This document discusses information theory and related concepts such as entropy, Kullback-Leibler divergence, mutual information, independent component analysis, clustering algorithms, change point detection, kernel density estimation, and nonparametric regression. It provides mathematical definitions and formulas for these concepts. Figures are included to illustrate clustering and change point detection methods. The document contains information that could be useful for understanding techniques in machine learning, signal processing, and statistics.
Calculus 10th edition anton solutions manualReece1334
Download at: https://goo.gl/e1svMM
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The work deals finite frequency H∞ control design for continuous time nonlinear systems, we provide sufficient conditions, ensuring that the closed-loop model is stable. Simulations will be gifted to show level of attenuation that a H∞ lower can be by our method obtained developed where further comparison.
International Journal of Engineering Research and Applications (IJERA) is an open access online peer reviewed international journal that publishes research and review articles in the fields of Computer Science, Neural Networks, Electrical Engineering, Software Engineering, Information Technology, Mechanical Engineering, Chemical Engineering, Plastic Engineering, Food Technology, Textile Engineering, Nano Technology & science, Power Electronics, Electronics & Communication Engineering, Computational mathematics, Image processing, Civil Engineering, Structural Engineering, Environmental Engineering, VLSI Testing & Low Power VLSI Design etc.
A copy of my slides from the SILO Seminar at UW Madison on our recent developments for the NEO-K-Means methods including new optimization routines and results.
Response Surface in Tensor Train format for Uncertainty QuantificationAlexander Litvinenko
We apply low-rank Tensor Train format to solve PDEs with uncertain coefficients. First, we approximate uncertain permeability coefficient in TT format, then the operator and then apply iterations to solve stochastic Galerkin system.
Calculus 10th edition anton solutions manualReece1334
Download at: https://goo.gl/e1svMM
People also search:
calculus 10th edition pdf
anton calculus pdf
howard anton calculus 10th edition solution pdf
calculus late transcendentals combined with wiley plus set
calculus multivariable version
calculus by howard anton pdf free download
calculus anton bivens davis 10th edition solutions pdf
calculus anton pdf download
The work deals finite frequency H∞ control design for continuous time nonlinear systems, we provide sufficient conditions, ensuring that the closed-loop model is stable. Simulations will be gifted to show level of attenuation that a H∞ lower can be by our method obtained developed where further comparison.
International Journal of Engineering Research and Applications (IJERA) is an open access online peer reviewed international journal that publishes research and review articles in the fields of Computer Science, Neural Networks, Electrical Engineering, Software Engineering, Information Technology, Mechanical Engineering, Chemical Engineering, Plastic Engineering, Food Technology, Textile Engineering, Nano Technology & science, Power Electronics, Electronics & Communication Engineering, Computational mathematics, Image processing, Civil Engineering, Structural Engineering, Environmental Engineering, VLSI Testing & Low Power VLSI Design etc.
A copy of my slides from the SILO Seminar at UW Madison on our recent developments for the NEO-K-Means methods including new optimization routines and results.
Response Surface in Tensor Train format for Uncertainty QuantificationAlexander Litvinenko
We apply low-rank Tensor Train format to solve PDEs with uncertain coefficients. First, we approximate uncertain permeability coefficient in TT format, then the operator and then apply iterations to solve stochastic Galerkin system.
The SlideShare 101 is a quick start guide if you want to walk through the main features that the platform offers. This will keep getting updated as new features are launched.
The SlideShare 101 replaces the earlier "SlideShare Quick Tour".
Notes for Calculus B (MATH 10360) at the University of Notre Dame. Topics include integration, volume of rotation of a curve, integration by parts, Euler's method, initial value, etc.
01. Differentiation-Theory & solved example Module-3.pdfRajuSingh806014
Total No. of questions in Differentiation are-
In Chapter Examples 31
Solved Examples 32
The rate of change of one quantity with respect to some another quantity has a great importance. For example the rate of change of displacement of a particle with respect to time is called its velocity and the rate of change of velocity is
called its acceleration.
The following results can easily be established using the above definition of the derivative–
d
(i) dx (constant) = 0
The rate of change of a quantity 'y' with respect to another quantity 'x' is called the derivative or differential coefficient of y with respect to x.
