The document discusses solving ordinary differential equations using Taylor's series method. It presents the Taylor's series for the first order differential equation dy/dx = f(x,y) and gives an example of solving the equation y = x + y, y(0) = 1 using this method. The solution is obtained by taking the Taylor's series expansion and determining the derivatives of y evaluated at x0 = 0. The values of y are computed at x = 0.1 and x = 0.2. A second example solves the differential equation dy/dx = 3x + y^2 using the same approach.
This presentation gives the basic idea about the methods of solving ODEs
The methods like variation of parameters, undetermined coefficient method, 1/f(D) method, Particular integral and complimentary functions of an ODE
This presentation gives the basic idea about the methods of solving ODEs
The methods like variation of parameters, undetermined coefficient method, 1/f(D) method, Particular integral and complimentary functions of an ODE
Introduction of process control, Process control, Example of controlled process, Feedback control system, Feed forward control system,Classification of variables in chemical process, Components of control system
Series solution of ordinary differential equation
advance engineering mathematics
The power series method is the standard method for solving linear ODEs with variable
coefficients. It gives solutions in the form of power series. These series can be used for computing values, graphing curves, proving formulas, and exploring properties of
solutions, as we shall see.
1. Which of the following is the correct matrix representation .docxjackiewalcutt
1.
Which of the following is the correct matrix representation of the October Inventory of small and large t-shirts and pants?
Inventory for August
Inventory for September
Inventory for October
Small
Large
Small
Large
Small
Large
T-Shirts
2
3
4
6
7
8
Pants
1
4
3
5
5
6
Answer
1.
If find -2A.
Answer
1.
If and find A - B.
Answer
1.
If find 2A.
Answer
1.
Matrix A has dimensions 2 x 3. Matrix B has dimensions 3 x 6. These two matrices can be multiplied to find the product AB.
Answer True False
1.
Evaluate
Answer
Does not exist.
1.
Evaluate
Answer
Does not exist
1.
Evaluate
Answer
Does not exist.
1.
Find the determinant of
Answer
14
-14
1
-1
1.
Find the determinant of
Answer
-48
-56
56
48
1.
What is the determinant of the following matrix?
Answer
-10
-14
-20
-25
1.
What is the determinant of the following matrix? Does the matrix have an inverse?
Answer
5; no
5; yes
1; no
1; yes
1.
Is the following system consistent or inconsistent?
8x + y + 4 = 0
y = -8x - 4
Answer
consistent
inconsistent
1.
Is the following system consistent or inconsistent?
7x + 6 = -2y
-14x -4y + 2 = 0
Answer
consistent
inconsistent
1.
Is the following system consistent or inconsistent?
-2x - 2y = 6
10x + 10y = -30
Answer
consistent
inconsistent
1.
Is the following system consistent or inconsistent?
2y = x - 7
-2x - 6y = -14
Answer
consistent
inconsistent
1.
Is the following system consistent or inconsistent?
y = 2x + 5
-2x + y = -2
Answer
consistent
inconsistent
If a system has exactly one solution it is called _______________.
Answer
consistent
inconsistent
independent
dependent
1.
Does the following system of equations have a solution?
Answer
Yes
No
1.
What is the approximate solution of the following system of equations?
Answer
(2, -7)
(-7, 2)
(7, 2)
(-7, -2)
1.
Solve the following system of equations by using the substitution method.
3y – 2x = 11
y + 2x = 9
Answer
(2, 5)
(-2, -5)
(4, 5)
Inconsistent
1.
Solve the following system of equations by using the substitution method.
y = -3x + 5
5x – 4y = -3
Answer
(-1, -2)
(2, 1)
(3, 4)
(1, 2)
1.
Solve the following system of equations by using the elimination method.
x – y = 11
2x + y = 19
Answer
(1, 10)
(-1, -1)
(12, 2)
(10, -1)
1.
Solve the following system of equations by using the elimination method.
-4x – 2y = -12
4x + 8y = -24
Answer
(5, 3)
(-6, -6)
(3, 1)
(6, -6)
1.
Solve the following system of equations using matrices.
3x – 2y = 31
3x + 2y = -1
Answer
(5, -8)
(3, 5)
(-3, 9)
(2, 8)
1.
Solve the following system of equations using matrices.
4x + 5y = -7
3x – 6y = 24
Answer
(1, 4)
(2, -3)
(5, 6)
(3, 4)
1.
The sum of two numbers is 7. Four times the first number is one more than 5 times the second. Find the two numbe ...
Operation “Blue Star” is the only event in the history of Independent India where the state went into war with its own people. Even after about 40 years it is not clear if it was culmination of states anger over people of the region, a political game of power or start of dictatorial chapter in the democratic setup.
The people of Punjab felt alienated from main stream due to denial of their just demands during a long democratic struggle since independence. As it happen all over the word, it led to militant struggle with great loss of lives of military, police and civilian personnel. Killing of Indira Gandhi and massacre of innocent Sikhs in Delhi and other India cities was also associated with this movement.
