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Unit XIII · Electronics

Rectifiers & diode current

FormulaUse
If=VfrfI_f = \frac{V_f}{r_f}
Forward current
Ir=VrrrI_r = \frac{V_r}{r_r}
Reverse current
Form factor=VrmsVav\text{Form factor} = \frac{V_{\mathrm{rms}}}{V_{\mathrm{av}}}
Form factor
Half-wave:Tout=Tin\text{Half-wave:}\quad T_{\mathrm{out}}=T_{\mathrm{in}}
fout=finf_{\mathrm{out}}=f_{\mathrm{in}}
Time period and frequency
Half-wave:Vrms=V02\text{Half-wave:}\quad V_{\mathrm{rms}}=\frac{V_0}{2}
Vav=V0πV_{\mathrm{av}}=\frac{V_0}{\pi}
RMS and average output voltage
Full-wave:Tout=Tin2\text{Full-wave:}\quad T_{\mathrm{out}}=\frac{T_{\mathrm{in}}}{2}
fout=2finf_{\mathrm{out}}=2f_{\mathrm{in}}
Time period and frequency
Full-wave:Vrms=V02\text{Full-wave:}\quad V_{\mathrm{rms}}=\frac{V_0}{\sqrt{2}}
Vav=2V0πV_{\mathrm{av}}=\frac{2V_0}{\pi}
RMS and average output voltage

Units X–XI · Magnetism & electromagnetic induction

Magnetic field, force & charged particles

FormulaUse
Φ=B⃗⋅A⃗=BAcos⁡θ\Phi=\vec{B}\cdot\vec{A}=BA\cos\theta
Magnetic flux through a vector area
Φ=BAsin⁡θ\Phi=BA\sin\theta
Magnetic flux through a plane area
B=ΦAB=\frac{\Phi}{A}
Magnetic flux density for perpendicular field
B=μ0I2πrB=\frac{\mu_0 I}{2\pi r}
Field outside a long straight conductor
B=μ0Ir2πR2B=\frac{\mu_0 Ir}{2\pi R^2}
Field inside a solid long straight conductor
B=μ0I2RB=\frac{\mu_0 I}{2R}
Field at centre of one circular loop
B=μ0NI2RB=\frac{\mu_0 NI}{2R}
Field at centre of N-turn coil
B=μ0nIB=\mu_0 nI
Field inside a long solenoid
Bend=μ0nI2B_{\mathrm{end}}=\frac{\mu_0 nI}{2}
Field at end of a solenoid
F=BILsin⁡θF=BIL\sin\theta
Force on a current-carrying conductor
τ=NIBAcos⁡α\tau=NIBA\cos\alpha
Torque on a current coil
FL=μ0I1I22πd\frac{F}{L}=\frac{\mu_0 I_1 I_2}{2\pi d}
Force per unit length between parallel currents
F=qvBsin⁡θF=qvB\sin\theta
Force on a moving charge in magnetic field
r=mvqB=pqBr=\frac{mv}{qB}=\frac{p}{qB}
Cyclotron radius
r=2m KEqBr=\frac{\sqrt{2m\,\mathrm{KE}}}{qB}
Cyclotron radius in terms of kinetic energy
qm=2VB2r2\frac{q}{m}=\frac{2V}{B^2r^2}
Charge-to-mass ratio from cyclotron potential
F⃗=qE⃗+q(v⃗×B⃗)\vec{F}=q\vec{E}+q(\vec{v}\times\vec{B})
Lorentz force
v=EBv=\frac{E}{B}
Velocity selected by crossed E and B fields