Let y = f(x) be a continuous function of a variable quantity x, where x is independent and y is
(ii)
(iii)
(iv)
(v)
d
dx (ax) = a
d (xn) = nxn–1
dx
d ex =ex
dx
d (ax) = ax log a
dependent variable quantity. Let x be an arbitrary small change in the value of x and y be the
dx
d
(vi) dx
e
(logex) = 1/x
corresponding change in y then lim
y
if it exists, d 1
x0 x
is called the derivative or differential coefficient of y with respect to x and it is denoted by
(vii) dx
(logax) =
x log a
dy . y', y
dx 1
or Dy.
d
(viii) dx (sin x) = cos x
So, dy dx
dy
dx
lim
x0
lim
x0
y
x
f (x x) f (x)
x
(ix) (ix)
(x) (x)
d
dx (cos x) = – sin x
d (tan x) = sec2x
dx
The process of finding derivative of a function is called differentiation.
If we again differentiate (dy/dx) with respect to x
(xi)
d (cot x) = – cosec2x
dx
d
then the new derivative so obtained is called second derivative of y with respect to x and it is
Fd2 y
(xii) dx
d
(xiii) dx
(secx)= secx tan x
(cosec x) = – cosec x cot x
denoted by
HGdx2 Jor y" or y2 or D2y. Similarly,
d 1
we can find successive derivatives of y which
(xiv) dx
(sin–1 x) = , –1< x < 1
1 x2
may be denoted by
d –1 1
d3 y d4 y
dn y
(xv) dx (cos x) = –
,–1 < x < 1
dx3 ,
dx4 , ........, dxn , ......
d
(xvi) dx
(tan–1 x) = 1
1 x2
Note : (i)
y is a ratio of two quantities y and
x
(xvii) (xvii)
d (cot–1 x) = – 1
where as dy
dx
dy
is not a ratio, it is a single
dx
d
(xviii) (xviii)
(sec–1 x) =
1 x2
1
|x| > 1
quantity i.e.
dx dy÷ dx
dx x x2 1
(ii)
dy is
dx
d (y) in which d/dx is simply a symbol
dx
(xix)
d (cosec–1 x) = – 1
dx
of operation and not 'd' divided by dx.
d
(xx) dx
(sinh x) = cosh x
d
(xxi) dx
d
(cosh x) = sinh x
Theorem V Derivative of the function of the function. If 'y' is a function of 't' and t' is a function of 'x' then
(xxii) dx
d
(tanh x) = sech2 x
dy =
dx
dy . dt
dt dx
(xxiii) dx
d
(xxiv) dx
d
(coth x) = – cosec h2 x (sech x) = – sech x tanh x
Theorem VI Derivative of parametric equations If x = (t) , y = (t) then
dy dy / dt
=
(xxv) dx
(cosech x) = – cosec hx coth x
dx dx / dt
(xxvi) (xxvi)
(xxvii) (xxvii)
d (sin h–1 x) =
Diseno en ingenieria mecanica de Shigley - 8th ---HDes
descarga el contenido completo de aqui http://paralafakyoumecanismos.blogspot.com.ar/2014/08/libro-para-mecanismos-y-elementos-de.html
Solutions manual for calculus an applied approach brief international metric ...Larson612
Solutions Manual for Calculus An Applied Approach Brief International Metric Edition 10th Edition by Larson IBSN 9781337290579
Full download: https://goo.gl/RtxZKH
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.
DERIVATION OF MODIFIED BERNOULLI EQUATION WITH VISCOUS EFFECTS AND TERMINAL V...Wasswaderrick3
In this book, we use conservation of energy techniques on a fluid element to derive the Modified Bernoulli equation of flow with viscous or friction effects. We derive the general equation of flow/ velocity and then from this we derive the Pouiselle flow equation, the transition flow equation and the turbulent flow equation. In the situations where there are no viscous effects , the equation reduces to the Bernoulli equation. From experimental results, we are able to include other terms in the Bernoulli equation. We also look at cases where pressure gradients exist. We use the Modified Bernoulli equation to derive equations of flow rate for pipes of different cross sectional areas connected together. We also extend our techniques of energy conservation to a sphere falling in a viscous medium under the effect of gravity. We demonstrate Stokes equation of terminal velocity and turbulent flow equation. We look at a way of calculating the time taken for a body to fall in a viscous medium. We also look at the general equation of terminal velocity.