Model Attribute Check Company Auto PropertyCeline George
In Odoo, the multi-company feature allows you to manage multiple companies within a single Odoo database instance. Each company can have its own configurations while still sharing common resources such as products, customers, and suppliers.
2024.06.01 Introducing a competency framework for languag learning materials ...Sandy Millin
http://sandymillin.wordpress.com/iateflwebinar2024
Published classroom materials form the basis of syllabuses, drive teacher professional development, and have a potentially huge influence on learners, teachers and education systems. All teachers also create their own materials, whether a few sentences on a blackboard, a highly-structured fully-realised online course, or anything in between. Despite this, the knowledge and skills needed to create effective language learning materials are rarely part of teacher training, and are mostly learnt by trial and error.
Knowledge and skills frameworks, generally called competency frameworks, for ELT teachers, trainers and managers have existed for a few years now. However, until I created one for my MA dissertation, there wasn’t one drawing together what we need to know and do to be able to effectively produce language learning materials.
This webinar will introduce you to my framework, highlighting the key competencies I identified from my research. It will also show how anybody involved in language teaching (any language, not just English!), teacher training, managing schools or developing language learning materials can benefit from using the framework.
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.
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.
How to Make a Field invisible in Odoo 17Celine George
It is possible to hide or invisible some fields in odoo. Commonly using “invisible” attribute in the field definition to invisible the fields. This slide will show how to make a field invisible in odoo 17.
Embracing GenAI - A Strategic ImperativePeter Windle
Artificial Intelligence (AI) technologies such as Generative AI, Image Generators and Large Language Models have had a dramatic impact on teaching, learning and assessment over the past 18 months. The most immediate threat AI posed was to Academic Integrity with Higher Education Institutes (HEIs) focusing their efforts on combating the use of GenAI in assessment. Guidelines were developed for staff and students, policies put in place too. Innovative educators have forged paths in the use of Generative AI for teaching, learning and assessments leading to pockets of transformation springing up across HEIs, often with little or no top-down guidance, support or direction.
This Gasta posits a strategic approach to integrating AI into HEIs to prepare staff, students and the curriculum for an evolving world and workplace. We will highlight the advantages of working with these technologies beyond the realm of teaching, learning and assessment by considering prompt engineering skills, industry impact, curriculum changes, and the need for staff upskilling. In contrast, not engaging strategically with Generative AI poses risks, including falling behind peers, missed opportunities and failing to ensure our graduates remain employable. The rapid evolution of AI technologies necessitates a proactive and strategic approach if we are to remain relevant.
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
Introduction to AI for Nonprofits with Tapp NetworkTechSoup
Dive into the world of AI! Experts Jon Hill and Tareq Monaur will guide you through AI's role in enhancing nonprofit websites and basic marketing strategies, making it easy to understand and apply.
1. Numerical Methods
Ordinary Differential Equations - 1
Dr. N. B. Vyas
Department of Mathematics,
Atmiya Institute of Technology & Science,
Rajkot (Gujarat) - INDIA
niravbvyas@gmail.com
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
2. Ordinary Differential Equations
Taylor’s Series Method:
Consider the first order Differential Equation
dy
dx
= f(x, y), y(x0) = y0
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
3. Ordinary Differential Equations
Taylor’s Series Method:
Consider the first order Differential Equation
dy
dx
= f(x, y), y(x0) = y0
The Taylor’s series is
y(x) = y(x0) +
(x − x0)
1!
y (x0) +
(x − x0)2
2!
y (x0) + . . .
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
4. Taylor’s Series Method
Ex:1
Solve y = x + y, y(0) = 1 by Taylor’s series
method. Hence find values of y at x = 0.1 and
x = 0.2
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
5. Taylor’s Series Method
Sol.: Here y = f(x, y) = x + y, x0 = 0 and y0 = 1
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
6. Taylor’s Series Method
Sol.: Here y = f(x, y) = x + y, x0 = 0 and y0 = 1
y = x + y
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
7. Taylor’s Series Method
Sol.: Here y = f(x, y) = x + y, x0 = 0 and y0 = 1
y = x + y ⇒ y (0) = 1
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
8. Taylor’s Series Method
Sol.: Here y = f(x, y) = x + y, x0 = 0 and y0 = 1
y = x + y ⇒ y (0) = 1
y = 1 + y
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
9. Taylor’s Series Method
Sol.: Here y = f(x, y) = x + y, x0 = 0 and y0 = 1
y = x + y ⇒ y (0) = 1
y = 1 + y ⇒ y (0) = 1 + y (0) = 1 + 1 = 2
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
10. Taylor’s Series Method
Sol.: Here y = f(x, y) = x + y, x0 = 0 and y0 = 1
y = x + y ⇒ y (0) = 1
y = 1 + y ⇒ y (0) = 1 + y (0) = 1 + 1 = 2
y = y
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
11. Taylor’s Series Method
Sol.: Here y = f(x, y) = x + y, x0 = 0 and y0 = 1
y = x + y ⇒ y (0) = 1
y = 1 + y ⇒ y (0) = 1 + y (0) = 1 + 1 = 2
y = y ⇒ y (0) = y (0) = 2
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
12. Taylor’s Series Method
Sol.: Here y = f(x, y) = x + y, x0 = 0 and y0 = 1
y = x + y ⇒ y (0) = 1
y = 1 + y ⇒ y (0) = 1 + y (0) = 1 + 1 = 2
y = y ⇒ y (0) = y (0) = 2
yiv
= y
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
13. Taylor’s Series Method
Sol.: Here y = f(x, y) = x + y, x0 = 0 and y0 = 1
y = x + y ⇒ y (0) = 1
y = 1 + y ⇒ y (0) = 1 + y (0) = 1 + 1 = 2
y = y ⇒ y (0) = y (0) = 2
yiv
= y ⇒ yiv
(0) = y (0) = 2 . . .