Electrostatics

Charge, field, potential & capacitors

FormulaUse
Q=neQ=ne
Quantisation of charge
F=14πε0q1q2r2F=\frac{1}{4\pi\varepsilon_0}\frac{q_1q_2}{r^2}
Coulomb force in vacuum
F=14πε0εrq1q2r2F=\frac{1}{4\pi\varepsilon_0\varepsilon_r}\frac{q_1q_2}{r^2}
Coulomb force in a medium
k=14πε0k=\frac{1}{4\pi\varepsilon_0}
Coulomb constant
E=Fq0=kqr2E=\frac{F}{q_0}=\frac{kq}{r^2}
Electric field strength
ΦE=E⃗⋅A⃗=EAcos⁡θ\Phi_E=\vec{E}\cdot\vec{A}=EA\cos\theta
Electric flux through vector area
ΦE=EAsin⁡θ\Phi_E=EA\sin\theta
Electric flux through plane area
ΦE=Qε0\Phi_E=\frac{Q}{\varepsilon_0}
Gauss's law in vacuum
E=σ2ε0E=\frac{\sigma}{2\varepsilon_0}
Field of an infinite charged sheet
E=σε0E=\frac{\sigma}{\varepsilon_0}
Field between oppositely charged sheets
V=Wq0=kqrV=\frac{W}{q_0}=\frac{kq}{r}
Potential at a point charge
E=−ΔVΔrE=-\frac{\Delta V}{\Delta r}
Electric field as potential gradient
ΔV=kq(1r1−1r2)\Delta V=kq\left(\frac{1}{r_1}-\frac{1}{r_2}\right)
Potential difference between two points
C=QVC=\frac{Q}{V}
Capacitance
C=ε0AdC=\frac{\varepsilon_0 A}{d}
C=ε0εrAdC=\frac{\varepsilon_0\varepsilon_r A}{d}
Parallel-plate capacitance without / with dielectric
W=12QV=12CV2=Q22CW=\frac{1}{2}QV=\frac{1}{2}CV^2=\frac{Q^2}{2C}
Energy stored in a capacitor
1Ceq=1C1+1C2+⋯\frac{1}{C_{\mathrm{eq}}}=\frac{1}{C_1}+\frac{1}{C_2}+\cdots
Capacitors in series
Ceq=C1+C2+⋯C_{\mathrm{eq}}=C_1+C_2+\cdots
Capacitors in parallel
τ=RC\tau=RC
RC time constant
Charging:q=q0(1−e−t/(RC))\text{Charging:}\quad q=q_0\left(1-e^{-t/(RC)}\right)
V=V0(1−e−t/(RC))V=V_0\left(1-e^{-t/(RC)}\right)
I=I0e−t/(RC)I=I_0e^{-t/(RC)}
Charging capacitor
Discharging:q=q0e−t/(RC)\text{Discharging:}\quad q=q_0e^{-t/(RC)}
V=V0e−t/(RC)V=V_0e^{-t/(RC)}
I=I0e−t/(RC)I=I_0e^{-t/(RC)}
Discharging capacitor (magnitude)

Rotational & circular motion

Circular motion & gravity

FormulaUse
Fc=mv2rF_c=\frac{mv^2}{r}
Centripetal force
mv2r=GMmr2\frac{mv^2}{r}=\frac{GMm}{r^2}
Satellite in circular orbit
mv2r=μN\frac{mv^2}{r}=\mu N
Car on an unbanked circular road
mv2r=kqQr2\frac{mv^2}{r}=\frac{kqQ}{r^2}
Electron around nucleus (classical model)
mv2r=qvB\frac{mv^2}{r}=qvB
Charged particle in magnetic field
mv2r=T\frac{mv^2}{r}=T
Object tied to a string in horizontal circle
v=rgtan⁡θv=\sqrt{rg\tan\theta}
Critical speed for a banked road
ginside=GM(R−d)R3g_{\mathrm{inside}}=\frac{GM(R-d)}{R^3}
Gravitational acceleration at depth d
gsurface=GMR2g_{\mathrm{surface}}=\frac{GM}{R^2}
Gravitational acceleration at Earth surface
goutside=GM(R+h)2g_{\mathrm{outside}}=\frac{GM}{(R+h)^2}
Gravitational acceleration at height h

