Calc stuff 2

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Last updated 9:26 PM on 6/23/26
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94 Terms

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xn+1n+1\frac{x^{n+1}}{n+1} + C

∫xn dx =

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1xd(x)\int\frac{1}{x}d\left(x\right)

ln|x| + C

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∫ ekx dx

ekxk+C\frac{e^{kx}}{k}+C

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Chain Rule: d/dx [f(g(x))] =

f’(g) g’(x)

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∫cos(kx) dx =

1k\frac{1}{k} sin(kx) + c

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∫sin(kx) dx =

1k\frac{1}{k} cos(kx) + c

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∫sec2 x dx =

tan(x) + c

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∫csc(x) cot(x) dx =

-csc(x) + c

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∫sec(x) tan(x) dx =

sec(x) + C

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∫csc² x dx =

-cot(x) + C

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Slope of the Secant Line

A measure of the slope of the tangent line, or the rate of change, of f(x)f(x) at the given point (a,f(a))(a, f(a)) calculated as f(x)f(a)xa\frac{f(x) - f(a)}{x - a} .

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Instantaneous Velocity

The limiting values of the average velocities over shorter and shorter time periods.

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Limit of a Function

To say that limxaf(x)=L\lim_{x \to a} f(x) = L means that as xx approaches aa, but xax \neq a, then f(x)f(x) must approach LL.

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One-Sided Limits

A limit where the value is different when approaching from either the positive side (xa+x \to a^+) or the negative side (xax \to a^-).

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Infinite Limit Theorem (Positive Even Integer)

If nn is a positive even integer, then limxa+1(xa)n=\lim_{x \to a^+} \frac{1}{(x-a)^n} = \infty, limxa1(xa)n=\lim_{x \to a^-} \frac{1}{(x-a)^n} = \infty, and limxa1(xa)n=\lim_{x \to a} \frac{1}{(x-a)^n} = \infty.

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Infinite Limit Theorem (Positive Odd Integer)

If nn is a positive odd integer, then limxa+1(xa)n=\lim_{x \to a^+} \frac{1}{(x-a)^n} = \infty and limxa1(xa)n=\lim_{x \to a^-} \frac{1}{(x-a)^n} = -\infty, hence the two-sided limit is DNE (Does Not Exist).

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Sum Law Limits

The limit law stating limxa[f(x)+g(x)]=limxaf(x)+limxag(x)\lim_{x \to a} [f(x) + g(x)] = \lim_{x \to a} f(x) + \lim_{x \to a} g(x).

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Limits Product Law

The limit law stating limxa[f(x)g(x)]=(limxaf(x))(limxag(x))\lim_{x \to a} [f(x) g(x)] = (\lim_{x \to a} f(x)) (\lim_{x \to a} g(x)).

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Direct Substitution Property

If ff is a function such that aa is in the domain of ff, then limxaf(x)=f(a)\lim_{x \to a} f(x) = f(a).

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Squeeze Theorem

If f(x)g(x)h(x)f(x) \leq g(x) \leq h(x) when xx is near aa (but not necessarily equal to aa) and limxaf(x)=L=limxah(x)\lim_{x \to a} f(x) = L = \lim_{x \to a} h(x), then limxag(x)=L\lim_{x \to a} g(x) = L.

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Continuity at a Point

A function ff is continuous at aa if:
1. f(a)f(a) is defined;
2. limxaf(x)\lim_{x \to a} f(x) exists;
3. limxaf(x)=f(a)\lim_{x \to a} f(x) = f(a).

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Limit Definition of Derivative

The derivative of a function at a number aa, denoted by f(a)f'(a), is defined as f(a)=limh0f(a+h)f(a)hf'(a) = \lim_{h \to 0} \frac{f(a+h) - f(a)}{h}.

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Differentiable at a Number

A function ff is differentiable at a number aa if the limit f(a)=limh0f(a+h)f(a)hf'(a) = \lim_{h \to 0} \frac{f(a+h) - f(a)}{h} exists.

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Differentiability Implies Continuity

If f(x)f(x) is differentiable at aa, then ff is continuous at aa.

