Formula Sheet
Trigonometric Identities/Definitions
ππππ π + ππππ π = π
πππ ππ = π πππ π πππ π
πππ ππ = ππππ π − ππππ π = πππππ π − π
πππ π
πππ π
π
πππ π =
πππ π
π
πππ π
=
πππ π πππ π
π
πππ π =
πππ π
πππ π =
πππ π =
π + ππππ π = ππππ π
π + ππππ π = ππππ π
Elementary Derivatives/Differentiation Rules
π
[πππ ππππππππ] = π
π
π
π
π
[π ] = πππ−π
π
π
π
π
[√π] =
π
π
π√ π
π
[πππ π] = πππ π
π
π
π
[πππ π] = −πππ π
π
π
π
[πππ π] = ππππ π
π
π
π
[πππ π] = −ππππ π
π
π
π
[πππ π] = πππ π πππ π
π
π
π
[πππ π] = −πππ π πππ π
π
π
π
π
[ππ π] =
π
π
π
π
[πππ π] = ππ π + π
π
π
π
π
[π ] = ππ
π
π
Product Rule:(ππ)′ = π′ π + π′π
π ′
Quotient Rule:(π) =
π′ π−π′ π
ππ
Chain Rule:[π(π)]′ = π′ (π)π′
Inverse Rule:
[π−π (π)]′ =
π
π′ [π−π (π)]
For any real numberπ,
π(π)
[∫
′
π(π)π
π] = π[π(π)]π′ (π)
π
Elementary Integrals
ππ+π
∫ π π
π =
+ πͺ ππ π ≠ −π
π+π
π
∫
π
π
π = ππ|π| + πͺ
π
∫ πππ ππ π
π = −(πππ ππ)/π + πͺ
∫ πππ ππ π
π = (πππ ππ)/π + πͺ
∫ πππ π π
π = −ππ|πππ π| + πͺ = ππ|πππ π| + πͺ
∫ ππ π
π = ππ + πͺ
∫ πππ π π
π = ππ|πππ π + πππ π| + πͺ
General Exponential and Logarithms of Base a
ππ β ππππ π
ππππ π β
ππ π
ππ π
π
π
[π ] = ππ ππ π
π
π
π
π
[ππππ π] =
π
π
π ππ π
∫ ππ π
π =
∫
ππ
+πͺ
ππ π
π
π
π = ππππ |π| + πͺ
π ππ π
Inverse Trigonometric Functions
Function
Domain
π¬π’π§−π π
[−π, π]
ππ¨π¬ −π π
[−π, π]
Range
π
π
[− , ]
π π
[π, π
]
π
π
[−∞, ∞]
(− , )
πππ−π π
π π
π
π¬ππ −π π = ππ¨π¬ −π ( )
π
Definition
π = π¬π’π§−π π
means
π¬π’π§ π = π
π = ππ¨π¬ −π π
means
ππ¨π¬ π = π
π = πππ§−π π
means
πππ§ π = π
π
ππ¬π −π π = π¬π’π§−π ( )
π
π
ππ¨π −π π = πππ§−π ( )
π
Derivatives of Inverse Trigonometric Functions
Trig. Function
--- negate --->
π
π
[π¬π’π§−π π] =
π
π
√π − ππ
π
π
[πππ§−π π] =
π
π
π + ππ
π
π
[π¬ππ −π π] =
π
π
|π|√ππ − π
Co-Trig Function
π
π
[ππ¨π¬ −π π] = −
π
π
√π − ππ
π
π
[ππ¨π −π π] = −
π
π
π + ππ
π
π
[ππ¬π −π π] = −
π
π
|π|√ππ − π
Integrals Evaluated with Inverse Trigonometric Functions
∫
π
π
π
π = π¬π’π§−π ( ) + πͺ
π
√ππ − ππ
π
π
πππ§−π ( ) + πͺ
π
π
π
π
π
∫
π
π = π¬ππ −π | | + πͺ
π
π
π√ππ − ππ
∫
π
ππ + ππ
π
π =
Hyperbolic Functions
Name
Hyperbolic Sine
Hyperbolic Cosine
Definition
ππ − π−π
π¬π’π§π‘ π =
π
π
π + π−π
ππ¨π¬π‘ π =
π
Derivative
Integral
π
[ππππ π] = ππ¨π¬π‘ π
π
π
π
[ππππ π] = π¬π’π§π‘ π
π
π
∫ π¬π’π§π‘ π π
π = ππ¨π¬π‘ π + πͺ
∫ ππ¨π¬π‘ π π
π = π¬π’π§π‘ π + πͺ
Integration by Parts
π
∫ π π
π = ππ − ∫ π π
π
π
∫ π π
π = [ππ]ππ − ∫ π π
π
π
π
Priority for choosing π is:
Logarithmic, Inverse Trigonometric, Algebraic/Polynomial, Trigonometric, Exponential