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
14. Taylor’s Series Method
Sol.: Here y = f(x, y) = x + y, x0 = 0 and y0 = 1
y = x + y ⇒ y (0) = 1
y = 1 + y ⇒ y (0) = 1 + y (0) = 1 + 1 = 2
y = y ⇒ y (0) = y (0) = 2
yiv
= y ⇒ yiv
(0) = y (0) = 2 . . .
Taylor’s series is
y(x) = y(x0)+
(x − x0)
1!
y (x0)+
(x − x0)2
2!
y (x0)+. . .
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
15. Taylor’s Series Method
y(x) = 1 + xy (0) +
x2
2!
y (0) +
x3
3!
y (0) . . .
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
16. Taylor’s Series Method
y(x) = 1 + xy (0) +
x2
2!
y (0) +
x3
3!
y (0) . . .
= 1 + x(1) +
x2
2
(2) +
x3
6
(2) +
x4
24
(2) + . . .
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
17. Taylor’s Series Method
y(x) = 1 + xy (0) +
x2
2!
y (0) +
x3
3!
y (0) . . .
= 1 + x(1) +
x2
2
(2) +
x3
6
(2) +
x4
24
(2) + . . .
= 1 + x + x2
+
x3
3
+
x4
12
+ . . .
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
18. Taylor’s Series Method
y(x) = 1 + xy (0) +
x2
2!
y (0) +
x3
3!
y (0) . . .
= 1 + x(1) +
x2
2
(2) +
x3
6
(2) +
x4
24
(2) + . . .
= 1 + x + x2
+
x3
3
+
x4
12
+ . . .
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
24. Taylor’s Series
Ex Using Taylor’s series method, obtain the solution
of
dy
dx
= 3x + y2
, given that y(0) = 1. Find the
value of y for x = 0.1
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
25. Taylor’s Series
Sol. Here,y = f(x, y) = 3x + y2
, x0 = 0 and y0 = 1.
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
26. Taylor’s Series
Sol. Here,y = f(x, y) = 3x + y2
, x0 = 0 and y0 = 1.
y = 3x + y2
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
27. Taylor’s Series
Sol. Here,y = f(x, y) = 3x + y2
, x0 = 0 and y0 = 1.
y = 3x + y2
⇒ y (x0) = 3(x0) + y2
0 = 3(0) + 1 = 1
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
28. Taylor’s Series
Sol. Here,y = f(x, y) = 3x + y2
, x0 = 0 and y0 = 1.
y = 3x + y2
⇒ y (x0) = 3(x0) + y2
0 = 3(0) + 1 = 1
y = 3 + 2yy
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
29. Taylor’s Series
Sol. Here,y = f(x, y) = 3x + y2
, x0 = 0 and y0 = 1.
y = 3x + y2
⇒ y (x0) = 3(x0) + y2
0 = 3(0) + 1 = 1
y = 3 + 2yy ⇒ y (x0) = 3 + 2(1)(1) = 5
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
30. Taylor’s Series
Sol. Here,y = f(x, y) = 3x + y2
, x0 = 0 and y0 = 1.
y = 3x + y2
⇒ y (x0) = 3(x0) + y2
0 = 3(0) + 1 = 1
y = 3 + 2yy ⇒ y (x0) = 3 + 2(1)(1) = 5
y = 2(y )2
+ 2yy
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
31. Taylor’s Series
Sol. Here,y = f(x, y) = 3x + y2
, x0 = 0 and y0 = 1.
y = 3x + y2
⇒ y (x0) = 3(x0) + y2
0 = 3(0) + 1 = 1
y = 3 + 2yy ⇒ y (x0) = 3 + 2(1)(1) = 5
y = 2(y )2
+ 2yy ⇒ y (x0) = 2(1)2
+ 2(5) = 12
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
32. Taylor’s Series
Sol. Here,y = f(x, y) = 3x + y2
, x0 = 0 and y0 = 1.
y = 3x + y2
⇒ y (x0) = 3(x0) + y2
0 = 3(0) + 1 = 1
y = 3 + 2yy ⇒ y (x0) = 3 + 2(1)(1) = 5
y = 2(y )2
+ 2yy ⇒ y (x0) = 2(1)2
+ 2(5) = 12
By Taylor’s series,
y(x) = y0+(x−x0)y (x0)+
(x − x0)2
2!
y (x0)+
(x − x0)3
3!
y (x0)+. . .
