The document discusses velocity and acceleration in terms of position (x). It defines acceleration as the derivative of velocity with respect to time and velocity as the derivative of position with respect to time. It then provides proofs of these relationships by taking derivatives. The document also includes an example problem that demonstrates finding the velocity of a particle moving in a straight line given its position function. It provides another example of finding the position of a particle over time given its initial position and velocity and its acceleration as a function of position.
Analytic Solutions of an Iterative Functional Differential Equation with Dela...inventionjournals
ABSTRACT : This This paper is concerned with an iterative functional differential equation with the form
z C
x z
b
x az
x z
,
)
( )
(
1
( ) .By constructing a convergent power series solution of an auxiliary equation
b [ag(z) g( z)] [g( z) ag( z)][ g( z) ag(z)] g(z), zC 2 2 2
the analytic solutions for the original equation are obtained. We not only discuss the constant given in Schröder
transformation at resonance( i.e., at a root of the unity), but also discuss those near resonance (i.e., near a
root of the unity) under Brjuno condition.
It is a brief presentation on quantum computation, which is created as I have investigation on guided study with my instructor Professor Sen Yang at CUHK
Research Inventy : International Journal of Engineering and Scienceresearchinventy
Research Inventy : International Journal of Engineering and Science is published by the group of young academic and industrial researchers with 12 Issues per year. It is an online as well as print version open access journal that provides rapid publication (monthly) of articles in all areas of the subject such as: civil, mechanical, chemical, electronic and computer engineering as well as production and information technology. The Journal welcomes the submission of manuscripts that meet the general criteria of significance and scientific excellence. Papers will be published by rapid process within 20 days after acceptance and peer review process takes only 7 days. All articles published in Research Inventy will be peer-reviewed.
In this paper, we consider the scaling invariant spaces for fractional Navier-Stokes in the
Lebesgue spaces ( ) p n L R and homogeneous Besov spaces
, ( ) s n
p q B R respectively.
Analytic Solutions of an Iterative Functional Differential Equation with Dela...inventionjournals
ABSTRACT : This This paper is concerned with an iterative functional differential equation with the form
z C
x z
b
x az
x z
,
)
( )
(
1
( ) .By constructing a convergent power series solution of an auxiliary equation
b [ag(z) g( z)] [g( z) ag( z)][ g( z) ag(z)] g(z), zC 2 2 2
the analytic solutions for the original equation are obtained. We not only discuss the constant given in Schröder
transformation at resonance( i.e., at a root of the unity), but also discuss those near resonance (i.e., near a
root of the unity) under Brjuno condition.
It is a brief presentation on quantum computation, which is created as I have investigation on guided study with my instructor Professor Sen Yang at CUHK
Research Inventy : International Journal of Engineering and Scienceresearchinventy
Research Inventy : International Journal of Engineering and Science is published by the group of young academic and industrial researchers with 12 Issues per year. It is an online as well as print version open access journal that provides rapid publication (monthly) of articles in all areas of the subject such as: civil, mechanical, chemical, electronic and computer engineering as well as production and information technology. The Journal welcomes the submission of manuscripts that meet the general criteria of significance and scientific excellence. Papers will be published by rapid process within 20 days after acceptance and peer review process takes only 7 days. All articles published in Research Inventy will be peer-reviewed.
In this paper, we consider the scaling invariant spaces for fractional Navier-Stokes in the
Lebesgue spaces ( ) p n L R and homogeneous Besov spaces
, ( ) s n
p q B R respectively.
