4 1 Antidervatives

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Transcript 4 1 Antidervatives

4-1: Antiderivatives
Objective:
1. To define and find
antiderivatives
Assignment:
β€’ P. 255-258: 5-7, 15-41
odd, 47, 49, 51, 60, 67,
75, 87-92
Warm Up 1
Find each derivative.
1
2
1. 𝑦 = π‘₯ 2 + 3π‘₯ + 1
1
2
2. 𝑦 = π‘₯ 2 + 3π‘₯ βˆ’ 1
Warm Up 2
Given 𝑦 β€² = π‘₯ + 3, what is 𝑦?
Objective 1
To define and find
antiderivatives
Differential Equations
A differential
equation in π‘₯ and
𝑦 is an equation
involving π‘₯, 𝑦, and
derivatives of 𝑦.
𝑦′ = π‘₯ + 3
𝑦 = 12π‘₯ 2 + 3π‘₯ + 1
Solving differential equations involves working
backwards from 𝑦′ to find 𝑦. This process is
called integration or antidifferentiation.
Antiderivative
𝑓(π‘₯) = π‘₯ + 3
Antiderivatives
A function 𝐹 is an antiderivative of 𝑓 on an
interval 𝐼 if 𝐹 β€² π‘₯ = 𝑓(π‘₯) for all π‘₯ in 𝐼.
𝐹 π‘₯ = 12π‘₯ 2 + 3π‘₯ βˆ’ 1
𝐹 π‘₯ = 12π‘₯ 2 + 3π‘₯
𝐹 π‘₯ = 12π‘₯ 2 + 3π‘₯ + 1
𝐹 π‘₯ = 12π‘₯ 2 + 3π‘₯ + 2
Antiderivatives
If 𝐹 is an antiderivative of 𝑓 on an interval 𝐼,
then 𝐺 is also an antiderivative of 𝑓 on 𝐼 iff
𝐺(π‘₯) = 𝐹(π‘₯) + 𝐢, for all π‘₯ in 𝐼, where 𝐢 is a
constant.
General
𝑓(π‘₯) = π‘₯ + 3
𝐹 π‘₯ = 12π‘₯ 2 + 3π‘₯ βˆ’ 1
𝐺 π‘₯ = 12π‘₯ 2 + 3π‘₯ + 𝐢
We denote the entire family of
antiderivatives of 𝑓 by adding a constant 𝐢.
antiderivative
of 𝑓
Antiderivatives
If 𝐹 is an antiderivative of 𝑓 on an interval 𝐼,
then 𝐺 is also an antiderivative of 𝑓 on 𝐼 iff
𝐺(π‘₯) = 𝐹(π‘₯) + 𝐢, for all π‘₯ in 𝐼, where 𝐢 is a
constant.
𝑓(π‘₯) = π‘₯ + 3
𝐹 π‘₯ = 12π‘₯ 2 + 3π‘₯ βˆ’ 1
𝐺 π‘₯ = 12π‘₯ 2 + 3π‘₯ + 𝐢
We denote the entire family of
antiderivatives of 𝑓 by adding a constant 𝐢.
General
solution to
the
differential
equation
𝐺′ π‘₯ = π‘₯ + 3
Antiderivatives
If 𝐹 is an antiderivative of 𝑓 on an interval 𝐼,
then 𝐺 is also an antiderivative of 𝑓 on 𝐼 iff
𝐺(π‘₯) = 𝐹(π‘₯) + 𝐢, for all π‘₯ in 𝐼, where 𝐢 is a
constant.
𝑓(π‘₯) = π‘₯ + 3
𝐹 π‘₯ = 12π‘₯ 2 + 3π‘₯ βˆ’ 1
𝐺 π‘₯ =
1 2
2π‘₯
+ 3π‘₯ + 𝐢
Constant of
Integration
Exercise 1
Find the general solution to the differential
equation 𝑦′ = 2.
Differentials
The differential equation
𝑑𝑦
𝑑π‘₯
= 𝑓(π‘₯) can be written as
Differential Form
𝑑𝑦 = 𝑓 π‘₯ 𝑑π‘₯
Differential
of 𝑦
Approximates
βˆ†π‘¦
Differential
of π‘₯
Approximates
βˆ†π‘₯
𝑑𝑦 is the amount of change in the
tangent line when π‘₯ changes by 𝑑π‘₯
βˆ†π‘¦ is the amount of change in
π’š = 𝒇(𝒙) when π‘₯ changes by βˆ†π‘₯
Indefinite Integration
To solve this differential equation, we apply the
process of antidifferentiation or indefinite
integration, which is denoted by ∫ .