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
33. Taylor’s Series
Sol. Here,y = f(x, y) = 3x + y2
, x0 = 0 and y0 = 1.
y = 3x + y2
⇒ y (x0) = 3(x0) + y2
0 = 3(0) + 1 = 1
y = 3 + 2yy ⇒ y (x0) = 3 + 2(1)(1) = 5
y = 2(y )2
+ 2yy ⇒ y (x0) = 2(1)2
+ 2(5) = 12
By Taylor’s series,
y(x) = y0+(x−x0)y (x0)+
(x − x0)2
2!
y (x0)+
(x − x0)3
3!
y (x0)+. . .
= 1 + x +
x2
2!
(5) +
x3
3!
(12) + . . .
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
34. Taylor’s Series
Sol. Here,y = f(x, y) = 3x + y2
, x0 = 0 and y0 = 1.
y = 3x + y2
⇒ y (x0) = 3(x0) + y2
0 = 3(0) + 1 = 1
y = 3 + 2yy ⇒ y (x0) = 3 + 2(1)(1) = 5
y = 2(y )2
+ 2yy ⇒ y (x0) = 2(1)2
+ 2(5) = 12
By Taylor’s series,
y(x) = y0+(x−x0)y (x0)+
(x − x0)2
2!
y (x0)+
(x − x0)3
3!
y (x0)+. . .
= 1 + x +
x2
2!
(5) +
x3
3!
(12) + . . .
= 1 + x +
5x2
2!
+ 2x3
+ . . .
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
35. Taylor’s Series
Sol. Here,y = f(x, y) = 3x + y2
, x0 = 0 and y0 = 1.
y = 3x + y2
⇒ y (x0) = 3(x0) + y2
0 = 3(0) + 1 = 1
y = 3 + 2yy ⇒ y (x0) = 3 + 2(1)(1) = 5
y = 2(y )2
+ 2yy ⇒ y (x0) = 2(1)2
+ 2(5) = 12
By Taylor’s series,
y(x) = y0+(x−x0)y (x0)+
(x − x0)2
2!
y (x0)+
(x − x0)3
3!
y (x0)+. . .
= 1 + x +
x2
2!
(5) +
x3
3!
(12) + . . .
= 1 + x +
5x2
2!
+ 2x3
+ . . .
y(0.1) =
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
36. Taylor’s Series
Sol. Here,y = f(x, y) = 3x + y2
, x0 = 0 and y0 = 1.
y = 3x + y2
⇒ y (x0) = 3(x0) + y2
0 = 3(0) + 1 = 1
y = 3 + 2yy ⇒ y (x0) = 3 + 2(1)(1) = 5
y = 2(y )2
+ 2yy ⇒ y (x0) = 2(1)2
+ 2(5) = 12
By Taylor’s series,
y(x) = y0+(x−x0)y (x0)+
(x − x0)2
2!
y (x0)+
(x − x0)3
3!
y (x0)+. . .
= 1 + x +
x2
2!
(5) +
x3
3!
(12) + . . .
= 1 + x +
5x2
2!
+ 2x3
+ . . .
y(0.1) =
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
37. Taylor’s Series
Ex Using Taylor’s series method, find the solution of
dy
dx
= 2y + 3ex
, y(0) = 0,at x = 0.2
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
38. Taylor’s Series
Sol. Here,y = f(x, y) = 2y + 3ex
, x0 = 0 and y0 = 0.
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
39. Taylor’s Series
Sol. Here,y = f(x, y) = 2y + 3ex
, x0 = 0 and y0 = 0.
y = 2y + 3ex
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
40. Taylor’s Series
Sol. Here,y = f(x, y) = 2y + 3ex
, x0 = 0 and y0 = 0.
y = 2y + 3ex
⇒ y (x0) = 2(y0) + 3ex0
= 2(0) + 3e0
= 3
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
41. Taylor’s Series
Sol. Here,y = f(x, y) = 2y + 3ex
, x0 = 0 and y0 = 0.
y = 2y + 3ex
⇒ y (x0) = 2(y0) + 3ex0
= 2(0) + 3e0
= 3
y = 2y + 3ex
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
42. Taylor’s Series
Sol. Here,y = f(x, y) = 2y + 3ex
, x0 = 0 and y0 = 0.
y = 2y + 3ex
⇒ y (x0) = 2(y0) + 3ex0
= 2(0) + 3e0
= 3
y = 2y + 3ex
⇒ y (x0) = 2(y0) + 3ex0
= 2(3) + 3e0
= 9
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
43. Taylor’s Series
Sol. Here,y = f(x, y) = 2y + 3ex
, x0 = 0 and y0 = 0.
y = 2y + 3ex
⇒ y (x0) = 2(y0) + 3ex0
= 2(0) + 3e0
= 3
y = 2y + 3ex
⇒ y (x0) = 2(y0) + 3ex0
= 2(3) + 3e0
= 9
y = 2y + 3ex
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
44. Taylor’s Series
Sol. Here,y = f(x, y) = 2y + 3ex
, x0 = 0 and y0 = 0.