Unconventional phase transitions in frustrated systems (March, 2014)Shu Tanaka
Presentation file using the workshop which was held at the University of Tokyo (March 26, 2014). The presentation was based on two papers:
- Physical Review B Vol. 87, 214401 (2013)
http://journals.aps.org/prb/abstract/10.1103/PhysRevB.87.214401
(preprint: http://arxiv.org/abs/1209.2520)
(A brief explanation: http://www.slideshare.net/shu-t/prb-87214401slideshare)
- Physical Review E Vol. 88, 052138 (2013)
http://journals.aps.org/pre/abstract/10.1103/PhysRevE.88.052138
(preprint: http://arxiv.org/abs/1308.2467)
(A brief explanation: http://www.slideshare.net/shu-t/interlayerinteraction-dependence-of-latent-heat-in-the-heisenberg-model-on-a-stacked-triangular-lattice-with-competing-interactions)
2014年3月26日に東京大学で開催された「統計物理学の新しい潮流」での講演スライドです。この講演は、以下の2つの論文に関係するものです。
- Physical Review B Vol. 87, 214401 (2013)
http://journals.aps.org/prb/abstract/10.1103/PhysRevB.87.214401
(preprint: http://arxiv.org/abs/1209.2520)
(A brief explanation: http://www.slideshare.net/shu-t/prb-87214401slideshare)
- Physical Review E Vol. 88, 052138 (2013)
http://journals.aps.org/pre/abstract/10.1103/PhysRevE.88.052138
(preprint: http://arxiv.org/abs/1308.2467)
(A brief explanation: http://www.slideshare.net/shu-t/interlayerinteraction-dependence-of-latent-heat-in-the-heisenberg-model-on-a-stacked-triangular-lattice-with-competing-interactions)
International Journal of Mathematics and Statistics Invention (IJMSI) is an international journal intended for professionals and researchers in all fields of computer science and electronics. IJMSI publishes research articles and reviews within the whole field Mathematics and Statistics, new teaching methods, assessment, validation and the impact of new technologies and it will continue to provide information on the latest trends and developments in this ever-expanding subject. The publications of papers are selected through double peer reviewed to ensure originality, relevance, and readability. The articles published in our journal can be accessed online.
Unconventional phase transitions in frustrated systems (March, 2014)Shu Tanaka
Presentation file using the workshop which was held at the University of Tokyo (March 26, 2014). The presentation was based on two papers:
- Physical Review B Vol. 87, 214401 (2013)
http://journals.aps.org/prb/abstract/10.1103/PhysRevB.87.214401
(preprint: http://arxiv.org/abs/1209.2520)
(A brief explanation: http://www.slideshare.net/shu-t/prb-87214401slideshare)
- Physical Review E Vol. 88, 052138 (2013)
http://journals.aps.org/pre/abstract/10.1103/PhysRevE.88.052138
(preprint: http://arxiv.org/abs/1308.2467)
(A brief explanation: http://www.slideshare.net/shu-t/interlayerinteraction-dependence-of-latent-heat-in-the-heisenberg-model-on-a-stacked-triangular-lattice-with-competing-interactions)
2014年3月26日に東京大学で開催された「統計物理学の新しい潮流」での講演スライドです。この講演は、以下の2つの論文に関係するものです。
- Physical Review B Vol. 87, 214401 (2013)
http://journals.aps.org/prb/abstract/10.1103/PhysRevB.87.214401
(preprint: http://arxiv.org/abs/1209.2520)
(A brief explanation: http://www.slideshare.net/shu-t/prb-87214401slideshare)
- Physical Review E Vol. 88, 052138 (2013)
http://journals.aps.org/pre/abstract/10.1103/PhysRevE.88.052138
(preprint: http://arxiv.org/abs/1308.2467)
(A brief explanation: http://www.slideshare.net/shu-t/interlayerinteraction-dependence-of-latent-heat-in-the-heisenberg-model-on-a-stacked-triangular-lattice-with-competing-interactions)
International Journal of Mathematics and Statistics Invention (IJMSI) is an international journal intended for professionals and researchers in all fields of computer science and electronics. IJMSI publishes research articles and reviews within the whole field Mathematics and Statistics, new teaching methods, assessment, validation and the impact of new technologies and it will continue to provide information on the latest trends and developments in this ever-expanding subject. The publications of papers are selected through double peer reviewed to ensure originality, relevance, and readability. The articles published in our journal can be accessed online.
Second-order Cosmological Perturbations Engendered by Point-like MassesMaxim Eingorn
R. Brilenkov and M. Eingorn, Second-order cosmological perturbations engendered by point-like masses, ApJ 845 (2017) 153: http://iopscience.iop.org/article/10.3847/1538-4357/aa81cd
In the ΛCDM framework, presenting nonrelativistic matter inhomogeneities as discrete massive particles, we develop the second‐order cosmological perturbation theory. Our approach relies on the weak gravitational field limit. The derived equations for the second‐order scalar, vector, and tensor metric corrections are suitable at arbitrary distances, including regions with nonlinear contrasts of the matter density. We thoroughly verify fulfillment of all Einstein equations, as well as self‐consistency of order assignments. In addition, we achieve logical positive results in the Minkowski background limit. Feasible investigations of the cosmological backreaction manifestations by means of relativistic simulations are also outlined.
