AP Calculas AB

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Last updated 1:49 PM on 4/24/26
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80 Terms

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What does lim f(x) tell us?

End behavior / Horiontal Asymptote

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3 Reasons we don’t take a dirrivative

Discontinuity, Sharp Turn, Vertical Tangent

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Know this statement if the prompt says f(x) is differentiable

f(x) is diffrientiable and since diffrientability implies continuity f(x) is continuous

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dirrivative of sin(x)

cos(x)

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dirrivative of cos(x)

-sin(x)

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dirrivative of tan(x)

sec2x

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dirrivative of sec(x)

sec(x) * tan(x)

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dirrivative of csc(x)

-csc(x) * cot(x)

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dirrivative of cot(x)

-csc2x

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Particle is moving down

v(t) is less than 0

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Particle is moving up

v(t) is greater than 0

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Particle is stopped

v(t)=0

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Particle is slowing down

v(t) and v’(t) have diffrent signs

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The particle is speeding up

v(t) and v’(t) have the same sign

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The particle’s aceleration is negative

v’(t) is less than 0

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the particles aceleration is positive

v’(t) is greater than 0

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the particle changes direction

v(t) changes signs

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average velocity

change in position / change in time

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average aceleration

change in velocity / change in time

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f(x) is increasing

f’(x) is greater than 0

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f(x) Is deacreasing

f’(x) is less than 0

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f(x) has a relative maximum

f’(x) changes from - to +

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f(x) has a relative minimum

f’(x) changed from + to -

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f’(x) has an exstrema

f’(x) changes signs

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f(x) is concave down

f’’(x) is less than 0

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f(x) is concave down

f’’(x) is less than 0

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f(x) has a critical point

f’(x) = 0 or DNE

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f(x) has a point of inflection

f’’(x) changes signs and slope of f’(x) changes signs

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degree on top is than less than degree on bottom as x approaches infinity

0

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degree on top is greater than degree on bottom as x approaches infinity

DNE

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Degree on top is Equal to degree on bottom

ratio of leading coefficients

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Conditions for IVT

f is continuous on [A,B]

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Conditions for MVT

f is continuous on [A,B] and diffrientiable on (A,B)

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Graph of y= ex

(0,1) and (1,e)

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Graph of y= ln(x)

(1,0) and (e,1)

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e =

2.72

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e is between

1/3 < 1/e < 1/2

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dirrivative of ln(u)

u’ / u

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dirrivative of eu

eu * u’

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dirrivative of au

a * u’ lna

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intagrating ax

ax * 1/lna +c

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intagrating ex

ex + c

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intagrating 1/x

ln|x| + c

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if f and g are inverses with (a,b) on f and (b,a) on g, f’(a)

1/g’(b)

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change of bases logab

ln b / ln a

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direct variation

y= kx

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inverse variation

y = k/x

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exponential growth

y= Cekt

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intagrating sin(x)

-cos(x) + c

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intagrating cos(x)

sin(x) + c

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intagrating csc2(x)

-cot(x) + c

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intagrating sec2(x)

tan(x)

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intagrating sec(x) * tan(x)

sec(x) + c

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intagrating csc(x) * tan(x)

sec(x) +c

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intagrating csc(x) * cot(x)

-csc(x) + c

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ln 1

0

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e0

1

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ln 0

DNE

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intagrating cot(x)

ln|sin(x)|

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intagrating sec(x)

ln|sec(x) + tan(x)| + c

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intagrating csc(x)

-ln|csc(x) + cot(x)| + c

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dirivative of arc sin(u)

u’ / squareroot 1 - u2

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dirivative arc cos(u)

-u’ / squareroot 1 - u2

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dirivative arc tan

u’ / 1+u2

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dirivative arc cot(u)

-u’ / 1+u2

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dirrivative of arc sec(u)

u’ / |u| square root u2 -1

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dirrivative of arc csc(u)

-u’ / |u| square root u2 -1

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integral of du/ square root a2 - u2

arc sin(u/a) + c

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Total DIstance

intagration of |v(t)|

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intagration of tan(x)

-ln|cos(x)| + c

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intagral of du / a2 + u2

1/a arc tan u/a +c

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intagration of du/ u * square root u2 + a2

1/a arc sec |u| / a +c

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finding area by disk

pie integral (radius)2

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finiding area by washer

pie intragal of (outer)2 - pie (inner)2

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Cross Section: squares

intagral of (base)2

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Cross Section: squares equilateral triangles

squareroot of 3 / 4 intagral of (base)2

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Cross Section: isosceles right triangles

½ intagral of (base)2

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cross section: semicircles

pie / 8 (base)²

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Steps for solving a separable differential equations

seperate integrate solve

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