y = 2y + 3ex
⇒ y (x0) = 2(y0) + 3ex0
= 2(0) + 3e0
= 3
y = 2y + 3ex
⇒ y (x0) = 2(y0) + 3ex0
= 2(3) + 3e0
= 9
y = 2y + 3ex
⇒ y (x0) = 2(y0 ) + 3ex0
= 2(9) + 3e0
= 21
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
45. Taylor’s Series
Sol. Here,y = f(x, y) = 2y + 3ex
, x0 = 0 and y0 = 0.
y = 2y + 3ex
⇒ y (x0) = 2(y0) + 3ex0
= 2(0) + 3e0
= 3
y = 2y + 3ex
⇒ y (x0) = 2(y0) + 3ex0
= 2(3) + 3e0
= 9
y = 2y + 3ex
⇒ y (x0) = 2(y0 ) + 3ex0
= 2(9) + 3e0
= 21
yiv
= 2y + 3ex
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
46. Taylor’s Series
Sol. Here,y = f(x, y) = 2y + 3ex
, x0 = 0 and y0 = 0.
y = 2y + 3ex
⇒ y (x0) = 2(y0) + 3ex0
= 2(0) + 3e0
= 3
y = 2y + 3ex
⇒ y (x0) = 2(y0) + 3ex0
= 2(3) + 3e0
= 9
y = 2y + 3ex
⇒ y (x0) = 2(y0 ) + 3ex0
= 2(9) + 3e0
= 21
yiv
= 2y + 3ex
⇒ yiv
(x0) = 45
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
47. Taylor’s Series
Sol. Here,y = f(x, y) = 2y + 3ex
, x0 = 0 and y0 = 0.
y = 2y + 3ex
⇒ y (x0) = 2(y0) + 3ex0
= 2(0) + 3e0
= 3
y = 2y + 3ex
⇒ y (x0) = 2(y0) + 3ex0
= 2(3) + 3e0
= 9
y = 2y + 3ex
⇒ y (x0) = 2(y0 ) + 3ex0
= 2(9) + 3e0
= 21
yiv
= 2y + 3ex
⇒ yiv
(x0) = 45
By Taylor’s series,
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
48. Taylor’s Series
Sol. Here,y = f(x, y) = 2y + 3ex
, x0 = 0 and y0 = 0.
y = 2y + 3ex
⇒ y (x0) = 2(y0) + 3ex0
= 2(0) + 3e0
= 3
y = 2y + 3ex
⇒ y (x0) = 2(y0) + 3ex0
= 2(3) + 3e0
= 9
y = 2y + 3ex
⇒ y (x0) = 2(y0 ) + 3ex0
= 2(9) + 3e0
= 21
yiv
= 2y + 3ex
⇒ yiv
(x0) = 45
By Taylor’s series,
y(x) = y0+(x−x0)y (x0)+
(x − x0)2
2!
y (x0)+
(x − x0)3
3!
y (x0)+. . .
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
49. Taylor’s Series
Sol. Here,y = f(x, y) = 2y + 3ex
, x0 = 0 and y0 = 0.
y = 2y + 3ex
⇒ y (x0) = 2(y0) + 3ex0
= 2(0) + 3e0
= 3
y = 2y + 3ex
⇒ y (x0) = 2(y0) + 3ex0
= 2(3) + 3e0
= 9
y = 2y + 3ex
⇒ y (x0) = 2(y0 ) + 3ex0
= 2(9) + 3e0
= 21
yiv
= 2y + 3ex
⇒ yiv
(x0) = 45
By Taylor’s series,
y(x) = y0+(x−x0)y (x0)+
(x − x0)2
2!
y (x0)+
(x − x0)3
3!
y (x0)+. . .
= 0 + x(3) +
x2
2!
(9) +
x3
3!
(21) +
x4
4!
(45) + . . .
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
52. Taylor’s Series Method
Ex:
Use Taylor’s series method to solve
dy
dx
= x2
+ y2
,
y(0) = 1. Find y(0.1) correct up to 4 decimal
places.
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
53. Taylor’s Series Method
Ex:
Use Taylor’s series method to solve
dy
dx
= x2
y − 1,
y(0) = 1. Find y(0.03).
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
55. Picard’s Method
Picard’s Method:
Consider the first order differential equation.
dy
dx
= f(x, y) − − − (1)
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
56. Picard’s Method
Picard’s Method:
Consider the first order differential equation.
dy
dx
= f(x, y) − − − (1)
subject to y(x0) = y0
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
57. Picard’s Method
Picard’s Method:
Consider the first order differential equation.
dy
dx
= f(x, y) − − − (1)
subject to y(x0) = y0
The equation (1) can be written as
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
58. Picard’s Method
Picard’s Method:
Consider the first order differential equation.
dy
dx
= f(x, y) − − − (1)
subject to y(x0) = y0
The equation (1) can be written as
dy = f(x, y)dx
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
59. Picard’s Method
Picard’s Method:
Consider the first order differential equation.
dy
dx
= f(x, y) − − − (1)
subject to y(x0) = y0
The equation (1) can be written as
dy = f(x, y)dx
Integrating between the limits for x and y, we get
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
60. Picard’s Method
Picard’s Method:
Consider the first order differential equation.