Text Book: An Introduction to Mechanics by Kleppner and Kolenkow
Chapter 1: Vectors and Kinematics
-Explain the concept of vectors.
-Explain the concepts of position, velocity and acceleration for different kinds of motion.
References:
Halliday, Resnick and Walker
Berkley Physics Volume-1
Microscopic Mechanisms of Superconducting Flux Quantum and Superconducting an...Qiang LI
We have provided microscopic explanations to superconducting flux quantum and (superconducting and normal) persistent current. Flux quantum is generated by current carried by "deep electrons" at surface states. And values of the flux quantum differs according to the electronic states and coupling of the carrier electrons. Generation of persistent carrier electrons does not dissipate energy; instead there would be emission of real phonons and release of corresponding energy into the environment; but the normal carrier electrons involved still dissipate energy. Even for or persistent carriers,there should be a build-up of energy of the middle state and a build-up of the probability of virtual transition of electrons to the middle state, and the corresponding relaxation should exist accordingly.
The French Revolution, which began in 1789, was a period of radical social and political upheaval in France. It marked the decline of absolute monarchies, the rise of secular and democratic republics, and the eventual rise of Napoleon Bonaparte. This revolutionary period is crucial in understanding the transition from feudalism to modernity in Europe.
For more information, visit-www.vavaclasses.com
Instructions for Submissions thorugh G- Classroom.pptxJheel Barad
This presentation provides a briefing on how to upload submissions and documents in Google Classroom. It was prepared as part of an orientation for new Sainik School in-service teacher trainees. As a training officer, my goal is to ensure that you are comfortable and proficient with this essential tool for managing assignments and fostering student engagement.
Read| The latest issue of The Challenger is here! We are thrilled to announce that our school paper has qualified for the NATIONAL SCHOOLS PRESS CONFERENCE (NSPC) 2024. Thank you for your unwavering support and trust. Dive into the stories that made us stand out!
Synthetic Fiber Construction in lab .pptxPavel ( NSTU)
Synthetic fiber production is a fascinating and complex field that blends chemistry, engineering, and environmental science. By understanding these aspects, students can gain a comprehensive view of synthetic fiber production, its impact on society and the environment, and the potential for future innovations. Synthetic fibers play a crucial role in modern society, impacting various aspects of daily life, industry, and the environment. ynthetic fibers are integral to modern life, offering a range of benefits from cost-effectiveness and versatility to innovative applications and performance characteristics. While they pose environmental challenges, ongoing research and development aim to create more sustainable and eco-friendly alternatives. Understanding the importance of synthetic fibers helps in appreciating their role in the economy, industry, and daily life, while also emphasizing the need for sustainable practices and innovation.
Unit 8 - Information and Communication Technology (Paper I).pdfThiyagu K
This slides describes the basic concepts of ICT, basics of Email, Emerging Technology and Digital Initiatives in Education. This presentations aligns with the UGC Paper I syllabus.
Biological screening of herbal drugs: Introduction and Need for
Phyto-Pharmacological Screening, New Strategies for evaluating
Natural Products, In vitro evaluation techniques for Antioxidants, Antimicrobial and Anticancer drugs. In vivo evaluation techniques
for Anti-inflammatory, Antiulcer, Anticancer, Wound healing, Antidiabetic, Hepatoprotective, Cardio protective, Diuretics and
Antifertility, Toxicity studies as per OECD guidelines
Acetabularia Information For Class 9 .docxvaibhavrinwa19
Acetabularia acetabulum is a single-celled green alga that in its vegetative state is morphologically differentiated into a basal rhizoid and an axially elongated stalk, which bears whorls of branching hairs. The single diploid nucleus resides in the rhizoid.