Unit XVI · Nuclear physics

Nucleus, decay & radiation dose

FormulaUse
R=R0A1/3R=R_0 A^{1/3}
Nuclear radius
V=43πR03AV=\frac{4}{3}\pi R_0^3 A
Nuclear volume
Activity A=−ΔNΔt=λN\text{Activity } A=-\frac{\Delta N}{\Delta t}=\lambda N
Activity and decay rate
N=N0e−λt=N0(12)nN=N_0 e^{-\lambda t}=N_0\left(\frac{1}{2}\right)^n
Undecayed nuclei
Ndecayed=N0[1−(12)n]N_{\mathrm{decayed}}=N_0\left[1-\left(\frac{1}{2}\right)^n\right]
Nuclei decayed after n half-lives
n=tT1/2n=\frac{t}{T_{1/2}}
Number of half-lives
λ=ln⁡2T1/2=0.693T1/2\lambda=\frac{\ln 2}{T_{1/2}}=\frac{0.693}{T_{1/2}}
Decay constant
τ=1λ=T1/2ln⁡2\tau=\frac{1}{\lambda}=\frac{T_{1/2}}{\ln 2}
Mean life
D=EmD=\frac{E}{m}
Absorbed dose
Dequivalent=Dabsorbed×RBED_{\mathrm{equivalent}}=D_{\mathrm{absorbed}}\times\mathrm{RBE}
Equivalent dose
α:ZAX→Z−2A−4Y+24He\alpha:\quad {}^{A}_{Z}\mathrm{X}\rightarrow{}^{A-4}_{Z-2}\mathrm{Y}+{}^{4}_{2}\mathrm{He}
Alpha decay
β−:ZAX→Z+1AY+−10e+νˉ\beta^-:\quad {}^{A}_{Z}\mathrm{X}\rightarrow{}^{A}_{Z+1}\mathrm{Y}+{}^{0}_{-1}\mathrm{e}+\bar{\nu}
Beta-minus decay
β+:ZAX→Z−1AY++10e+ν\beta^+:\quad {}^{A}_{Z}\mathrm{X}\rightarrow{}^{A}_{Z-1}\mathrm{Y}+{}^{0}_{+1}\mathrm{e}+\nu
Beta-plus decay
γ:ZAX∗→ZAX+00γ\gamma:\quad {}^{A}_{Z}\mathrm{X}^{*}\rightarrow{}^{A}_{Z}\mathrm{X}+{}^{0}_{0}\gamma
Gamma decay

Unit XII · Alternating current

Alternating current

FormulaUse
V=V0sin⁡ωtV=V_0\sin\omega t
I=I0sin⁡ωtI=I_0\sin\omega t
Instantaneous AC voltage and current
Vrms=V02V_{\mathrm{rms}}=\frac{V_0}{\sqrt{2}}
Irms=I02I_{\mathrm{rms}}=\frac{I_0}{\sqrt{2}}
RMS values
θ=ωt=2πft=2πTt\theta=\omega t=2\pi ft=\frac{2\pi}{T}t
Phase of AC
c=1ε0μ0c=\frac{1}{\sqrt{\varepsilon_0\mu_0}}
cmedium=cnc_{\mathrm{medium}}=\frac{c}{n}
Speed of light in vacuum / medium
Z=R2+(XL−XC)2Z=\sqrt{R^2+(X_L-X_C)^2}
Impedance of a series RLC circuit
XC=1ωC=12πfCX_C=\frac{1}{\omega C}=\frac{1}{2\pi fC}
Capacitive reactance
XL=ωL=2πfLX_L=\omega L=2\pi fL
Inductive reactance
Pav=VrmsIrmscos⁡ϕ=V0I02cos⁡ϕP_{\mathrm{av}}=V_{\mathrm{rms}}I_{\mathrm{rms}}\cos\phi=\frac{V_0I_0}{2}\cos\phi
Average power in AC circuit
Power factor=cos⁡ϕ\text{Power factor}=\cos\phi
Power factor
Pav=0P_{\mathrm{av}}=0
Average power in a pure capacitor or inductor

Unit VII · Waves & oscillations

SHM, waves, sound & optics

FormulaUse
F⃗∝−x⃗\vec{F}\propto-\vec{x}
a⃗∝−x⃗\vec{a}\propto-\vec{x}
a=−ω2xa=-\omega^2x
Restoring force and acceleration in SHM
S in one vibration=4A\text{S in one vibration}=4A
T=1fT=\frac{1}{f}
ω=2πf\omega=2\pi f
Basic SHM relations
x=x0sin⁡ωtx=x_0\sin\omega t
v=v0cos⁡ωtv=v_0\cos\omega t
SHM starting from mean position
x=x0cos⁡ωtx=x_0\cos\omega t
v=−v0sin⁡ωtv=-v_0\sin\omega t
SHM starting from extreme position
PE=12kx2\mathrm{PE}=\frac{1}{2}kx^2
KE=12kx02(1−x2x02)\mathrm{KE}=\frac{1}{2}kx_0^2\left(1-\frac{x^2}{x_0^2}\right)
Energy in SHM
v=fλv=f\lambda
wave number=1λ\text{wave number}=\frac{1}{\lambda}
Wave equation and wave number
I∝A2I\propto A^2
A∝IA\propto\sqrt{I}
Intensity–amplitude relation
v=Fμv=\sqrt{\frac{F}{\mu}}
Speed of transverse wave on a string
v=Eρv=\sqrt{\frac{E}{\rho}}
Speed of longitudinal wave
λde Broglie=hp=hmv=h2m KE\lambda_{\text{de Broglie}}=\frac{h}{p}=\frac{h}{mv}=\frac{h}{\sqrt{2m\,\mathrm{KE}}}
de Broglie wavelength
n=cvn=\frac{c}{v}
n1sin⁡θ1=n2sin⁡θ2n_1\sin\theta_1=n_2\sin\theta_2
Refractive index and Snell's law
vsound=γPρv_{\mathrm{sound}}=\sqrt{\frac{\gamma P}{\rho}}
γ=CpCv\gamma=\frac{C_p}{C_v}
Laplace formula for speed of sound
vtv0=TT0\frac{v_t}{v_0}=\sqrt{\frac{T}{T_0}}
vt=v0+0.61tv_t=v_0+0.61t
Speed of sound versus temperature