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The Power Rule Derivatives

The differentiation rule stating that for any real number nn, ddx[xn]=nxn1\frac{d}{dx} [x^n] = n x^{n-1}.

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The Product Rule

The differentiation rule stating that ddx[f(x)g(x)]=f(x)g(x)+f(x)g(x)\frac{d}{dx} [f(x) g(x)] = f'(x) g(x) + f(x) g'(x).

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The Quotient Rule

The differentiation rule stating that ddx[f(x)g(x)]=g(x)f(x)f(x)g(x)[g(x)]2\frac{d}{dx} [\frac{f(x)}{g(x)}] = \frac{g(x) f'(x) - f(x) g'(x)}{[g(x)]^2}.

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Particle at Rest

The state of a moving particle when its velocity at time tt is equal to zero (v(t)=0v(t) = 0).

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Horizontal Tangent Line

A line on a function f(x)f(x) where the slope is zero, found by setting the derivative f(x)=0f'(x) = 0.

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Big Three Limits

  1. limx0sin(ax)ax=1\lim_{x\to0}\frac{\sin(ax)}{ax}=1 ;

  2. limx01cos(ax)ax=0\lim_{x\to0}\frac{1-\cos\left(ax\right)}{ax}=0 ;

  3. limx0tan(x)x=1\lim_{x \to 0} \frac{\tan(x)}{x} = 1 .

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dd(x)ln(g(x))\frac{d}{d\left(x\right)}\ln\left(g\left(x\right)\right)

g(x)g(x)\frac{g^{\prime}\left(x\right)}{g\left(x\right)}

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dd(x)(loga(x))\frac{d}{d\left(x\right)}\left(\log_{a}\left(x\right)\right)

1xln(a),x>0\frac{1}{x\ln\left(a\right)},x>0 .

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dd(x)(logag(x))\frac{d}{d\left(x\right)}\left(\log_{a}g\left(x\right)\right)

g(x)g(x)lna\frac{g^{\prime}\left(x\right)}{g\left(x\right)\ln a}

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dd(x)(ex)\frac{d}{d\left(x\right)}\left(e^{x}\right)

exe^{x}

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d(dx)(ax)\frac{d}{\left(dx\right)}\left(a^{x}\right)

axln(a)a^{x}\ln\left(a\right)

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dd(x)(eg(x))\frac{d}{d\left(x\right)}\left(e^{g\left(x\right)}\right)

eg(x)g(x)e^{g\left(x\right)}g^{\prime}\left(x\right)

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dd(x)(ag(x))\frac{d}{d\left(x\right)}\left(a^{g\left(x\right)}\right)

ln(a)ag(x)g(x)\ln\left(a\right)a^{g\left(x\right)}g^{\prime}\left(x\right)

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dd(x)cos1(x)\frac{d}{d\left(x\right)}\cos^{-1}\left(x\right) =

11x2\frac{-1}{\sqrt{1-x^2}}

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dd(x)sin1(x)\frac{d}{d\left(x\right)}\sin^{-1}\left(x\right) =

11x2\frac{1}{\sqrt{1-x^2}}

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dd(x)cot1(x)\frac{d}{d\left(x_{}\right)}\cot^{-1}\left(x\right) =

11+x2\frac{-1}{1+x^2}

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dd(x)csc1(x)\frac{d}{d\left(x\right)}\csc^{-1}\left(x\right) =

1x1x2\frac{-1}{|x|\sqrt{1-x^2}}

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dd(x)tan1(x)\frac{d}{d\left(x\right)}\tan^{-1}\left(x\right) =

11+x2\frac{1}{1+x^2}

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dd(x)sec1(x)\frac{d}{d\left(x\right)}\sec^{-1}\left(x\right)

1x1x2\frac{1}{\left|x\right|\sqrt{1-x^2}}

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sec2(x) =

1 + tan²(x)

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d/dx (1/x) =

1x2-\frac{1}{x^2}

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dd(x)(x)=\frac{d}{d\left(x\right)}\left(\sqrt{x}\right)=