The ability to recreate computational results with minimal effort and actionable metrics provides a solid foundation for scientific research and software development. When people can replicate an analysis at the touch of a button using open-source software, open data, and methods to assess and compare proposals, it significantly eases verification of results, engagement with a diverse range of contributors, and progress. However, we have yet to fully achieve this; there are still many sociotechnical frictions.
Inspired by David Donoho's vision, this talk aims to revisit the three crucial pillars of frictionless reproducibility (data sharing, code sharing, and competitive challenges) with the perspective of deep software variability.
Our observation is that multiple layers — hardware, operating systems, third-party libraries, software versions, input data, compile-time options, and parameters — are subject to variability that exacerbates frictions but is also essential for achieving robust, generalizable results and fostering innovation. I will first review the literature, providing evidence of how the complex variability interactions across these layers affect qualitative and quantitative software properties, thereby complicating the reproduction and replication of scientific studies in various fields.
I will then present some software engineering and AI techniques that can support the strategic exploration of variability spaces. These include the use of abstractions and models (e.g., feature models), sampling strategies (e.g., uniform, random), cost-effective measurements (e.g., incremental build of software configurations), and dimensionality reduction methods (e.g., transfer learning, feature selection, software debloating).
I will finally argue that deep variability is both the problem and solution of frictionless reproducibility, calling the software science community to develop new methods and tools to manage variability and foster reproducibility in software systems.
Exposé invité Journées Nationales du GDR GPL 2024
Nutraceutical market, scope and growth: Herbal drug technologyLokesh Patil
As consumer awareness of health and wellness rises, the nutraceutical market—which includes goods like functional meals, drinks, and dietary supplements that provide health advantages beyond basic nutrition—is growing significantly. As healthcare expenses rise, the population ages, and people want natural and preventative health solutions more and more, this industry is increasing quickly. Further driving market expansion are product formulation innovations and the use of cutting-edge technology for customized nutrition. With its worldwide reach, the nutraceutical industry is expected to keep growing and provide significant chances for research and investment in a number of categories, including vitamins, minerals, probiotics, and herbal supplements.
Comparing Evolved Extractive Text Summary Scores of Bidirectional Encoder Rep...University of Maribor
Slides from:
11th International Conference on Electrical, Electronics and Computer Engineering (IcETRAN), Niš, 3-6 June 2024
Track: Artificial Intelligence
https://www.etran.rs/2024/en/home-english/
(May 29th, 2024) Advancements in Intravital Microscopy- Insights for Preclini...Scintica Instrumentation
Intravital microscopy (IVM) is a powerful tool utilized to study cellular behavior over time and space in vivo. Much of our understanding of cell biology has been accomplished using various in vitro and ex vivo methods; however, these studies do not necessarily reflect the natural dynamics of biological processes. Unlike traditional cell culture or fixed tissue imaging, IVM allows for the ultra-fast high-resolution imaging of cellular processes over time and space and were studied in its natural environment. Real-time visualization of biological processes in the context of an intact organism helps maintain physiological relevance and provide insights into the progression of disease, response to treatments or developmental processes.
In this webinar we give an overview of advanced applications of the IVM system in preclinical research. IVIM technology is a provider of all-in-one intravital microscopy systems and solutions optimized for in vivo imaging of live animal models at sub-micron resolution. The system’s unique features and user-friendly software enables researchers to probe fast dynamic biological processes such as immune cell tracking, cell-cell interaction as well as vascularization and tumor metastasis with exceptional detail. This webinar will also give an overview of IVM being utilized in drug development, offering a view into the intricate interaction between drugs/nanoparticles and tissues in vivo and allows for the evaluation of therapeutic intervention in a variety of tissues and organs. This interdisciplinary collaboration continues to drive the advancements of novel therapeutic strategies.