dy
dx
= f(x, y) − − − (1)
subject to y(x0) = y0
The equation (1) can be written as
dy = f(x, y)dx
Integrating between the limits for x and y, we get
y
y0
dy =
x
x0
f(x, y)dx
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
61. Picard’s Method
Picard’s Method:
Consider the first order differential equation.
dy
dx
= f(x, y) − − − (1)
subject to y(x0) = y0
The equation (1) can be written as
dy = f(x, y)dx
Integrating between the limits for x and y, we get
y
y0
dy =
x
x0
f(x, y)dx
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
62. Picard’s Method
(y − y0) =
x
x0
f(x, y)dx
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
63. Picard’s Method
(y − y0) =
x
x0
f(x, y)dx
y = y0 +
x
x0
f(x, y)dx − − − (2)
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
64. Picard’s Method
(y − y0) =
x
x0
f(x, y)dx
y = y0 +
x
x0
f(x, y)dx − − − (2)
Equation (2) is known as integral equation and
can be solved by successive approximation or
iteration.
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
65. Picard’s Method
(y − y0) =
x
x0
f(x, y)dx
y = y0 +
x
x0
f(x, y)dx − − − (2)
Equation (2) is known as integral equation and
can be solved by successive approximation or
iteration.
Now by Picard’s method, for 1st
approximation
y1
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
66. Picard’s Method
(y − y0) =
x
x0
f(x, y)dx
y = y0 +
x
x0
f(x, y)dx − − − (2)
Equation (2) is known as integral equation and
can be solved by successive approximation or
iteration.
Now by Picard’s method, for 1st
approximation
y1
we replace y by y0 in f(x, y) in R.H.S of eq. (2),
we get
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
67. Picard’s Method
(y − y0) =
x
x0
f(x, y)dx
y = y0 +
x
x0
f(x, y)dx − − − (2)
Equation (2) is known as integral equation and
can be solved by successive approximation or
iteration.
Now by Picard’s method, for 1st
approximation
y1
we replace y by y0 in f(x, y) in R.H.S of eq. (2),
we get
y1 = y0 +
x
x0
f(x, y0)dx
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
69. Picard’s Method
For 2nd
approximation y2,
we replace y by y1 in f(x, y) in R.H.S of eq. (2),
we get
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
70. Picard’s Method
For 2nd
approximation y2,
we replace y by y1 in f(x, y) in R.H.S of eq. (2),
we get
y2 = y0 +
x
x0
f(x, y1)dx
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
71. Picard’s Method
For 2nd
approximation y2,
we replace y by y1 in f(x, y) in R.H.S of eq. (2),
we get
y2 = y0 +
x
x0
f(x, y1)dx
In general,
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
72. Picard’s Method
For 2nd
approximation y2,
we replace y by y1 in f(x, y) in R.H.S of eq. (2),
we get
y2 = y0 +
x
x0
f(x, y1)dx
In general,
yn+1 = y0 +
x
x0
f(x, yn)dx for n = 0, 1, 2, . . .
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
73. Picard’s Method
For 2nd
approximation y2,
we replace y by y1 in f(x, y) in R.H.S of eq. (2),
we get
y2 = y0 +
x
x0
f(x, y1)dx
In general,
yn+1 = y0 +
x
x0
f(x, yn)dx for n = 0, 1, 2, . . .
stop the process when the two consecutive values
of y are same up to desired accuracy.
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
74. Picard’s Method
Note:
This method is applicable to a limited class of
equations in which the successive integration can
be performed easily.
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
75. Picard’s Method
Ex Using Picard’s method solve
dy
dx
= 3 + 2xy where y(0) = 1 for x = 0.1.