12x\frac{1}{2\sqrt{x}}

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Particle is slowing down:

v(t) and a(t) have different signs

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Particle is moving left/down:

v(t) < 0 (negative)

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Particle is moving right/up:

v(t) > 0 (positive)

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Particle is speeding up: (|velocity| is getting bigger)

v(t) and a(t) have same sign

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Intermediate Value Theorem

If f is continuous on [a,b] and k is any number between f(a) and f(b), then there is at least one number c between a and b such that f(c) = k

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Steps for Absolute Mins/Max:

  1. Find critical numbers using derivative

  1. Identify endpoints

  2. f(critical point) and f(end point)

  3. Determine absolute max/min values by comparing the y-values, stated in a sentence

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Mean Value Theorem

f(c)=f(b)f(a)baf^{\prime}\left(c\right)=\frac{f\left(b\right)-f\left(a\right)}{b-a}

If f is continuous on [a,b] and differentiable on (a,b), then there exists a number “c” on (a,b):

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x = c if a critical number because

f’(x) = 0 or f’(x) is undefined

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f(x) is ____ on [a,b] because f’(x) > 0

increasing

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f(x) is ____ on [a,b] because f’(x) < 0

decreasing

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f(x) is ____ on (a,b) because f’’(x) > 0

concave up

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f(x) is ____ on (a,b) because f’’(x) < 0

concave down

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f’’(x) = 0 or = DNE and f“(x) changes sign around point c. (Or if f’(x) slope changes sign and f’’(x) = 0 or DNE)

Inflection point

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tanxdx=∫\tan xdx=

lncosx+C-\ln\left|\cos x\right|+C

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(1(x2+a2))d(x)\int\left(\frac{1}{\left(x^2+a^2\right)}\right)d\left(x\right)

1atan1(xa)+C\frac{1}{a}\tan^{-1}\left(\frac{x}{a}\right)+C

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F.T.O.C :ab ⁣f(x)dx=\int_{a}^{b}\!f^{\prime}\left(x\right)\,dx=

f(b)f(a)f\left(b\right)-f\left(a\right)

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ab ⁣f(x)+g(x)dx=\int_{a}^{b}\!f\left(x\right)+g\left(x\right)\,dx=

ab ⁣f(x)d(x)+ab ⁣g(x)d(x)\int_{a}^{b}\!f\left(x\right)d\left(x\right)+\int_{a}^{b}\!g\left(x\right)d\left(x\right)

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ab ⁣f(x)g(x)dx=\int_{a}^{b}\!f\left(x\right)-g\left(x\right)\,dx=

ab ⁣f(x)d(x)ab ⁣g(x)d(x)\int_{a}^{b}\!f\left(x\right)\,d\left(x\right)-\int_{a}^{b}\!g\left(x\right)d\left(x\right)

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ab ⁣cf(x)dx=\int_{a}^{b}\!cf\left(x\right)\,dx=

cab ⁣f(x)dxc\int_{a}^{b}\!f\left(x\right)\,dx

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ab ⁣f(x)dx=\int_{a}^{b}\!f\left(x\right)\,dx=

ba ⁣f(x)dx-\int_{b}^{a}\!f\left(x\right)\,dx

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aa ⁣f(x)dx=\int_{a}^{a}\!f\left(x\right)\,dx=

0

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Average Value of a Function

1baab ⁣f(x)d(x)\frac{1}{b-a}\int_{a}^{b}\!f\left(x\right)d\left(x\right)

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Second F.T.O.C. P1:

dd(x)ax ⁣f(t)d(t)=\frac{d}{d\left(x\right)}\int_{a}^{x}\!f\left(t\right)\,d\left(t\right)= f(x)

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Second F.T.O.C. P2:

dd(x)ag(x) ⁣f(t)d(t)=\frac{d}{d\left(x\right)}\int_{a}^{g\left(x\right)}\!f\left(t\right)d\left(t\right)=  ⁣f(g(x))g(x)\!f\left(g\left(x\right)\right)\cdot\,g^{\prime}\left(x\right)

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ab ⁣f(x)dx\int_{a}^{b}\!f\left(x\right)\,dx represents the ___ ______ in the function f from time a to b.

net change

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Steps to solve differential equations.

