Mathematics¶
Calculus
\(\int udv = u\cdot v-\int du\cdot v\)
\(\displaystyle\Gamma(n)=\int_{0}^{\infty}x^{n-1}e^{-x}dx=(n-1)!\)
\(cos ^2(i\theta)+sin^2(i\theta) = cosh^2(\theta)- sinh^2(\theta)\)
\(cos(i\theta) = cosh(\theta)\)
\(sin(i\theta) = i\cdot sinh(\theta)\)
\(sin(x) = \dfrac{e^{jx}-e^{-jx}}{2j}\)
\(sinh(x) = \dfrac{e^{x}-e^{-x}}{2}\)
\(2\cos \alpha \cos \beta= \cos(\alpha-\beta)+\cos(\alpha+\beta)\)
\(2\sin \alpha \cos \beta= \sin(\alpha+\beta)+\sin(\alpha-\beta)\)
\(2\sin \alpha \sin \beta = \cos(\alpha-\beta)-\cos(\alpha+\beta)\)
\(\dfrac{sin(x)}{x}\)
zero-crossovers : \(x=K \pi\), \(K \in I - \{0\}\)
\(e^{-1}\)
=0.3678
Complex Analysis
\(e^{j2\pi k}e^{j\theta} = e^{j\theta}\)
\(i^n+i^{n+1}+i^{n+2}+i^{n+3}=0\)
root of unity
sum of ‘n’ roots of unity = 0
product of ‘n’ roots of unity = \((-1)^{n-1}\)
CR equation
\(f'(z_o) = u_x +i v_x=v_y-iu_y=e^{-i\theta}(u_r + iv_r)\)
cartesian
\(u_x=v_y \\ v_x = -u_y\)
polar
\(u_r=\frac{1}{r}v_{\theta} \\ v_r=-\frac{1}{r}u_{\theta}\)
milne thompson method
residue theorem
singular point→ point where complex function becomes non-analyticlaurent series around singularity: $\( f(z) = \sum \limits _{n=0}^{\infty} a_{n} (z-a)^{n} +\sum \limits _{m=1}^{\infty} b_{-m} (z-a)^{-m} \)$
\[\displaystyle \int_C f (z) dz = 2 \pi i \cdot\text{(sum of residues at the singular points within $z_o$ )}\]\[\text{residue}(f(z_o))=\text{coefficient of $(z-a)^{-1}$}=\lim \limits_{z\rightarrow z_o} \dfrac{1}{(n-1)!}\Big[ \dfrac{d^{n-1}}{dz^{n-1}}[(z-z_o)^nf(z)]\Big]\]
ODE
order → highest order derivative
degree → degree of highest order differential coefficient provided equation is polynomial in all differential coefficients
integration and differentiation
\(\displaystyle \int \dfrac{1}{\sqrt{x^2+a^2}} dx = \sin^{-1} \Big(\frac{x}{a}\Big) + C\)
\(\displaystyle \int \dfrac{1}{\sqrt{x^2-a^2}} dx = \cos^{-1} \Big(\frac{x}{a}\Big) + C\)
\(\displaystyle \int \dfrac{1}{x^2-a^2} dx = \dfrac{1}{a}\tan^{-1} \Big(\frac{x}{a}\Big) + C\)
variable separable
\(f(x) dx +g(y)dy =0\)
exact differential equation
\({M\left( {x,y} \right)dx + N\left( {x,y} \right)dy }= 0\)
\(\dfrac{{\partial M}}{{\partial x}} = \dfrac{{\partial N}}{{\partial y}}\)
\(\displaystyle\int dv = \int_\text{y = const} Mdx + \int_\text{\text{independent of x}} Ndy\)
\(\dfrac{dy}{dx}+p(x)y=r(x)\)
\(\displaystyle y e^{-\int p(x) dx } = \Big[\int r(x)e^{\int p(x) dx } dx +C \Big]\)
LDE of higher order
\(y=CF+PI\)
CF
CF is solution of \((D^n +a_1D^{n-1}+\dots +k_nD^0)y=0\)
if roots are
real and distinct: \(y =c_1e^{m_1x}+c_2e^{m_2x}\)if roots are
real and equal: \(y =(c_1+c_2x)e^{mx}\)if roots are
complex conjugate: \(y =(c_1\cos(\beta x)+c_2sin(\beta x))e^{\alpha x}\)PI
PI is solution of \((D^n +a_1D^{n-1}+\dots +k_nD^0)y=x\)
Linear Algebra
rank
atleast one minor of A of order r doesn’t vanish → rank(A) = r
eigen vectors
\([A] [X] =\lambda [X]\)
Probability
binomial distribution
\(\mu = np\)
\(\sigma ^2 = npq\)
\(\displaystyle P(r)= \binom{n}{r} p^r q^{n-r}\)