Solution to quadratic equations ax² + bx + c = 0
x = \frac{-b \pm \sqrt{b^2-4ac}}{2a}Browse, search, and copy commonly used LaTeX formulas. Click any formula to copy it to your clipboard.
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Solution to quadratic equations ax² + bx + c = 0
x = \frac{-b \pm \sqrt{b^2-4ac}}{2a}Expansion of (x+y)ⁿ
(x+y)^n = \sum_{k=0}^{n} \binom{n}{k} x^{n-k} y^kFactorization of difference of two squares
a^2 - b^2 = (a+b)(a-b)Definition of derivative as a limit
f'(x) = \lim_{h \to 0} \frac{f(x+h) - f(x)}{h}Derivative of composite functions
\frac{d}{dx}[f(g(x))] = f'(g(x)) \cdot g'(x)Connection between derivatives and integrals
\int_a^b f(x) \, dx = F(b) - F(a), \quad F'(x) = f(x)Gaussian distribution probability density
f(x) = \frac{1}{\sigma\sqrt{2\pi}} e^{-\frac{1}{2}\left(\frac{x-\mu}{\sigma}\right)^2}Update probability based on new evidence
P(A|B) = \frac{P(B|A)P(A)}{P(B)}Matrix eigenvalue and eigenvector
A\vec{v} = \lambda\vec{v}Inner product of two vectors
\vec{a} \cdot \vec{b} = \sum_{i=1}^{n} a_i b_i = |\vec{a}||\vec{b}|\cos\thetaFundamental trigonometric identity
\sin^2\theta + \cos^2\theta = 1Complex exponential and trigonometric functions
e^{i\theta} = \cos\theta + i\sin\thetaForce equals mass times acceleration
F = maEinstein's famous equation
E = mc^2Fundamental equation of quantum mechanics
i\hbar\frac{\partial}{\partial t}\Psi = \hat{H}\PsiArea of circle with radius r
A = \pi r^2Volume of sphere with radius r
V = \frac{4}{3}\pi r^3Necessary conditions for complex differentiability
\frac{\partial u}{\partial x} = \frac{\partial v}{\partial y}, \quad \frac{\partial u}{\partial y} = -\frac{\partial v}{\partial x}Integral transform for solving ODEs
\mathcal{L}\{f(t)\} = F(s) = \int_0^{\infty} e^{-st}f(t) \, dtTaylor series expansion around point a
f(x) = \sum_{n=0}^{\infty} \frac{f^{(n)}(a)}{n!}(x-a)^nRepresentation of periodic functions as sum of sines and cosines
f(x) = \frac{a_0}{2} + \sum_{n=1}^{\infty} \left(a_n\cos\left(\frac{n\pi x}{L}\right) + b_n\sin\left(\frac{n\pi x}{L}\right)\right)Connection between line integrals and surface integrals
\oint_C \vec{F} \cdot d\vec{r} = \iint_S (\nabla \times \vec{F}) \cdot d\vec{S}Sample means approach normal distribution as sample size increases
\lim_{n \to \infty} P\left(\frac{\bar{X}_n - \mu}{\sigma/\sqrt{n}} \leq z\right) = \Phi(z)Distance from origin in 3D space
d = \sqrt{x^2 + y^2 + z^2}Evaluate limits of indeterminate forms
\lim_{x \to c} \frac{f(x)}{g(x)} = \lim_{x \to c} \frac{f'(x)}{g'(x)}Product rule for integration
\int u \, dv = uv - \int v \, duInverse of 2×2 matrix
A^{-1} = \frac{1}{\det(A)}\begin{pmatrix} d & -b \\ -c & a \end{pmatrix}Interval estimate for population mean
\bar{x} \pm z_{\alpha/2} \frac{\sigma}{\sqrt{n}}Fundamental equations of electromagnetism
\nabla \cdot \vec{E} = \frac{\rho}{\epsilon_0}, \quad \nabla \times \vec{E} = -\frac{\partial \vec{B}}{\partial t}Method to convert quadratic to vertex form