  1. separate variables

  2. integrate each side

  3. make sure to place C on side with independent variable (usually x)

  4. plug initial condition and solve for C (if given)

  5. solve for dependent variable (usually y)

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y=Cekty=Ce^{kt} or y=y0ekty=y_0e^{kt}

Exponential growth

y= end amount

C or y0 = initial amount

k = growth constant/growth rate

t = time elapsed

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y=y0ekty=y_0e^{-kt}

Exponential decay

negative sign = decays over time, rather than growing.

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Velocity

v(t) = s’(t) = ∫a(t)dt

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acceleration

a(t) = v’(t) = s’’(t)

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speed

|v'(t)|

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average velocity

s(b)s(a)ba\frac{s\left(b\right)-s\left(a\right)}{b-a} (given v(t)); or 1baab ⁣v(t)dt\frac{1}{b-a}\int_{a}^{b}\!v\left(t\right)\,dt (given a(t))

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average acceleration

v(b)v(a)ba\frac{v\left(b\right)-v\left(a\right)}{b-a} (given v(t)); or 1baab ⁣a(t)dt\frac{1}{b-a}\int_{a}^{b}\!a\left(t\right)\,dt (given a(t))

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Displacement

ab ⁣v(t)dt\int_{a}^{b}\!v\left(t\right)\,dt

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total distance

ab ⁣v(t)dt\int_{a}^{b}\left|\!v\left(t\right)\right|\,dt

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position at b

s(b)=s(a)+ab ⁣v(t)dts\left(b\right)=s\left(a\right)+\int_{a}^{b}\!v\left(t\right)\,dt

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Area perpendicular to x-axis; f(x) is top curve, g(x) is bottom, a and b are x-coordinates of point of intersection.

ab ⁣[f(x)g(x)]dx=\int_{a}^{b}\!\left\lbrack f\left(x\right)-g\left(x\right)\right\rbrack\,dx=

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Area perpendicular to y-axis; f(y) is right curve, g(y) is left curve, a and b are y-coordinates of point of intersection.

ab ⁣[f(y)g(y)]d(y)=\int_{a}^{b}\!\left\lbrack f\left(y\right)-g\left(y\right)]d\left(y\right)=\right.

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Volume steps

  1. Decide whether it’s a dx or dy

  2. Find a formula in terms of x or y

  3. Find the limits (make sure they match x or y)

  4. integrate and evaluate

Volume = ∫Area

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Volume of a disc around a Horizontal Axis of rotation

V = ab ⁣πr2dx\int_{a}^{b}\!\pi r^2dx

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Volume of a washer around a horizontal axis of rotation.

ab ⁣[πR2πr2]d(x)\int_{a}^{b}\!\left\lbrack\pi R^2-\pi r^2\right\rbrack d\left(x\right)

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ab ⁣A(x)dx\int_{a}^{b}\!A\left(x\right)\,dx

Volume of a slab (cross-section) around a horizontal axis of rotation. A(x) is the area for the cross section.

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Volume of a disc around a vertical axis of rotation

V = ab ⁣πr2dy\int_{a}^{b}\!\pi r^2dy

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Volume of a washer around a vertical axis of rotation

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Volume of a slab (cross-section) around a vertical axis of rotation. A(y) is the area for the cross section.

ab ⁣A(y)dy\int_{a}^{b}\!A\left(y\right)\,dy

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Volume using shells

V = ∫2πr h (Thickness)

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For volume rotated around a vertical axis (y-axis), using shells method.

ab ⁣2π(r)(h(x))d(x))\int_{a}^{b}\!2\pi\left(r\right)\left(h\left(x\right)\right)d\left(x\right))

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For volume rotated around a horizontal axis (x-axis), using shells method.

ab ⁣2π(r)(h(y))d(y)\int_{a}^{b}\!2\pi\left(r\right)\left(h\left(y\right)\right)d\left(y\right)