4. Velocity & Acceleration in
Terms of x
If v = f(x);
2
2
2
2
1
v
dx
d
dt
xd
Proof:
dt
dv
dt
xd
2
2
5. Velocity & Acceleration in
Terms of x
If v = f(x);
2
2
2
2
1
v
dx
d
dt
xd
Proof:
dt
dv
dt
xd
2
2
dt
dx
dx
dv
6. Velocity & Acceleration in
Terms of x
If v = f(x);
2
2
2
2
1
v
dx
d
dt
xd
Proof:
dt
dv
dt
xd
2
2
dt
dx
dx
dv
v
dx
dv
7. Velocity & Acceleration in
Terms of x
If v = f(x);
2
2
2
2
1
v
dx
d
dt
xd
Proof:
dt
dv
dt
xd
2
2
dt
dx
dx
dv
v
dx
dv
2
2
1
v
dv
d
dx
dv
8. Velocity & Acceleration in
Terms of x
If v = f(x);
2
2
2
2
1
v
dx
d
dt
xd
Proof:
dt
dv
dt
xd
2
2
dt
dx
dx
dv
v
dx
dv
2
2
1
v
dv
d
dx
dv
2
2
1
v
dx
d
9. e.g. (i) A particle moves in a straight line so that
Find its velocity in terms of x given that v = 2 when x = 1.
xx 23
10. e.g. (i) A particle moves in a straight line so that
Find its velocity in terms of x given that v = 2 when x = 1.
xv
dx
d
23
2
1 2
xx 23
11. e.g. (i) A particle moves in a straight line so that
Find its velocity in terms of x given that v = 2 when x = 1.
xx 23
xv
dx
d
23
2
1 2
cxxv 22
3
2
1
12. e.g. (i) A particle moves in a straight line so that
Find its velocity in terms of x given that v = 2 when x = 1.
xx 23
xv
dx
d
23
2
1 2
cxxv 22
3
2
1
0
1132
2
1
i.e.
2,1when
22
c
c
vx
13. e.g. (i) A particle moves in a straight line so that
Find its velocity in terms of x given that v = 2 when x = 1.
xx 23
xv
dx
d
23
2
1 2
cxxv 22
3
2
1
0
1132
2
1
i.e.
2,1when
22
c
c
vx
22
26 xxv
14. e.g. (i) A particle moves in a straight line so that
Find its velocity in terms of x given that v = 2 when x = 1.
xx 23
xv
dx
d
23
2
1 2
cxxv 22
3
2
1
0
1132
2
1
i.e.
2,1when
22
c
c
vx
22
26 xxv
2
26 xxv
15. e.g. (i) A particle moves in a straight line so that
Find its velocity in terms of x given that v = 2 when x = 1.
xx 23
xv
dx
d
23
2
1 2
cxxv 22
3
2
1
0
1132
2
1
i.e.
2,1when
22
c
c
vx
22
26 xxv
2
26 xxv
NOTE:
02
v
16. e.g. (i) A particle moves in a straight line so that
Find its velocity in terms of x given that v = 2 when x = 1.
xx 23
xv
dx
d
23
2
1 2
cxxv 22
3
2
1
0
1132
2
1
i.e.
2,1when
22
c
c
vx
22
26 xxv
2
26 xxv
NOTE:
02
v
026 2
xx
17. e.g. (i) A particle moves in a straight line so that
Find its velocity in terms of x given that v = 2 when x = 1.
xx 23
xv
dx
d
23
2
1 2
cxxv 22
3
2
1
0
1132
2
1
i.e.
2,1when
22
c
c
vx
22
26 xxv
2
26 xxv
NOTE:
02
v
026 2
xx
032 xx
18. e.g. (i) A particle moves in a straight line so that
Find its velocity in terms of x given that v = 2 when x = 1.
xx 23
xv
dx
d
23
2
1 2
cxxv 22
3
2
1
0
1132
2
1
i.e.
2,1when
22
c
c
vx
22
26 xxv
2
26 xxv
NOTE:
02
v
026 2
xx
032 xx
30 x
19. e.g. (i) A particle moves in a straight line so that
Find its velocity in terms of x given that v = 2 when x = 1.
xx 23
xv
dx
d
23
2
1 2
cxxv 22
3
2
1
0
1132
2
1
i.e.
2,1when
22
c
c
vx
22
26 xxv
2
26 xxv
NOTE:
02
v
026 2
xx
032 xx
30 x
Particle moves between x = 0
and x = 3 and nowhere else.