Integration of Trigonometric Functions
∫ π¬π’π§π π ππ¨π¬π π π
π
∫ π¬π’π§π π ππ¨π¬π π π
π
If any of π and π is odd, then write it as (2 x something + 1)
and replace
π¬π’π§π π = π − ππ¨π¬π πor ππ¨π¬π π = π − ππππ π
and substitute π = ππ¨π¬ πorπ = π¬π’π§ π, respectively.
If both of π and π is even, then replace
π+ππ¨π¬ ππ
π−ππ¨π¬ ππ
ππ¨π¬π π =
and/or π¬π’π§π π =
π
π
until an odd power appears, and so use the method above.
π
Integrals involving square roots
π
Replaceπ + ππ¨π¬ ππ = π ππ¨π¬π π πorπ − ππ¨π¬ ππ = π π¬π’π§π π π
Use ππππ π + ππππ π = π
Rationalize: Multiply with the conjugate
π
∫[πππ(π − π)π − πππ(π + π)π]π
π
π
π
∫ πππ ππ πππ ππ π
π = ∫[πππ(π − π)π + πππ(π + π)π] π
π
π
π
∫ πππ ππ πππ ππ π
π = ∫[πππ(π − π)π + πππ(π + π)π] π
π
π
Write the expression inside the integral as a product of
ππππ π and ππππ π
π
Then replace πππ π = ππππ π − π or ππππ π = ππππ π + π
Finally, integrate by parts: Let π
π = ππππ π π
π or πππ π πππ π π
π,
or integrate by substitution: Let π
π = ππππ π π
π orπ ππ π πππ π π
π
π
π
∫ ππππ π π
π = πππ π ππππ + ππ|πππ π + ππππ| + πͺ
π
π
π
π π
∫ ππππ π π
π = (π + πππ π πππ )π + πͺ = + πππ ππ + πͺ
π
π π
π
π
π
∫ ππππ π π
π = (π − πππ π πππ )π + πͺ = − πππ ππ + πͺ
π
π π
∫ πππ ππ πππ ππ π
π =
Integrals involving
products of sines and cosines
Integrals involving
products and powers of
secants and tangents
Very useful integrals
Integration with Trigonometric Substitution
If the integral contains
√ππ − ππ
Substitute
π = π πππ π½
√ππ + ππ
√ππ − ππ
π = π πππ π½
π = π πππ π½
Integration of Rational Functions with Partial Fractions
π·(π)
Consider ∫ πΈ(π) π
π where P(x) and Q(x) are polynomials.
1) If deg P(x) < deg Q(x) and
if
then use the decomposition
π·(π)
π¨π
π¨π
π¨π
=
+
+ β―+
πΈ(π) π − ππ π − ππ
π − ππ
and the Heaviside Cover-up Method to find π¨π , π¨π , … , π¨π
π·(π)
π¨π
π¨π
π¨π
=
+
+ β―+
π
(π − π)π
πΈ(π) π − π (π − π)
πΈ(π) = (π − ππ )(π − ππ ) … (π − ππ )
are distinct linear factors
πΈ(π) = (π − π)π
are repeated linear factors
πΈ(π) = (πππ + ππ + π)π
are repeated irreducible
quadratic factors
πΈ(π) = product of linear and irreducible
quadratic factors
π·(π)
π¨π π + π©π
π¨π π + π©π
π¨π π + π©π
= π
+
+ β―+
π
π
(πππ + ππ + π)π
πΈ(π) ππ + ππ + π (ππ + ππ + π)
π·(π)
πΈ(π)
= sum of decompositions from corresponding cases
2) If deg P(x) ≥ deg Q(x), then use long division to write
π·(π)
πΉ(π)
= πΊ(π) +
πΈ(π)
πΈ(π)
where deg R(x) < deg Q(x). Integrate S(x) normally and use part one above for R(x)/Q(.
