mathPhys
for RUG, in 2023
40 flashcards · Physics · by Kristóf Nagy
sin -> e^
cos -> e^
geometric/power series sum
if ∣r∣<1|r| < 1∣r∣<1
taylor series around a
Maclaurin series
binomial (1+x)k
binomial expansion/identity (x+y)n
cos(2x)
sin(2x)
cos(x)*cos(y)
sin(x)*sin(y)
δ(ak)=\delta(ak) = δ(ak)=
δ(ak)=1∣a∣δ(k)\delta (ak) = \frac{1}{|a|} \delta(k)δ(ak)=∣a∣1δ(k)
Fourier power series
f(x)=∑n=−∞∞cneinπxLf(x)=\sum_{n=-\infty}^{\infty}c_n e^{i\frac{n\pi x}{L}}f(x)=∑n=−∞∞cneiLnπx
Fourier power series cn
cn=12L∫−LLf(x)e−inπxLc_n =\frac{1}{2L} \int_{-L}^{L} f(x) e^{-i\frac{n\pi x}{L}}cn=2L1∫−LLf(x)e−iLnπx dxdxdx
even function rule
f(−x)=f(x)f(-x) = f(x)f(−x)=f(x)
odd function rule
f(−x)=−f(x)f(-x) = -f(x)f(−x)=−f(x)
even function examples
cos(x),x2,x4,...cos(x),x^2,x^4,...cos(x),x2,x4,...
odd function examples
sin(x),x,x3,...sin(x), x, x^3, ...sin(x),x,x3,...
odd integral rule
∫−aaodd=∫−aaodd∗even=0\int_{-a}^{a} odd = \int_{-a}^{a} odd * even = 0∫−aaodd=∫−aaodd∗even=0
Fourier series
f(x)=a0+∑n=1∞ancos(nπxL)+∑n=1∞bnsin(nπxL)f(x)=a_0 + \sum_{n=1}^{\infty}a_n cos(\frac{n\pi x}{L}) + \sum_{n=1}^{\infty}b_n sin(\frac{n\pi x}{L})f(x)=a0+∑n=1∞ancos(Lnπx)+∑n=1∞bnsin(Lnπx)
Fourier series a0
a0=12L∫−LLf(x)dxa_0=\frac{1}{2L}\int_{-L}^{L} f(x) dxa0=2L1∫−LLf(x)dx
Fourier series an
an=1L∫−LLf(x)cos(nπxL)dxa_n=\frac{1}{L}\int_{-L}^{L} f(x) cos(\frac{n\pi x}{L})dxan=L1∫−LLf(x)cos(Lnπx)dx
Fourier series bn
bn=1L∫−LLf(x)sin(nπxL)dxb_n=\frac{1}{L}\int_{-L}^{L} f(x) sin(\frac{n\pi x}{L})dxbn=L1∫−LLf(x)sin(Lnπx)dx
aux eq, 2 Re sol -> y_c
yc=c1er1t+c2er2ty_c=c_1 e^{r_1 t} + c_2 e^{r_2 t}yc=c1er1t+c2er2t
aux eq, 1 Re sol -> y_c
yc=c1ert+c2terty_c = c_1 e^{rt} + c_2 t e^{rt}yc=c1ert+c2tert
aux eq, 2 Im sol -> y_c
yc=eat(c1cos(bt)+c2sin(bt))y_c = e^{at}(c_1 cos(bt) + c_2 sin(bt))yc=eat(c1cos(bt)+c2sin(bt))
yp:eay_p: e^ayp:ea
yp=Aeay_p=Ae^ayp=Aea
yp:x2exy_p: x^2e^xyp:x2ex
yp=(Ax3+Bx2+Cx)exy_p=(Ax^3+Bx^2+Cx)e^xyp=(Ax3+Bx2+Cx)ex
ypy_pyp : cos x or sin x
yp=Acos(x)+Bsin(x)y_p=Acos(x)+Bsin(x)yp=Acos(x)+Bsin(x) (replace A and B with seperate x combination part if also x)
inverse Fourier transform
f(x)=∫−∞+∞F(k)e2πikxdkf(x)=\int_{-\infty}^{+\infty} F(k)e^{2\pi ikx}dkf(x)=∫−∞+∞F(k)e2πikxdk
forward Fourier transform
F(k)=∫−∞+∞f(x)e−2πikxdxF(k)=\int_{-\infty}^{+\infty} f(x)e^{-2\pi ikx}dxF(k)=∫−∞+∞f(x)e−2πikxdx
Dirac delta (k)
δ(k)=∫−∞+∞e−i2πkxdx\delta(k)=\int_{-\infty}^{+\infty} e^{-i 2\pi kx}dxδ(k)=∫−∞+∞e−i2πkxdx
Kronecker delta (nm)
∫−LLei(n−m)πLxdx=(2L)δnm\int_{-L}^{L} e^{i \frac{(n-m)\pi}{L}x} dx = (2L)\delta_{nm}∫−LLeiL(n−m)πxdx=(2L)δnm
delta integral
delta(-x)=
|f(x)|2
f(x)⋅f∗(x)f(x) \cdot f^*(x)f(x)⋅f∗(x) =∣f(x)∣2=|f(x)|^2=∣f(x)∣2
basic sin cos ^2
sin2(x)+cos2(x)=1sin^2(x)+cos^2(x)=1sin2(x)+cos2(x)=1
euler's formula
geometric series sum