Toxic effects of heavy metals : Lead and Arsenicsanjana502982
Heavy metals are naturally occuring metallic chemical elements that have relatively high density, and are toxic at even low concentrations. All toxic metals are termed as heavy metals irrespective of their atomic mass and density, eg. arsenic, lead, mercury, cadmium, thallium, chromium, etc.
70. E = {ε1, . . . , εm}, m < n
E ε {(Xε, Yε)}ε∈E
R =
1
m
ε∈E
(Yε − f(z) − CXε)2
(11)
f(z) C
f(z)
ˆfs(z)
50 / 74
71. z ˆfs(z)
leave-one-out
ˆHs(D) = −
1
n
n
i=1
ln ˆfs,i(xi), (12)
ˆfs,i(xi) xi
ˆHs(D) Simple Regression Entropy
Estimator (SRE) [Hino+, 2015]
51 / 74
72. SRE: how it works
−3 −2 −1 0 1 2 3
0.00.10.20.30.4
Normal
x
density
0 1 2 3 40.240.280.320.36
Normal
epsilon^2
f(z)
Fitted density function Fitted intercept ˆfs(z = 0.5)
52 / 74
73. SRE: how it works
−3 −2 −1 0 1 2 3
0.000.100.200.30
Bimodal
x
density
1.0 1.5 2.0 2.5 3.0 3.5 4.00.2250.2350.245
Bimodal
epsilon^2
f(z)
Fitted density function Fitted intercept ˆfs(z = 0.5)
53 / 74
74. ε xi ∈ D
Yε ≃ f(xi) + CXε
Yε = kε
ncpεp C = ptr∇2f(xi)
4(p/2+1) xi
Y i
ε Ci :
Y i
ε ≃ f(xi) + Ci
Xε
54 / 74
75. Y i
ε = f(xi) + CiXε
xi ∈ D
−
1
n
n
i=1
ln Y i
ε = −
1
n
n
i=1
ln f(xi) + Ci
Xε
= −
1
n
n
i=1
ln f(xi) 1 +
CiXε
f(xi)
= −
1
n
n
i=1
ln f(xi) −
1
n
n
i=1
ln 1 +
CiXε
f(xi)
≃ −
1
n
n
i=1
ln f(xi) −
1
n
n
i=1
Ci
f(xi)
Xε
55 / 74
76. −
1
n
n
i=1
ln Y i
ε ≃ −
1
n
n
i=1
ln f(xi) −
1
n
n
i=1
Ci
f(xi)
Xε
¯Yε = − 1
n
n
i=1 ln Y i
ε
H(D) = − 1
n
n
i=1 f(xi)
¯C = − 1
n
n
i=1
Ci
f(xi)
ε > 0
¯Yε = H(D) + ¯CXε (13)
56 / 74
77. ε ∈ E (13)
Rd =
1
m
ε∈E
( ¯Yε − H(D) − ¯CXε)2
Direct Regression Entropy
Estimator (DRE) [Hino+, 2015]
57 / 74
82. kε ≃ cpnf(z)εp
+ cpn
p
4(p/2 + 1)
tr∇2
f(z)εp+2
X = (εp, εp+2) Y = kε
Y = β⊤X
kε Poisson
62 / 74
83. max L(β) =
m
i=1
e−X⊤
i β(X⊤
i β)Yi
Yi!