The Heaviside Cover-up Method: A quick method for finding the coefficients π¨π , π¨π , … , π¨π in
π·(π)
π¨π
π¨π
π¨π
=
+
+β―+
(π − ππ )(π − ππ ) … (π − ππ ) π − ππ π − ππ
π − ππ
To find π¨π :
1) Cover the factor π − ππ on the left-hand-side of the equation above
2) Evaluate the left-hand-side for π = ππ
That is,
π¨π =
π·(ππ )
(π − ππ ) … (π − ππ−π )(π − ππ+π ) … (π − ππ )
Improper Integrals
∞
If π(π) is continuous on [π, ∞), then
π
∫ π(π)π
π βΆ= π₯π’π¦ ∫ π(π)π
π
π→∞ π
π
π
Type I
If π(π) is continuous on(−∞, π], then
π
∫ π(π)π
π βΆ= π₯π’π¦ ∫ π(π)π
π
π→−∞ π
−∞
∞
If π(π) is continuous on (−∞, ∞), then
π
∞
∫ π(π)π
π βΆ= ∫ π(π)π
π + ∫ π(π)π
π
−∞
−∞
π
π
If π(π) is continuous on [π, π), then
∫ π(π)π
π βΆ= π₯π’π¦− ∫ π(π)π
π
π
π
Type II
If π(π) is continuous on (π, π], then
π
π→π
π
π
∫ π(π)π
π βΆ= π₯π’π¦+ ∫ π(π)π
π
π
π→π
π
π
If π(π) is continuous on [π, π) ∪ (π, π], then
π
π
∫ π(π)π
π βΆ= ∫ π(π)π
π + ∫ π(π)π
π
π
π
π
Integral Convergence Tests
The p-Integral Test on
∞
π
∫ π π
π
π π
where π is any positive real number
The Direct Comparison Test (DCT):
If π(π) and π(π) are continuous on
[π, ∞) such that
π ≤ π(π) ≤ π(π)
then
∞
Converges if π > 1, and
Diverges ifπ ≤ π
∞
∞
∞
If ∫π π(π)π
π diverges, then ∫π π(π)π
π diverges
(Smaller one diverges => larger one diverges)
∞
π ≤ ∫ π(π)π
π ≤ ∫ π(π)π
π
π
∞
If ∫π π(π)π
π converges, then ∫π π(π)π
π converges
(Larger one converges => smaller one converges)
π
π
→DCT Tricks
Compare withππ by removing constants from the numerator or
denominator, or using the following inequalities:
πππ(π) ≤ π, πππ(π) ≤ π, ππ(π) ≤ π, ππ(π) ≤ √π
The Limit Comparison Test (LCT):
If π(π) and π(π) are continuous on
[π, ∞) such that
π(π)
π₯π’π¦
π→∞ π(π)
is a positive real number, then
→LCT Tricks
∞
∞
∫π π(π)π
π and ∫π π(π)π
π
both converge or both diverge
(both integrals behave likewise)
π(π)
If π(π) = π
(π), then compare with
π»πππ ππππ πππππππ ππππππ ππ π(π)
π(π) =
π»πππ ππππ πππππππ ππππππ ππ π
(π)
π
Order of growths:π−π^π , π−ππ , π−π , π−π , π−π , π−π , π−π/π , ππ(π) , π, ππ(π), √π, π, ππ , ππ , ππ , πππ , ππ
π
slower <------------------------------------grows----------------------------------------->faster
Sequences
ππ π
=π
π→∞ π
π₯π’π¦
π
π₯π’π¦ √π = π
π→∞
ππ
= π (πππ π)
π→∞ π!
