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DifferentiationIntegrationDifferential EquationsMaclaurin
Paper 3
Plus
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Perplex
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Integration
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Techniques of Integration
Kinematics
Techniques of Integration
Integration

Techniques of Integration

0 of 0 exercises completed

Techniques for evaluating integrals, including substitution for ​f(ax+b)​ and compositions, handling definite integrals with changed bounds, partial fractions, integration by parts, repeated parts, and cyclical parts.

Want a deeper conceptual understanding? Try our interactive lesson! (Plus Only)

Integrating f(ax+b)
SL 5.10

If ​F(x)=∫f(x)dx, then

​
∫f(ax+b)dx=a1​F(ax+b)🚫
​
Integration by substitution
SL 5.10

Integrating a composition of functions ​f(g(x))​ requires us to divide by ​g′(x), so it is easier to find the anti-derivative of anything of the form ​g′(x)f′(g(x))​ by first dividing by ​g′(x).


In symbols, we use the known fact

​
∫kg′(x)f′(g(x))dx=kf(g(x))+C🚫
​

and let ​u=g(x), giving us

​
∫kg′(x)f′(g(x))dx=k∫f′(u)du,🚫
​

an integral we can solve more easily:

​
k∫f′(u)du=kf(u)+C.
​


Then, we substitute ​g(x)​ back in to get our desired result of ​kf(g(x))+C.

Substitution and Integral Bounds
SL 5.10

When we make a substitution in a definite integral in the form

​
∫ab​kg′(x)f′(g(x))dx
​

we need to remember that the bounds are from ​x=a​ to ​x=b:

​
∫ab​kg′(x)f′(g(x))dx  ​=k∫x=ax=b​f′(u)du =[kf(u)]x=ax=b​​
​


We then have two choices:

  1. Plug ​x=a​ and ​x=b​ into ​u​ to find the bounds in terms of ​u.

  2. Plug ​u(x)​ back in and use the bounds ​a→b.

Integration by partial fractions
AHL 5.15

Consider the integral

​
∫(x−c)(x−d)ax+b​dx,
​

we can break the fraction into two parts:

​
(x−c)(x−d)ax+b​=x−cA​+x−dB​
​


Then, find ​A​ and ​B​ using a system of equations. Finally, integrate the two fractions.

Recall the product rule: ​(uv)′=u′v+uv′. Then, integrating both sides with respect to ​x​ yields

​
∫(uv)′dx=∫u′vdx+∫uv′dx,
​

but the integral of a derivative simply returns the original function, so we have

​
uv=∫u′vdx+∫uv′dx.
​

Replacing ​u′​ and ​v′​ with ​dxdu​​ and ​dxdv​​ respectively and rearranging terms gives us the result

​
∫udxdv​dx=uv−∫vdxdu​dx,
​

which we use to perform integration by parts.

Integration by parts
AHL 5.16

To perform integration by parts, we use

​
∫udxdv​dx=uv−∫vdxdu​dx📖
​


Another common way of writing this is

​
∫udv=uv−∫vdu📖
​


The first step is choosing what to make ​u​ and what to make ​dv. Since we will take the derivative of ​u, and integrate ​dv, we generally pick ​dv​ that is easy to integrate, and a ​u​ that gets simpler when we differentiate it.


Example: ​∫xexdx​

We choose ​u=x​ and ​dv=ex, because ​ex​ is easy to integrate, and the derivative of ​x​ is just ​1, which is simpler:

​
u=x,dv=ex⇒uv=xex,vdu=ex
​
​
∫xexdx=xex−∫exdx=xex−ex+C
​
Repeated integration by parts
AHL 5.16

Certain functions, like powers of ​x, will simplify after repeated differentiation.


Therefore, we may perform repeated integration by parts using such functions as our ​u​ knowing that they will eventually yield a simple ​∫vdu.