εp β1
ˆβ1
z ˆβ1/(cpn)
SRE LOO
Entropy Estimator with Poisson-noise structure and
Identity-link regression(EPI) [Hino+,under review]
63 / 74
86. Univariate Case
15 distributions
−3 −2 −1 0 1 2 3
0.00.10.20.30.4
Normal
x
density
−3 −2 −1 0 1 2 3
0.00.10.20.30.40.5
Skewed
x
density
−3 −2 −1 0 1 2 3
0.00.20.40.60.81.01.21.4
Strongly Skewed
x
density
−3 −2 −1 0 1 2 3
0.00.51.01.5
Kurtotic
x
density
−3 −2 −1 0 1 2 3
0.000.050.100.150.200.250.30
Bimodal
x
density
−3 −2 −1 0 1 2 3
0.00.10.20.30.4
Skewed Bimodal
x
density
66 / 74
87. Univariate Case
15 distributions
−3 −2 −1 0 1 2 3
0.000.050.100.150.200.250.30
Trimodal
x
density
−3 −2 −1 0 1 2 3
0.00.10.20.30.40.50.6
10 Claw
x
density
−3 −2 −1 0 1 2 3
0.00.10.20.30.4
Standard Power Exponential
x
density
−3 −2 −1 0 1 2 3
0.050.100.150.200.25
Standard Logistic
x
density
−3 −2 −1 0 1 2 3
0.10.20.30.40.5
Standard Classical Laplace
x
density
−3 −2 −1 0 1 2 3
0.10.20.3
t(df=5)
x
density
67 / 74
88. Univariate Case
15 distributions
−3 −2 −1 0 1 2 3
0.050.100.150.200.25
Mixed t
x
density
−3 −2 −1 0 1 2 3
0.00.20.40.60.81.0
Standard Exponential
x
density
−3 −2 −1 0 1 2 3
0.050.100.150.200.250.30
Cauchy
x
density
68 / 74
89. ●
●●
●
●
●
●
●
●
●
−3 −2 −1 0 1 2 3
0.00.10.20.30.4
Normal
x
density
−3 −2 −1 0 1 2 3
0.00.10.20.30.40.5
Skewed
x
density
−3 −2 −1 0 1 2 3
0.00.20.40.60.81.01.21.4
Strongly Skewed
x
density
−3 −2 −1 0 1 2 3
0.00.51.01.5
Kurtotic
x
density
−3 −2 −1 0 1 2 3
0.000.050.100.150.200.250.30
Bimodal
x
density
69 / 74
90. ●
●
●
●
●
●
●●
●
●
−3 −2 −1 0 1 2 3
0.00.10.20.30.4
Skewed Bimodal
x
density
−3 −2 −1 0 1 2 3
0.000.050.100.150.200.250.30
Trimodal
x
density
−3 −2 −1 0 1 2 3
0.00.10.20.30.40.50.6
10 Claw
x
density
−3 −2 −1 0 1 2 3
0.00.10.20.30.4
Standard Power Exponential
x
density
−3 −2 −1 0 1 2 3
0.050.100.150.200.25
Standard Logistic
x
density
69 / 74
91. ●●
●
●●
●
●
●
●
●
●
−3 −2 −1 0 1 2 3
0.10.20.30.40.5
Standard Classical Laplace
x
density
−3 −2 −1 0 1 2 3
0.10.20.3
t(df=5)
x
density
−3 −2 −1 0 1 2 3
0.050.100.150.200.25
Mixed t
x
density
−3 −2 −1 0 1 2 3
0.00.20.40.60.81.0
Standard Exponential
x
density
−3 −2 −1 0 1 2 3
0.050.100.150.200.250.30
Cauchy
x
density
69 / 74
95. I
[Faivishevsky&Goldberger, 2010] Faivishevsky, L. and Goldberger, J. (2010).
A Nonparametric Information Theoretic Clustering Algorithm.
ICML2010.
[Hino+, 2015] Hino, H., Koshijima, K., and Murata, N. (2015).
Non-parametric entropy estimators based on simple linear regression.
Computational Statistics & Data Analysis, 89(0):72 – 84.
[Hino&Murata, 2010] Hino, H. and Murata, N. (2010).
A conditional entropy minimization criterion for dimensionality reduction and
multiple kernel learning.
Neural Computation, 22(11):2887–2923.
[Hyv¨arinen&Oja, 2000] Hyv¨arinen, A. and Oja, E. (2000).
Independent component analysis: algorithms and applications.
Neural Networks, 13(4-5):411–430.
[Koshijima+, 2015] Koshijima, K., Hino, H., and Murata, N. (2015).
Change-point detection in a sequence of bags-of-data.
Knowledge and Data Engineering, IEEE Transactions on, 27(10):2632–2644.
73 / 74
96. II
[Murata+, 2013] Murata, N., Koshijima, K., and Hino, H. (2013).
Distance-based change-point detection with entropy estimation.
In Proceedings of the Sixth Workshop on Information Theoretic Methods in
Science and Engineering, pages 22–25.
74 / 74