π
π₯π’π¦ √π = π (π > 0)
π→∞
π π
π₯π’π¦ (π + ) = ππ
π→∞
π
π!
=π
π→∞ ππ
π₯π’π¦
π₯π’π¦
π₯π’π¦ ππ = π (|π| < 1)
π₯π’π¦ ππ = ∞ (π > 1)
π→∞
π→∞
Infinite Series
ππ , ππ , ππ , ππ , …
∞
∞
∑ ππ = π₯π’π¦ ∑ ππ = π₯π’π¦ πΊπ΅
∑ ππ = ππ + ππ + ππ + β―
π=π
Sequence
Infinite series
π=π
π΅
π΅→∞
π=π
π΅→∞
(used to evaluate a Telescoping series)
π΅
Partial Sums
πΊπ΅ = ππ + ππ + ππ + β― + ππ΅ = ∑ ππ
π=π
π
∞
∑ ππ
Geometric Series
π−π
π
Converges to π−π if |π| < 1
π
= π + ππ + ππ + ππ + β―
Diverges if |π| ≥ π
π=π
Types of Series Convergence
∞
∑∞
π=π ππ Converges Absolutely means that ∑π=π|ππ | converges.
∞
∞
∑∞
π=π ππ Converges Conditionally means that ∑π=π|ππ | diverges but ∑π=π ππ converges.
Convergence/Divergence Tests on ∑∞
π=π ππ
Test
Description
Usage
Nth-term
If π₯π’π¦ ππ ≠ π, then the series diverges
Integral
∑∞
π=π ππ converges ↔ ∫π ππ π
π converges
provided that ππ is continuous, positive and decreasing on [π, ∞)
p-Series
∑∞
π=π π converges if π > 1, and diverges if π ≤ π, provided π ≥ π.
π→∞
∞
Direct
Comparison
(DCT)
Limit
Comparison
(LCT)
π
Only to prove
divergence
It can evaluate the
improper integral
With DCT and LCT
π
If you can bound it
∞
∞
Given ∑∞
π=π π
π ≤ ∑π=π ππ ≤ ∑π=π ππ such that ππ , ππ , π
π ≥ π after some
above/below with
index π, then:
as series that
∞
(i) If ∑∞
π=π ππ converges, then ∑π=π ππ converges
converges/diverge
∞
(ii) If ∑∞
π=π π
π diverges, then ∑π=π ππ diverges
s, respectively
Suppose that ππ , ππ > 0 after some index π, then:
If ππ is a division of
ππ
two functions of n
(i) If π₯π’π¦ π ∈ (0, ∞),
π→∞ π
∞
then ∑∞
π=π ππ and ∑π=π ππ both converge or both diverge
π
∞
(ii) If π₯π’π¦ ππ = π and ∑∞
π=π ππ converges, then ∑π=π ππ converges
π→∞ π
ππ
∞
(iii) If π₯π’π¦ π = ∞ and ∑∞
π=π ππ diverges, then ∑π=π ππ diverges
π→∞ π
π
Ratio
ππ¨π§π―ππ«π ππ¬ π’π π₯π’π¦ ππ+π < 1
π→∞
π
∞
The series ∑π=π ππ , with ππ > 0 {
ππ+π
ππ’π―ππ«π ππ¬ π’π π₯π’π¦ π > 1
π→∞
Root
The series ∑∞
π=π ππ , with ππ ≥ π {
π
ππ¨π§π―ππ«π ππ¬ π’π π₯π’π¦ π√ππ < 1
π→∞
ππ’π―ππ«π ππ¬ π’π π₯π’π¦ π√ππ > 1
π→∞
Alternating
Series (AST)
π
The series ∑∞
π=π(−π) ππ converges if all three conditions below are
satisfied:
(i) All ππ ’s are positive
(ii) The sequence {ππ } is non-increasing after some index
(iii) π₯π’π¦ ππ = π
π→∞
If ππ is a product
of terms like
factorials and
powers
If ππ is an nth
power of some
terms, but not
necessarily all
Only to prove
convergence when
the sign changes
from every term to
the next
If it is easier to
show absolute
convergence
Absolute
Absolute Convergence implies Convergence:
Convergence
∞
If ∑∞
π=π|ππ | Converges, then ∑π=π ππ Converges
(ACT)
π
To find the Interval of Convergence (IOC) of a Power Series ∑∞
π=π ππ (π − π) :
(i)
(ii)
Letππ = ππ (π − π)π , so that |ππ | = |ππ ||π − π|π
Use the Ratio or Root test to find an open interval (π, π) on which the power series converges
|π
|
π
absolutely by forcing π₯π’π¦ |ππ+π| < 1or π₯π’π¦ √|ππ | < 1.