𝑑𝑦 = 𝑓 π‘₯ 𝑑π‘₯
𝑦=
𝑓 π‘₯ 𝑑π‘₯ = 𝐹 π‘₯ + 𝐢
Read as β€œthe antiderivative of 𝑓 with respect to π‘₯”
Indefinite Integration
To solve this differential equation, we apply the
process of antidifferentiation or indefinite
integration, which is denoted by ∫ .
𝑑𝑦 = 𝑓 π‘₯ 𝑑π‘₯
𝑦=
𝑓 π‘₯ 𝑑π‘₯ = 𝐹 π‘₯ + 𝐢
Read as β€œthe integral of 𝑓 with respect to π‘₯”
Indefinite Integration
To solve this differential equation, we apply the
process of antidifferentiation or indefinite
integration, which is denoted by ∫ .
𝑑𝑦 = 𝑓 π‘₯ 𝑑π‘₯
𝑦=
𝑓 π‘₯ 𝑑π‘₯ = 𝐹 π‘₯ + 𝐢
Integral sign
Integrand
Variable of
Integration
Constant of
Integration
Inverse Relationship
Differentiation and Integration are inverse
operations.
𝐹 β€² π‘₯ 𝑑π‘₯ = 𝐹 π‘₯ + 𝐢
𝑑
𝑑π‘₯
𝑓 π‘₯ 𝑑π‘₯ = 𝑓(π‘₯)
These equations can be use to build integration
rules from differentiation rules
Integration Rules
Differentiation Formula
Integration Formula
𝑑
𝐢 =0
𝑑π‘₯
0 𝑑π‘₯ = 𝐢
𝑑
π‘˜π‘₯ = π‘˜
𝑑π‘₯
π‘˜ 𝑑π‘₯ = π‘˜π‘₯
𝑑
π‘˜π‘“(π‘₯) = π‘˜π‘“ β€² (π‘₯)
𝑑π‘₯
π‘˜π‘“(π‘₯) 𝑑π‘₯ = π‘˜
𝑓(π‘₯) 𝑑π‘₯
Integration Rules
Differentiation Formula
𝑑 𝑛
π‘₯ = 𝑛π‘₯ π‘›βˆ’1
𝑑π‘₯
Integration Formula
π‘₯ 𝑛 𝑑π‘₯ =
Exercise 2
Describe the antiderivatives of 3π‘₯.
Exercise 3
Integrate the following.
1.
1
∫ π‘₯ 3 𝑑π‘₯
2. ∫ π‘₯ 𝑑π‘₯
3. ∫ 2 sin π‘₯ 𝑑π‘₯
You can check your
answer to an
integration problem
by differentiating
Exercise 4
Integrate the following.
1. ∫ 𝑑π‘₯
2. ∫ π‘₯ + 2 𝑑π‘₯
3. ∫ 3π‘₯ 4 βˆ’ 5π‘₯ 2 + π‘₯ 𝑑π‘₯
Exercise 5
π‘₯+1
𝑑π‘₯
π‘₯
Exercise 6
sin π‘₯
𝑑π‘₯
2
cos π‘₯
A Particular Solution
Up to this point, we
have only been finding
the general solution to
a differential equation.
Given an initial
condition, however,
we can find a
particular solution.
Differential Equation
𝑓 β€² (π‘₯) = 3π‘₯ 2 βˆ’ 1
General Solution
𝐹 π‘₯ = π‘₯3 βˆ’ π‘₯ + 𝐢
Initial Condition
𝐹 2 =4
Particular Solution
𝐹 π‘₯ = π‘₯3 βˆ’ π‘₯ βˆ’ 2
Exercise 7
β€²
1
,
π‘₯3
Find the general solution of 𝑓 π‘₯ =
π‘₯ > 0, and
find the particular solution that satisfies the initial
condition 𝐹(1) = 0.
Exercise 8
A ball is thrown upward with an initial velocity of 64
feet per second from an initial height of 80 feet.
Find the position function giving the height 𝑠 as a
function of the time 𝑑. When does the ball hit the
ground?
4-1: Antiderivatives
Objective:
1. To define and find
antiderivatives
Assignment:
β€’ P. 255-258: 5-7, 15-41
odd, 47, 49, 51, 60, 67,
75, 87-92