Example: ​I=∫x2e2xdx​

We let ​u=x2​ and ​v′=e2x​ because ​x2​ gets simpler when differentiated, and we know how tom integrate ​e2x:

​
u′=2x,v=21​e2x
​

So

​
I=x2⋅21​e2x−J∫2x⋅21​e2xdx​​
​

Now we have

​
J=∫xe2xdx,letu=x,v′=e2x
​
​
u′=1,v=21​e2x
​
​
∴J=x⋅21​e2x−∫1⋅21​e2xdx=21​e2x(x−21​)
​

So

​
I=21​e2x⋅(x2−x+21​)+C
​
Cyclical integration by parts
AHL 5.16

Cyclical integration by parts are the result of a product of two functions that do not reduce via differentiation. Instead, they "cycle," or eventually return the original integral as the ​∫vdu​ term.


In such cases, integrate by parts until you cycle back to the original integral ​I. Then, you may solve for ​I​ algebraically.


Example: ​I=∫cos(2x)exdx​

Let ​u=cos(2x)​ and ​v′=ex, then

​
u′=−2sin2x,v=ex
​

So

​
I=cos(2x)ex−J∫(−2sin2x)exdx​​(1)
​

This new integral ​J​ can be split by parts, so let ​u=−2sin2x​ and ​v′=ex, then

​
u′=−4cos2x,v=ex
​

So

​
J=∫(−2sin2x)exdx=−2sin(2x)ex−∫(−4cos2x)exdx
​

But this last integral is a multiple of the original ​I, specifically ​−4I:

​
J=−2sin(2x)ex−(−4I)(2)
​

From equation ​(1)​ we have

​
I=cos(2x)ex−J
​

Substituting in ​(2)​ we find

​
I=cos(2x)ex+2sin(2x)ex+(−4I)
​

So

​
5I=ex(cos2x+2sin2x)⇒I=51​ex(cos2x+2sin2x)+C
​

Nice work completing Techniques of Integration, here's a quick recap of what we covered:

Skills covered

Mixed Practice

Exercises checked off

I'm Plex, here to help you understand this concept!
/
Integration
/
Techniques of Integration
Kinematics
Techniques of Integration
Integration

Techniques of Integration

0 of 0 exercises completed

Techniques for evaluating integrals, including substitution for ​f(ax+b)​ and compositions, handling definite integrals with changed bounds, partial fractions, integration by parts, repeated parts, and cyclical parts.

Want a deeper conceptual understanding? Try our interactive lesson! (Plus Only)

Integrating f(ax+b)
SL 5.10

If ​F(x)=∫f(x)dx, then

​
∫f(ax+b)dx=a1​F(ax+b)🚫
​
Integration by substitution
SL 5.10

Integrating a composition of functions ​f(g(x))​ requires us to divide by ​g′(x), so it is easier to find the anti-derivative of anything of the form ​g′(x)f′(g(x))​ by first dividing by ​g′(x).


In symbols, we use the known fact

​
∫kg′(x)f′(g(x))dx=kf(g(x))+C🚫
​

and let ​u=g(x), giving us

​
∫kg′(x)f′(g(x))dx=k∫f′(u)du,🚫
​

an integral we can solve more easily:

​
k∫f′(u)du=kf(u)+C.
​


Then, we substitute ​g(x)​ back in to get our desired result of ​kf(g(x))+C.

Substitution and Integral Bounds
SL 5.10

When we make a substitution in a definite integral in the form

​
∫ab​kg′(x)f′(g(x))dx
​

we need to remember that the bounds are from ​x=a​ to ​x=b:

​
∫ab​kg′(x)f′(g(x))dx  ​=k∫x=ax=b​f′(u)du =[kf(u)]x=ax=b​​
​


We then have two choices:

  1. Plug ​x=a​ and ​x=b​ into ​u​ to find the bounds in terms of ​u.

  2. Plug ​u(x)​ back in and use the bounds ​a→b.

Integration by partial fractions
AHL 5.15

Consider the integral

​
∫(x−c)(x−d)ax+b​dx,
​

we can break the fraction into two parts:

​
(x−c)(x−d)ax+b​=x−cA​+x−dB​
​


Then, find ​A​ and ​B​ using a system of equations. Finally, integrate the two fractions.