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
76. Picard’s Method
Sol.:
By Picard’s method yn+1 = y0 +
x
x0
f(x, yn) dx
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
77. Picard’s Method
Sol.:
By Picard’s method yn+1 = y0 +
x
x0
f(x, yn) dx
Here x0 = 0, y0 = 1, f(x, y) = 3 + 2xy
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
78. Picard’s Method
Sol.:
By Picard’s method yn+1 = y0 +
x
x0
f(x, yn) dx
Here x0 = 0, y0 = 1, f(x, y) = 3 + 2xy
1st
approximation:
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
79. Picard’s Method
Sol.:
By Picard’s method yn+1 = y0 +
x
x0
f(x, yn) dx
Here x0 = 0, y0 = 1, f(x, y) = 3 + 2xy
1st
approximation:
put n = 0 and y0 = 1 in f(x, y)
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
80. Picard’s Method
Sol.:
By Picard’s method yn+1 = y0 +
x
x0
f(x, yn) dx
Here x0 = 0, y0 = 1, f(x, y) = 3 + 2xy
1st
approximation:
put n = 0 and y0 = 1 in f(x, y)
y1 = 1 +
x
0
(3 + 2x) dx
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
81. Picard’s Method
Sol.:
By Picard’s method yn+1 = y0 +
x
x0
f(x, yn) dx
Here x0 = 0, y0 = 1, f(x, y) = 3 + 2xy
1st
approximation:
put n = 0 and y0 = 1 in f(x, y)
y1 = 1 +
x
0
(3 + 2x) dx
∴ y1 = 1 + 3x + x2
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
84. Picard’s Method
2nd
approximation:
put n = 1 and y1 = 1 + 3x + x2
in f(x, y)
y2 = 1 +
x
0
3 + 2x(1 + 3x + x2
) dx
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
85. Picard’s Method
2nd
approximation:
put n = 1 and y1 = 1 + 3x + x2
in f(x, y)
y2 = 1 +
x
0
3 + 2x(1 + 3x + x2
) dx
= 1 +
x
0
3 + 2x + 6x2
+ 2x3
) dx
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
86. Picard’s Method
2nd
approximation:
put n = 1 and y1 = 1 + 3x + x2
in f(x, y)
y2 = 1 +
x
0
3 + 2x(1 + 3x + x2
) dx
= 1 +
x
0
3 + 2x + 6x2
+ 2x3
) dx
∴ y2 = 1 + 3x + x2
+ 2x3
+
x4
2
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
87. Picard’s Method
2nd
approximation:
put n = 1 and y1 = 1 + 3x + x2
in f(x, y)
y2 = 1 +
x
0
3 + 2x(1 + 3x + x2
) dx
= 1 +
x
0
3 + 2x + 6x2
+ 2x3
) dx
∴ y2 = 1 + 3x + x2
+ 2x3
+
x4
2
which is approximate solution, putting x = 0.1
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
88. Picard’s Method
2nd
approximation:
put n = 1 and y1 = 1 + 3x + x2
in f(x, y)
y2 = 1 +
x
0
3 + 2x(1 + 3x + x2
) dx
= 1 +
x
0
3 + 2x + 6x2
+ 2x3
) dx
∴ y2 = 1 + 3x + x2
+ 2x3
+
x4
2
which is approximate solution, putting x = 0.1
y(0.1) =
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
89. Picard’s Method
2nd
approximation:
put n = 1 and y1 = 1 + 3x + x2
in f(x, y)
y2 = 1 +
x
0
3 + 2x(1 + 3x + x2
) dx
= 1 +
x
0
3 + 2x + 6x2
+ 2x3
) dx
∴ y2 = 1 + 3x + x2
+ 2x3
+
x4
2
which is approximate solution, putting x = 0.1
y(0.1) = 1.31205
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
90. Picard’s Method
Ex:
Using Picard’s method, obtain a solution upto
4th
approx of the equation
dy
dx
= y + x, y(0) = 1.
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
91. Picard’s Method
Sol.:
By Picard’s method y = y0 +
x
x0
f(x, y) dx
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
92. Picard’s Method
Sol.:
By Picard’s method y = y0 +
x
x0
f(x, y) dx
Here x0 = 0, y0 = 1, f(x, y) = x + y
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
93. Picard’s Method
Sol.:
By Picard’s method y = y0 +
x
x0
f(x, y) dx
Here x0 = 0, y0 = 1, f(x, y) = x + y
1st
approximation: put y = y0 = 1 in f(x, y)
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
94. Picard’s Method
Sol.:
By Picard’s method y = y0 +
x
x0
f(x, y) dx
Here x0 = 0, y0 = 1, f(x, y) = x + y
1st
approximation: put y = y0 = 1 in f(x, y)
‘y1 = 1 +
x
0
(1 + x) dx
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
95. Picard’s Method
Sol.:
By Picard’s method y = y0 +
x
x0
f(x, y) dx
Here x0 = 0, y0 = 1, f(x, y) = x + y
1st
approximation: put y = y0 = 1 in f(x, y)
‘y1 = 1 +
x
0
(1 + x) dx
∴ y1 = 1 + x +
x2
2
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
105. Picard’s Method
4th
approximation:
put y = 1 + x + x2
+
x3
3
+
x4
24
in f(x, y)
‘y4 = 1 +
x
0
1 + 2x + x2
+
x3
3
+
x4
24
dx
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
106. Picard’s Method
4th
approximation:
put y = 1 + x + x2
+
x3
3
+
x4
24
in f(x, y)
‘y4 = 1 +
x
0
1 + 2x + x2
+
x3
3
+
x4
24
dx
∴ y4 = 1 + x + x2
+
x3
3
+
x4
12
+
x5
120
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
107. Picard’s Method
Ex:
Using Picard’s 2nd
approx. solution of the initial
value problem
dy
dx
= x2
+ y2
,for x = 0.4 correct to
4 decimal places given that y(0) = 0.
