DIFFERENTIAL EQUATIONS Note: Differential equations are equations containing a derivative. They can be solved by integration to obtain a general solution.

Slides:



Advertisements
Similar presentations
Differential Equations
Advertisements

Indefinite Integrals 6.1. Integration - Antidifferentiation - method of solution to a differential equation INdefinite Integral Integration Symbol Variable.
The Chain Rule Section 3.6c.
The Derivative. Objectives Students will be able to Use the “Newton’s Quotient and limits” process to calculate the derivative of a function. Determine.
Warm-up Problems Solve the IVP . Give the largest interval over which the solution is defined.
4.1 Antiderivatives and Indefinite Integrals Defn. A function F(x) is an antiderivative of f(x) on an interval I if F '(x)=f(x) for all x in I. ex. Find.
Basic Models in Theoretical Neuroscience Oren Shriki 2010 Differential Equations.
Find the exponential function whose graph passes through the two points. Initial value: Equation: Other point: Function:
3.3 –Differentiation Rules REVIEW: Use the Limit Definition to find the derivative of the given function.
Section 1.1 Differential Equations & Mathematical Models
The Mathematics of Star Trek Lecture 3: Equations of Motion and Escape Velocity.
Kinetic energy Derivation of kinetic energy. Kinetic Energy 2 starting equations F = m x a (Newton’s 2 nd law) W = Force x distance.
Calculus in Physics II x 0 = 0 x axis Knowing the car’s displacement history, find its velocity and acceleration. 1.
Using the Derivative AP Physics C Mrs. Coyle
Section 6.1 Polynomial Derivatives, Product Rule, Quotient Rule.
Mathematics. Session Differential Equations - 2 Session Objectives  Method of Solution: Separation of Variables  Differential Equation of first Order.
Slope Fields. Quiz 1) Find the average value of the velocity function on the given interval: [ 3, 6 ] 2) Find the derivative of 3) 4) 5)
4.1 The Indefinite Integral. Antiderivative An antiderivative of a function f is a function F such that Ex.An antiderivative of since is.
Derivation of the proportionality of velocity and radius for an object in circular motion under a constant centripetal force.
3.1 Definition of the Derivative & Graphing the Derivative
Modeling motion subject to drag forces PHYS 361 Spring, 2011.
Chapter 21 Exact Differential Equation Chapter 2 Exact Differential Equation.
Motion in One Dimension
Dr. Omar Al Jadaan Assistant Professor – Computer Science & Mathematics General Education Department Mathematics.
Differential Equations
4001 ANTIDERIVATIVES AND INDEFINITE INTEGRATION
Exponential Growth and Decay 6.4. Separation of Variables When we have a first order differential equation which is implicitly defined, we can try to.
4.1 Antiderivatives and Indefinite Integration Definition of Antiderivative: A function F is called an antiderivative of the function f if for every x.
Particle Motion: Total Distance, Speeding Up and Slowing Down THOMAS DUNCAN.
ANTIDERIVATIVES AND INDEFINITE INTEGRATION AB Calculus.
Example 1 Find the derivative of Function is written in terms of f(x), answer should be written in terms of f ′ (x) Continue 
Separable Differential Equations
Ch 8 : Conservation of Linear Momentum 1.Linear momentum and conservation 2.Kinetic Energy 3.Collision 1 dim inelastic and elastic nut for 2 dim only inellastic.
Solving equations with polynomials – part 2. n² -7n -30 = 0 ( )( )n n 1 · 30 2 · 15 3 · 10 5 · n + 3 = 0 n – 10 = n = -3n = 10 =
Lesson 4-10b Anti-Differentiation. Quiz Estimate the area under the graph of f(x) = x² + 1 from x = -1 to x = 2 …. Improve your estimate by using six.
Logarithmic Differentiation
 y’ = 3x and y’ = x are examples of differential equations  Differential Form dy = f(x) dx.
2.3 Rate of Change (Calc I Review). Average Velocity Suppose s(t) is the position of an object at time t, where a ≤ t ≤ b. The average velocity, or average.
Particular Solutions to Differential Equations Unit 4 Day 2.
9.1 Solving Differential Equations Mon Jan 04 Do Now Find the original function if F’(x) = 3x + 1 and f(0) = 2.
Blue part is out of 50 Green part is out of 50  Total of 100 points possible.
Chapter 21 Exact Differential Equation Chapter 2 Exact Differential Equation.
3.5 – Implicit Differentiation
4033-Properties of the Definite Integral (5.3) AB Calculus.
NEWTON’S 2 ND LAW OF MOTION By: Per.7. WHAT IS IT? Newton's second law Of Motion Newton's second law Of Motion can be formally stated as follows: The.
2.1 Introduction to DE 2.2 Concept of Solution 2.3Separation of Variable 2.4 Homogeneous Eq 2.5 Linear Eq 2.6 Exact Eq 2.7 Application of 1 st.
Scientific Principles Related to a Sidewinder By: Mr. Toole.
Chapter 4 Integration 4.1 Antidifferentiation and Indefinate Integrals.
Section 9.4 – Solving Differential Equations Symbolically Separation of Variables.
Introduction to Integrals Unit 4 Day 1. Do Now  Write a function for which dy / dx = 2 x.  Can you think of more than one?
Calculations Practice Sheet
DIFFERENTIAL EQUATIONS
Differential Equations
3.1 – Derivative of a Function
3.1 – Derivative of a Function
MTH1170 Differential Equations
Fundamental Concepts of Integral Calculus
Unit 6 – Fundamentals of Calculus Section 6
Differential Equations
Section Euler’s Method
Chapter 2 Objectives Describe motion in terms of changing velocity.
Section Indefinite Integrals
Prep Book Chapter 5 – Definition of the Derivative
Differential Equations
By Jordyn Kohl, Soumya Kamath, and Peter Ballentine
Total Distance Traveled
Differentials; Exact Equations
EXERCISE SET 7 – Differential Equations
Section 9.4 – Solving Differential Equations Symbolically
Section Indefinite Integrals
Presentation transcript:

DIFFERENTIAL EQUATIONS Note: Differential equations are equations containing a derivative. They can be solved by integration to obtain a general solution with +C. To obtain a specific solution requires additional information. Ex1 dy / dx + 7 = 2x dffntl eqtn dy / dx = 2x - 7 y =  (2x – 7) dx y = x 2 – 7x + C General Soln Integrate with respect to x

Ex2 Given that dy / dx = x x 2 and y = f(x) passes through (-2,2) then find the exact solution to this differential equation. ********* dy / dx = x x 2 = x x 2 x 2 = 1 + 4x -2 So y =  (1 + 4x -2 ) dx y = x + 4x -1 + C -1 y = x – 4 + C x At (-2,2) this becomes 2 = -2 – (-2) + C ie C = 2 Solution is y = x – x

Ex3 (from Physics) Newton’s 1 st law of motion states that v = u + at v – final velocity, u - initial velocity, a – acceleration, t- time In Physics the symbol for distance is s Velocity is basically speed Given thatspeed = difference in distance difference in time We now have v = ds / dt ctd

So v = u + at becomes ds / dt = u + at Integrate with respect to t givings =  (u + at) dt ors = ut + 1 / 2 at 2 + C Assuming that s, u, t, a are all zero simultaneously gives C = 0 and we now get s = ut + 1 / 2 at 2 which is Newton’s 2 nd law of motion.