Recall the product rule: ​(uv)′=u′v+uv′. Then, integrating both sides with respect to ​x​ yields

​
∫(uv)′dx=∫u′vdx+∫uv′dx,
​

but the integral of a derivative simply returns the original function, so we have

​
uv=∫u′vdx+∫uv′dx.
​

Replacing ​u′​ and ​v′​ with ​dxdu​​ and ​dxdv​​ respectively and rearranging terms gives us the result

​
∫udxdv​dx=uv−∫vdxdu​dx,
​

which we use to perform integration by parts.

Integration by parts
AHL 5.16

To perform integration by parts, we use

​
∫udxdv​dx=uv−∫vdxdu​dx📖
​


Another common way of writing this is

​
∫udv=uv−∫vdu📖
​


The first step is choosing what to make ​u​ and what to make ​dv. Since we will take the derivative of ​u, and integrate ​dv, we generally pick ​dv​ that is easy to integrate, and a ​u​ that gets simpler when we differentiate it.


Example: ​∫xexdx​

We choose ​u=x​ and ​dv=ex, because ​ex​ is easy to integrate, and the derivative of ​x​ is just ​1, which is simpler:

​
u=x,dv=ex⇒uv=xex,vdu=ex
​
​
∫xexdx=xex−∫exdx=xex−ex+C
​
Repeated integration by parts
AHL 5.16

Certain functions, like powers of ​x, will simplify after repeated differentiation.


Therefore, we may perform repeated integration by parts using such functions as our ​u​ knowing that they will eventually yield a simple ​∫vdu.

Example: ​I=∫x2e2xdx​

We let ​u=x2​ and ​v′=e2x​ because ​x2​ gets simpler when differentiated, and we know how tom integrate ​e2x:

​
u′=2x,v=21​e2x
​

So

​
I=x2⋅21​e2x−J∫2x⋅21​e2xdx​​
​

Now we have

​
J=∫xe2xdx,letu=x,v′=e2x
​
​
u′=1,v=21​e2x
​
​
∴J=x⋅21​e2x−∫1⋅21​e2xdx=21​e2x(x−21​)
​

So

​
I=21​e2x⋅(x2−x+21​)+C
​
Cyclical integration by parts
AHL 5.16

Cyclical integration by parts are the result of a product of two functions that do not reduce via differentiation. Instead, they "cycle," or eventually return the original integral as the ​∫vdu​ term.


In such cases, integrate by parts until you cycle back to the original integral ​I. Then, you may solve for ​I​ algebraically.


Example: ​I=∫cos(2x)exdx​

Let ​u=cos(2x)​ and ​v′=ex, then

​
u′=−2sin2x,v=ex
​

So

​
I=cos(2x)ex−J∫(−2sin2x)exdx​​(1)
​

This new integral ​J​ can be split by parts, so let ​u=−2sin2x​ and ​v′=ex, then

​
u′=−4cos2x,v=ex
​

So

​
J=∫(−2sin2x)exdx=−2sin(2x)ex−∫(−4cos2x)exdx
​

But this last integral is a multiple of the original ​I, specifically ​−4I:

​
J=−2sin(2x)ex−(−4I)(2)
​

From equation ​(1)​ we have

​
I=cos(2x)ex−J
​

Substituting in ​(2)​ we find

​
I=cos(2x)ex+2sin(2x)ex+(−4I)
​

So

​
5I=ex(cos2x+2sin2x)⇒I=51​ex(cos2x+2sin2x)+C
​

Nice work completing Techniques of Integration, here's a quick recap of what we covered:

Skills covered

Mixed Practice

Exercises checked off

I'm Plex, here to help you understand this concept!

Generating starter questions...

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