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
108. Picard’s Method
Sol.:
By Picard’s method y = y0 +
x
x0
f(x, y) dx
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
109. Picard’s Method
Sol.:
By Picard’s method y = y0 +
x
x0
f(x, y) dx
Here x0 = 0, y0 = 0, f(x, y) = x2
+ y2
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
110. Picard’s Method
Sol.:
By Picard’s method y = y0 +
x
x0
f(x, y) dx
Here x0 = 0, y0 = 0, f(x, y) = x2
+ y2
1st
approximation: put y = y0 = 0 in f(x, y)
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
111. Picard’s Method
Sol.:
By Picard’s method y = y0 +
x
x0
f(x, y) dx
Here x0 = 0, y0 = 0, f(x, y) = x2
+ y2
1st
approximation: put y = y0 = 0 in f(x, y)
‘y1 = 0 +
x
0
(x2
+ 0) dx
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
112. Picard’s Method
Sol.:
By Picard’s method y = y0 +
x
x0
f(x, y) dx
Here x0 = 0, y0 = 0, f(x, y) = x2
+ y2
1st
approximation: put y = y0 = 0 in f(x, y)
‘y1 = 0 +
x
0
(x2
+ 0) dx
∴ y1 =
x3
3
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
115. Picard’s Method
2nd
approximation:
put y = y1 =
x3
3
in f(x, y)
‘y2 = y0 +
x
0
x2
+
x3
3
2
dx
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
116. Picard’s Method
2nd
approximation:
put y = y1 =
x3
3
in f(x, y)
‘y2 = y0 +
x
0
x2
+
x3
3
2
dx
∴ y2 =
x3
3
+
x7
63
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
117. Picard’s Method
2nd
approximation:
put y = y1 =
x3
3
in f(x, y)
‘y2 = y0 +
x
0
x2
+
x3
3
2
dx
∴ y2 =
x3
3
+
x7
63
y(0.4) =
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
118. Picard’s Method
Ex:
Find the value of y for x = 0.1 by Picard’s
method given that
dy
dx
=
y − x
y + x
,y(0) = 1.
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
119. Picard’s Method
Sol.:
By Picard’s method y = y0 +
x
x0
f(x, y) dx
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
120. Picard’s Method
Sol.:
By Picard’s method y = y0 +
x
x0
f(x, y) dx
Here x0 = 0, y0 = 1, f(x, y) =
y − x
y + x
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
121. Picard’s Method
Sol.:
By Picard’s method y = y0 +
x
x0
f(x, y) dx
Here x0 = 0, y0 = 1, f(x, y) =
y − x
y + x
1st
approximation: put y = y0 = 1 in f(x, y)
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
122. Picard’s Method
Sol.:
By Picard’s method y = y0 +
x
x0
f(x, y) dx
Here x0 = 0, y0 = 1, f(x, y) =
y − x
y + x
1st
approximation: put y = y0 = 1 in f(x, y)
y1 = 1 +
x
0
1 − x
1 + x
dx = 1 +
x
0
2 − (1 + x)
1 + x
dx
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
123. Picard’s Method
Sol.:
By Picard’s method y = y0 +
x
x0
f(x, y) dx
Here x0 = 0, y0 = 1, f(x, y) =
y − x
y + x
1st
approximation: put y = y0 = 1 in f(x, y)
y1 = 1 +
x
0
1 − x
1 + x
dx = 1 +
x
0
2 − (1 + x)
1 + x
dx
= 1 +
x
0
2
1 + x
− 1 dx
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
124. Picard’s Method
Sol.:
By Picard’s method y = y0 +
x
x0
f(x, y) dx
Here x0 = 0, y0 = 1, f(x, y) =
y − x
y + x
1st
approximation: put y = y0 = 1 in f(x, y)
y1 = 1 +
x
0
1 − x
1 + x
dx = 1 +
x
0
2 − (1 + x)
1 + x
dx
= 1 +
x
0
2
1 + x
− 1 dx
∴ y1 = 1 − x + 2log(1 + x)
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
127. Picard’s Method
2nd
approximation:
put y = y1 = 1 + 2log(1 + x) − x in f(x, y)
y2 = 1 +
x
0
1 − x + 2log(1 + x) − x
1 − x + 2log(1 + x) + x
dx
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
128. Picard’s Method
2nd
approximation:
put y = y1 = 1 + 2log(1 + x) − x in f(x, y)
y2 = 1 +
x
0
1 − x + 2log(1 + x) − x
1 − x + 2log(1 + x) + x
dx
= 1 +
x
0
1 − 2x + 2log(1 + x)
1 + 2log(1 + x)
dx
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
129. Picard’s Method
2nd
approximation:
put y = y1 = 1 + 2log(1 + x) − x in f(x, y)
y2 = 1 +
x
0
1 − x + 2log(1 + x) − x
1 − x + 2log(1 + x) + x
dx
= 1 +
x
0
1 − 2x + 2log(1 + x)
1 + 2log(1 + x)
dx
= 1 +
x
0
1 −
2x
1 + 2log(1 + x)
dx
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
130. Picard’s Method
= 1 + x −
x
0
2x
1 + 2log(1 + x)
dx
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
131. Picard’s Method
= 1 + x −
x
0
2x
1 + 2log(1 + x)
dx
which is difficult to integrate therefore using 1st
approximation.
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -
132. Picard’s Method
= 1 + x −
x
0
2x
1 + 2log(1 + x)
dx
which is difficult to integrate therefore using 1st
approximation.
y(0.1) =
Dr. N. B. Vyas Numerical Methods Ordinary Differential Equations -