Continuity at x = a x=a x = a : f ( a ) f(a) f ( a ) defined, lim x → a f ( x ) \lim_{x\to a}f(x) lim x → a f ( x ) exists, and
lim x → a f ( x ) = f ( a ) \lim_{x\to a}f(x)=f(a) lim x → a f ( x ) = f ( a ) -- equivalently lim x → a − f ( x ) = lim x → a + f ( x ) = f ( a ) \lim_{x\to a^-}f(x)=\lim_{x\to a^+}f(x)=f(a) lim x → a − f ( x ) = lim x → a + f ( x ) = f ( a ) .
Differentiability at x = a x=a x = a : f ′ ( a ) = lim h → 0 [ f ( a + h ) − f ( a ) ] / h f'(a)=\lim_{h\to0}[f(a+h)-f(a)]/h f ′ ( a ) = lim h → 0 [ f ( a + h ) − f ( a )] / h exists. Differentiable
⇒ \Rightarrow ⇒ continuous, but NOT conversely (f ( x ) = ∣ x ∣ f(x)=|x| f ( x ) = ∣ x ∣ is continuous but not differentiable at
x = 0 x=0 x = 0 ).
Chain rule: for y = f ( u ) y=f(u) y = f ( u ) , u = g ( x ) u=g(x) u = g ( x ) , d y d x = d y d u ⋅ d u d x \dfrac{dy}{dx}=\dfrac{dy}{du}\cdot\dfrac{du}{dx} d x d y = d u d y ⋅ d x d u .
Inverse trigonometric derivatives:
d d x sin − 1 x = 1 1 − x 2 , d d x cos − 1 x = − 1 1 − x 2 , d d x tan − 1 x = 1 1 + x 2 , \frac{d}{dx}\sin^{-1}x=\frac{1}{\sqrt{1-x^2}},\quad \frac{d}{dx}\cos^{-1}x=-\frac{1}{\sqrt{1-x^2}},\quad \frac{d}{dx}\tan^{-1}x=\frac{1}{1+x^2}, d x d sin − 1 x = 1 − x 2 1 , d x d cos − 1 x = − 1 − x 2 1 , d x d tan − 1 x = 1 + x 2 1 ,
d d x cot − 1 x = − 1 1 + x 2 , d d x sec − 1 x = 1 ∣ x ∣ x 2 − 1 , d d x cosec − 1 x = − 1 ∣ x ∣ x 2 − 1 . \frac{d}{dx}\cot^{-1}x=-\frac{1}{1+x^2},\quad \frac{d}{dx}\sec^{-1}x=\frac{1}{|x|\sqrt{x^2-1}},\quad \frac{d}{dx}\text{cosec}^{-1}x=-\frac{1}{|x|\sqrt{x^2-1}}. d x d cot − 1 x = − 1 + x 2 1 , d x d sec − 1 x = ∣ x ∣ x 2 − 1 1 , d x d cosec − 1 x = − ∣ x ∣ x 2 − 1 1 .
Implicit differentiation: differentiate both sides w.r.t. x x x , applying the chain rule to
every y y y -term, then solve algebraically for d y / d x dy/dx d y / d x .
Exponential/logarithmic functions and derivatives: e x > 0 e^x>0 e x > 0 for all x x x , ln x \ln x ln x defined for
x > 0 x>0 x > 0 as the inverse of e x e^x e x ; d d x e x = e x \dfrac{d}{dx}e^x=e^x d x d e x = e x , d d x ln x = 1 x \dfrac{d}{dx}\ln x=\dfrac1x d x d ln x = x 1 ,
d d x a x = a x ln a \dfrac{d}{dx}a^x=a^x\ln a d x d a x = a x ln a , d d x log a x = 1 x ln a \dfrac{d}{dx}\log_ax=\dfrac{1}{x\ln a} d x d log a x = x ln a 1 ; composite forms
d d x e f ( x ) = e f ( x ) f ′ ( x ) \dfrac{d}{dx}e^{f(x)}=e^{f(x)}f'(x) d x d e f ( x ) = e f ( x ) f ′ ( x ) , d d x ln f ( x ) = f ′ ( x ) f ( x ) \dfrac{d}{dx}\ln f(x)=\dfrac{f'(x)}{f(x)} d x d ln f ( x ) = f ( x ) f ′ ( x ) .
Logarithmic differentiation: for y = [ f ( x ) ] g ( x ) y=[f(x)]^{g(x)} y = [ f ( x ) ] g ( x ) (variable base AND exponent) or a lengthy
product/quotient, take ln \ln ln of both sides first, differentiate implicitly, then multiply back by
y y y : d y d x = y ⋅ d d x [ ln y ] \dfrac{dy}{dx}=y\cdot\dfrac{d}{dx}\big[\ln y\big] d x d y = y ⋅ d x d [ ln y ] .
Parametric derivatives: for x = f ( t ) , y = g ( t ) x=f(t),\,y=g(t) x = f ( t ) , y = g ( t ) , d y d x = d y / d t d x / d t \dfrac{dy}{dx}=\dfrac{dy/dt}{dx/dt} d x d y = d x / d t d y / d t
(d x / d t ≠ 0 dx/dt\neq0 d x / d t = 0 ); the second derivative is …