20. 2
3xx
m/s2
(ii) A particle’s acceleration is given by . Initially, the particle is
1 unit to the right of O, and is traveling with a velocity of in
the negative direction. Find x in terms of t.
21. 2
3xx
m/s2
(ii) A particle’s acceleration is given by . Initially, the particle is
1 unit to the right of O, and is traveling with a velocity of in
the negative direction. Find x in terms of t.
22
3
2
1
xv
dx
d
22. 2
3xx
m/s2
(ii) A particle’s acceleration is given by . Initially, the particle is
1 unit to the right of O, and is traveling with a velocity of in
the negative direction. Find x in terms of t.
22
3
2
1
xv
dx
d
cxv 32
2
1
23. 2
3xx
m/s2
(ii) A particle’s acceleration is given by . Initially, the particle is
1 unit to the right of O, and is traveling with a velocity of in
the negative direction. Find x in terms of t.
22
3
2
1
xv
dx
d
0
12
2
1
i.e.
2,1,0when
32
c
c
vxt
cxv 32
2
1
24. 2
3xx
m/s2
(ii) A particle’s acceleration is given by . Initially, the particle is
1 unit to the right of O, and is traveling with a velocity of in
the negative direction. Find x in terms of t.
22
3
2
1
xv
dx
d
0
12
2
1
i.e.
2,1,0when
32
c
c
vxt
cxv 32
2
1
3
32
2
2
xv
xv
25. 2
3xx
m/s2
(ii) A particle’s acceleration is given by . Initially, the particle is
1 unit to the right of O, and is traveling with a velocity of in
the negative direction. Find x in terms of t.
22
3
2
1
xv
dx
d
0
12
2
1
i.e.
2,1,0when
32
c
c
vxt
cxv 32
2
1
3
32
2
2
xv
xv
3
2x
dt
dx
26. 2
3xx
m/s2
(ii) A particle’s acceleration is given by . Initially, the particle is
1 unit to the right of O, and is traveling with a velocity of in
the negative direction. Find x in terms of t.
22
3
2
1
xv
dx
d
0
12
2
1
i.e.
2,1,0when
32
c
c
vxt
cxv 32
2
1
3
32
2
2
xv
xv
3
2x
dt
dx
(Choose –ve to satisfy
the initial conditions)
27. 2
3xx
m/s2
(ii) A particle’s acceleration is given by . Initially, the particle is
1 unit to the right of O, and is traveling with a velocity of in
the negative direction. Find x in terms of t.
22
3
2
1
xv
dx
d
0
12
2
1
i.e.
2,1,0when
32
c
c
vxt
cxv 32
2
1
3
32
2
2
xv
xv
3
2x
dt
dx
2
3
2x
(Choose –ve to satisfy
the initial conditions)
28. 2
3xx
m/s2
(ii) A particle’s acceleration is given by . Initially, the particle is
1 unit to the right of O, and is traveling with a velocity of in
the negative direction. Find x in terms of t.
22
3
2
1
xv
dx
d
0
12
2
1
i.e.
2,1,0when
32
c
c
vxt
cxv 32
2
1
3
32
2
2
xv
xv
3
2x
dt
dx
2
3
2x
(Choose –ve to satisfy
the initial conditions)
2
3
2
1
x
dx
dt
41. A particle is moving along the x axis starting from a position 2 metres to
the right of the origin (that is, x = 2 when t = 0) with an initial velocity
of 5 m/s and an acceleration given by
2004 Extension 1 HSC Q5a)
xxx 22 3
(i) Show that 12
xx
42. A particle is moving along the x axis starting from a position 2 metres to
the right of the origin (that is, x = 2 when t = 0) with an initial velocity
of 5 m/s and an acceleration given by
2004 Extension 1 HSC Q5a)
xxx 22 3
(i) Show that 12
xx
xxv
dx
d
22
2
1 32
43. A particle is moving along the x axis starting from a position 2 metres to
the right of the origin (that is, x = 2 when t = 0) with an initial velocity
