate noise
August 16, 2019
Inpsired by: Khegai, et al. NMR Biomed 2014, Bahrami, et al. Quant Imaging Med Surg 2014.
22
Only fit change in Lactate:
MZ,L[n]
MZ,L[n+1]
23. Simulation: Constant flip angles
Bolus characteristics and T1 values
are fixed to nominal values (center
values in these plots)
Input-less fitting slightly better than
AUCratio
Changes in input (Tarrival, Tbolus)
cause major problems for Fitting with
Input
August 16, 201923
24. Simulation: Metabolite-specific
flip angles
Bolus characteristics and T1 values
are fixed to nominal values (center
values in these plots)
Input-less fitting slightly better than
AUCratio
Changes in input (Tarrival, Tbolus)
cause major problems for Fitting with
Input
Slight performance improvement
over constant flip angles, except for
B1 errors (larger flips used here)
August 16, 201924
25. Simulation: Metabolite-
specific, variable flip angles
Bolus characteristics and T1 values
are fixed to nominal values (center
values in these plots)
Changes in input (Tarrival, Tbolus)
cause major problems for Fitting with
Input and AUCratio
AUCratio performance improved if
bolus is known
Input-less now the most robust,
except to B1 errors
Overall slight performance
improvement over other flip angle
schedules August 16, 201925
26. Simulation: Fitting bolus
characteristics
T1 values are fixed to nominal
values
Allow for fitting on bolus
characteristics (Tarrival, Tbolus)
Improves robustness of Fitting with
Input at expense of slightly
decreased accuracy
August 16, 201926
28. Assuming unidirectional conversion
Bidirectional model is very
poorly conditioned (Swisher et
al. MRM 2014.)
• Hard to separate decay and
metabolic conversion
Lac-to-pyr in HP experiment
measured to be typically order
of magnitude of more less than
pyr-to-lac
August 16, 2019
Pyruvate Lactate
KPyrLac
T1,Pyr T1,Lac
kLacPyr
28
29. Alternative Tissue Models
Problem: Potentially large fraction of pyruvate signal comes from
vascular and/or extracellular compartments, which are a potential
confounder for metabolism conversion
Alternative models
a. Two-site kinetic model with input
b. “Perfused model” – separate extravascular and intravascular
compartments
c. Full model – separate Extravascular/extracellular,
intracellular, and intravascular compartments
Key for evaluation: Adding more model parameters will always fit
data better, so use Akaike Information Criteria (AIC) which
balances fit quality with number of model parameters
Assumptions
• Neglect kLP, lactate transport
• Vascular input function (VIF) estimated from heart voxels
• Fixed T1P = 45s, T1L = 25s
Bankson et al. Cancer Research 2016. doi: 10.1158/0008-5472.CAN-15-0171 August 16, 201929
Models b and c are comparable by AIC
(lower AIC is better)
30. Additional Considerations
Multiple conversion pathways (e.g. alanine, bicarbonate from pyruvate)
• AUCratio still applies (assuming uni-directional conversion)
• Kinetic modeling easily adapted
Fitting Constraints
• Spatial constraints similar to compressed sensing also possible
Magnitude vs complex data
• Noise statistics changed by magnitude operation
• Should use appropriate maximum likelihood estimator – example in fit_kPL()
August 16, 201930
31. Hyperpolarized-MRI-Toolbox
https://github.com/LarsonLab/hyperpolarized-mri-toolbox
Kinetic Modeling
• fit_pyr_kinetics() –input-less model, for pyruvate to lactate
(optionally bicarbonate and alanine)
• fit_kPL() – old version of input-less model
• fit_kPL_withinput – box-car input, two-site model
• fit_kPL_withgammainput – gamma-variate shape input, two-site
model
• ompute_* - AUCratio, time-to-peak, mean-time metrics
• test_fit_* functions for examples
Feeling adventurous?
• Perfused model now in “perfused_model” branch
• Make sure to ‘git pull’ regularly as this is a work in progress
August 16, 201932
33. Recommendations
Input-less kPL is just as robust as AUC ratios, and provides results in units of
[1/s] that can then be compared more generally
Ratiometric methods require reproducible Experimental setup (good flip angle
calibration, consistent injection, consistent cardiovascular physiology)
Perfused voxel model is promising as a more accurate model, but does require
additional estimates or measurements of vascular input function
Metabolite-specific and Variable flip angles may improve SNR and expected
accuracy, but can also create additional instability in model
August 16, 201934
Editor's Notes
Fitting algorithms
with variable flip
No assumptions or fitting on pyruvate input shape
Any RF shape
kPL Maps
Concentration normalized?
Masking based on where data is fit