ax^2 + bx + c = a\left(x + \frac{b}{2a}\right)^2 + c - \frac{b^2}{4a}Sum of finite geometric series
\sum_{k=0}^{n} ar^k = a\frac{1-r^{n+1}}{1-r}, \quad r \neq 1Sum of arithmetic sequence
\sum_{k=1}^{n} (a + (k-1)d) = \frac{n}{2}(2a + (n-1)d)Fundamental theorem of calculus
\int_{a}^{b} f(x) \, dx = F(b) - F(a)Derivative of product of functions
\frac{d}{dx}[f(x)g(x)] = f'(x)g(x) + f(x)g'(x)Derivative of quotient of functions
\frac{d}{dx}\left[\frac{f(x)}{g(x)}\right] = \frac{f'(x)g(x) - f(x)g'(x)}{[g(x)]^2}Derivative of power function
\frac{d}{dx}[x^n] = nx^{n-1}Arithmetic mean of a dataset
\bar{x} = \frac{1}{n} \sum_{i=1}^{n} x_iMeasure of data spread
\sigma^2 = \frac{1}{n} \sum_{i=1}^{n} (x_i - \mu)^2Square root of variance
\sigma = \sqrt{\frac{1}{n} \sum_{i=1}^{n} (x_i - \mu)^2}Measure of joint variability
\text{Cov}(X,Y) = \frac{1}{n}\sum_{i=1}^{n}(x_i - \bar{x})(y_i - \bar{y})Pearson correlation coefficient
r = \frac{\text{Cov}(X,Y)}{\sigma_X \sigma_Y}Probability of k successes in n trials
P(X = k) = \binom{n}{k}p^k(1-p)^{n-k}Definition of matrix product
(AB)_{ij} = \sum_{k=1}^{n} A_{ik} B_{kj}Determinant of 2×2 matrix
\det\begin{pmatrix} a & b \\ c & d \end{pmatrix} = ad - bcVector product in 3D space
\vec{a} \times \vec{b} = \begin{vmatrix} \vec{i} & \vec{j} & \vec{k} \\ a_1 & a_2 & a_3 \\ b_1 & b_2 & b_3 \end{vmatrix}Sum of diagonal elements
\text{tr}(A) = \sum_{i=1}^{n} a_{ii}Relationship between sides and angles in triangles
\frac{a}{\sin A} = \frac{b}{\sin B} = \frac{c}{\sin C}Generalization of Pythagorean theorem
c^2 = a^2 + b^2 - 2ab\cos CSine of double angle
\sin(2\theta) = 2\sin\theta\cos\thetaCosine of double angle
\cos(2\theta) = \cos^2\theta - \sin^2\thetaSine of sum of two angles
\sin(\alpha + \beta) = \sin\alpha\cos\beta + \cos\alpha\sin\betaEnergy of motion
KE = \frac{1}{2}mv^2Energy due to position in gravitational field
PE = mghLinear momentum of an object
p = mvRelationship between work and kinetic energy
W = \Delta KE = \frac{1}{2}m(v_f^2 - v_i^2)Relationship between voltage, current, and resistance
V = IRElectrostatic force between charges
F = k\frac{q_1 q_2}{r^2}Newton's law of universal gravitation
F = G\frac{m_1 m_2}{r^2}Relationship between wave speed, frequency, and wavelength
v = f\lambdaForce on charged particle in electromagnetic field
\vec{F} = q(\vec{E} + \vec{v} \times \vec{B})Connection between line integral and double integral in the plane
\oint_C (P\,dx + Q\,dy) = \iint_D \left(\frac{\partial Q}{\partial x} - \frac{\partial P}{\partial y}\right) dAConnection between surface integral and volume integral
\oiint_S \vec{F} \cdot d\vec{S} = \iiint_V (\nabla \cdot \vec{F}) \, dVPowers of complex numbers in polar form
(\cos\theta + i\sin\theta)^n = \cos(n\theta) + i\sin(n\theta)Approximation of definite integral using rectangles
\sum_{i=1}^{n} f(x_i^*) \Delta x_iProbability distribution for rare events
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