of 5 m/s and an acceleration given by
2004 Extension 1 HSC Q5a)
xxx 22 3
(i) Show that 12
xx
xxv
dx
d
22
2
1 32
cxxv 242
2
1
2
1
44. A particle is moving along the x axis starting from a position 2 metres to
the right of the origin (that is, x = 2 when t = 0) with an initial velocity
of 5 m/s and an acceleration given by
2004 Extension 1 HSC Q5a)
xxx 22 3
(i) Show that 12
xx
xxv
dx
d
22
2
1 32
cxxv 242
2
1
2
1
When x = 2, v = 5
45. A particle is moving along the x axis starting from a position 2 metres to
the right of the origin (that is, x = 2 when t = 0) with an initial velocity
of 5 m/s and an acceleration given by
2004 Extension 1 HSC Q5a)
xxx 22 3
(i) Show that 12
xx
xxv
dx
d
22
2
1 32
cxxv 242
2
1
2
1
When x = 2, v = 5
1 1
25 16 4
2 2
1
2
c
c
46. A particle is moving along the x axis starting from a position 2 metres to
the right of the origin (that is, x = 2 when t = 0) with an initial velocity
of 5 m/s and an acceleration given by
2004 Extension 1 HSC Q5a)
xxx 22 3
(i) Show that 12
xx
xxv
dx
d
22
2
1 32
cxxv 242
2
1
2
1
When x = 2, v = 5
1 1
25 16 4
2 2
1
2
c
c
12 242
xxv
47. A particle is moving along the x axis starting from a position 2 metres to
the right of the origin (that is, x = 2 when t = 0) with an initial velocity
of 5 m/s and an acceleration given by
2004 Extension 1 HSC Q5a)
xxx 22 3
(i) Show that 12
xx
xxv
dx
d
22
2
1 32
cxxv 242
2
1
2
1
When x = 2, v = 5
1 1
25 16 4
2 2
1
2
c
c
12 242
xxv
222
1 xv
48. A particle is moving along the x axis starting from a position 2 metres to
the right of the origin (that is, x = 2 when t = 0) with an initial velocity
of 5 m/s and an acceleration given by
2004 Extension 1 HSC Q5a)
xxx 22 3
(i) Show that 12
xx
xxv
dx
d
22
2
1 32
cxxv 242
2
1
2
1
When x = 2, v = 5
1 1
25 16 4
2 2
1
2
c
c
12 242
xxv
222
1 xv
12
xv
49. A particle is moving along the x axis starting from a position 2 metres to
the right of the origin (that is, x = 2 when t = 0) with an initial velocity
of 5 m/s and an acceleration given by
2004 Extension 1 HSC Q5a)
xxx 22 3
(i) Show that 12
xx
xxv
dx
d
22
2
1 32
cxxv 242
2
1
2
1
When x = 2, v = 5
1 1
25 16 4
2 2
1
2
c
c
12 242
xxv
222
1 xv
12
xv
Note: v > 0, in order
to satisfy initial
conditions
51. (ii) Hence find an expression for x in terms of t
12
x
dt
dx
52. (ii) Hence find an expression for x in terms of t
12
x
dt
dx
xt
x
dx
dt
2
2
0
1
53. (ii) Hence find an expression for x in terms of t
12
x
dt
dx
xt
x
dx
dt
2
2
0
1
x
xt 2
1
tan
54. (ii) Hence find an expression for x in terms of t
12
x
dt
dx
xt
x
dx
dt
2
2
0
1
x
xt 2
1
tan
2tantan 11
xt
55. (ii) Hence find an expression for x in terms of t
12
x
dt
dx
xt
x
dx
dt
2
2
0
1
x
xt 2
1
tan
2tantan 11
xt
2tantan 11
tx
56. (ii) Hence find an expression for x in terms of t
12
x
dt
dx
xt
x
dx
dt
2
2
0
1
x
xt 2
1
tan
2tantan 11
xt
2tantan 11
tx
2tantan 1
tx
57. (ii) Hence find an expression for x in terms of t
12
x
dt
dx
xt
x
dx
dt
2
2
0
1
x
xt 2
1
tan
2tantan 11
xt
2tantan 11
tx
2tantan 1
tx
t
t
x
tan21
2tan
58. (ii) Hence find an expression for x in terms of t
12
x
dt
dx
xt
x
dx
dt
2
2
0
1
x
xt 2
1
tan
2tantan 11
xt
2tantan 11
tx
2tantan 1
tx
t
t
x
tan21
2tan
Exercise 3E; 1 to 3 acfh,
7 , 9, 11, 13, 15, 17, 18,
20, 21, 24*