π→∞
(iii)
(iv)
π
π→∞
Now check if the power series converges (conditionally) or diverges at the endpoints π = π, π.
Finally, IOC= interval containing all x values on which the power series converges.
Taylor & MacLaurin Series:
The Taylor series of an infinitely differentiable function π(π) centered at π is given by
∞
π(π) (π)
π′′ (π)
π′′′ (π)
π
′ (π)(π
π
(π
(π
(π − π)π + β―
∑
− π) = π(π) + π
− π) +
− π) +
π!
π!
π!
π=π
When π = π, we obtain the MacLaurin series of π(π) as
∞
∑
π=π
∞
ππ = ∑
π=π
π(π) (π) π
π′′ (π) π π′′′ (π) π
π = π(π) + π′ (π)π +
π +
π +β―
π!
π!
π!
ππ
ππ ππ
=π+π+ + +β―
π!
π! π!
∞
πππ π = ∑
π=π
(−π)π πππ
ππ ππ ππ
=π− +
− +β―
(ππ)!
π! π! π!
∞
πππ π = ∑
π=π
(−π)π πππ+π
ππ ππ ππ
=π− + − +β―
(ππ + π)!
π! π! π!
Polar ο« Rectangular
π = π πππ π½
π = π πππ π½
π π = π π + ππ
π
π
πππ π½ = π¨π« π½ = πππ−π
π
π
These identities will be needed for symmetries:
πππ(−π½) = −πππ(π½)
πππ(−π½) = πππ(π½)
πππ(π
− π½) = πππ(π½)
πππ(π
− π½) = −πππ(π½)
Symmetries of a Polar Curve π(π½)
If the speed coefficient of ο± is 1,2,3,..
e.g. π(π½) = πππ(ππ½)
If…
Then symmetric w.r.t.
x-axis
π(−π½) = π(π½)
y-axis
π(−π½) = −π(π½)
y-axis
π(π
− π½) = π(π½)
x-axis
π(π
− π½) = −π(π½)
origin
π(π
+ π½) = π(π½)
If the speed coefficient of ο± is 1/k
e.g. π(π½) = πππ(π½/π); π = π
If…
Then symmetric w.r.t.
x-axis
π(−π½ + πππ
) = π(π½)
y-axis
π(−π½ + πππ
) = −π(π½)
y-axis
π(π
− π½ + πππ
) = π(π½)
x-axis
π(π
− π½ + πππ
) = −π(π½)
origin
π(π
+ π½ + πππ
) = π(π½)
Areas and LengthsRelated to Polar Curves
π
π·
The area inside a polar curveπ(π½) between πΆ ≤ π½ ≤ π· is given byπ¨ = π ∫πΆ ππ (π½) π
π½
The area between two polar curves ππ (π½)(inner) and ππ (π½) (outer) between πΆ ≤ π½ ≤ π· is given by
π¨=
π π· π
∫ [π (π½) − πππ (π½)] π
π½
π πΆ π
π·
The length of a polar curveπ(π½)where π½ runs from πΆ to π· is given byπ³ = ∫πΆ √[π(π½)]π + [π′ (π½)]π π
π½
0
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