Unit XI · Electromagnetism

Induction, transformers & generator

FormulaUse
ε=−ΔΦΔt\varepsilon=-\frac{\Delta\Phi}{\Delta t}
ε=−NΔΦΔt\varepsilon=-\frac{N\Delta\Phi}{\Delta t}
Induced EMF (Faraday's law)
I=−NΔΦRΔtI=-\frac{N\Delta\Phi}{R\Delta t}
q=−NΔΦRq=-\frac{N\Delta\Phi}{R}
Induced current and charge
ε=−vBLsin⁡θ\varepsilon=-vBL\sin\theta
Motional EMF
Flux linkage=NΦ=NBAcos⁡θ\text{Flux linkage}=N\Phi=NBA\cos\theta
Flux linkage
M=NsΦsIp=−εΔIp/ΔtM=\frac{N_s\Phi_s}{I_p}=-\frac{\varepsilon}{\Delta I_p/\Delta t}
Mutual inductance
L=NΦI=−εΔI/ΔtL=\frac{N\Phi}{I}=-\frac{\varepsilon}{\Delta I/\Delta t}
Self inductance
NsNp=VsVp=IpIs\frac{N_s}{N_p}=\frac{V_s}{V_p}=\frac{I_p}{I_s}
Ideal transformer ratios
VsIs=VpIpV_s I_s=V_p I_p
Ideal transformer power relation
η=PoutPin×100\eta=\frac{P_{\mathrm{out}}}{P_{\mathrm{in}}}\times100
Transformer efficiency
ε=NωABsin⁡θ\varepsilon=N\omega AB\sin\theta
ε0=NωAB\varepsilon_0=N\omega AB
Instantaneous and maximum generator EMF
I=εR=ε0sin⁡θRI=\frac{\varepsilon}{R}=\frac{\varepsilon_0\sin\theta}{R}
I0=ε0RI_0=\frac{\varepsilon_0}{R}
Generator current

Unit II · Force & motion

Projectile motion

FormulaUse
h=12gt2h=\frac{1}{2}gt^2
Vertical drop / height from rest
vx=ucos⁡θv_x=u\cos\theta
vy=usin⁡θ−gtv_y=u\sin\theta-gt
Projectile velocity components
tto summit=2Hg=usin⁡θgt_{\text{to summit}}=\sqrt{\frac{2H}{g}}=\frac{u\sin\theta}{g}
Time to maximum height
H=u2sin⁡2θ2gH=\frac{u^2\sin^2\theta}{2g}
Maximum height of projectile
R=u2sin⁡2θgR=\frac{u^2\sin2\theta}{g}
Range on level ground
T=2usin⁡θgT=\frac{2u\sin\theta}{g}
Time of flight
KEsummit=KEinitialcos⁡2θ\mathrm{KE}_{\mathrm{summit}}=\mathrm{KE}_{\mathrm{initial}}\cos^2\theta
Kinetic energy at summit
PEsummit=KEinitialsin⁡2θ\mathrm{PE}_{\mathrm{summit}}=\mathrm{KE}_{\mathrm{initial}}\sin^2\theta
Potential energy at summit
Rtan⁡θ=4HR\tan\theta=4H
Rtan⁡θ=12gT2R\tan\theta=\frac{1}{2}gT^2
H=gT28H=\frac{gT^2}{8}
Useful range–height–time relations

Unit XIV · Dawn of modern physics

Relativity, photons & photoelectric effect

FormulaUse
t=t01−v2c2t=\frac{t_0}{\sqrt{1-\frac{v^2}{c^2}}}
Time dilation
l=l01−v2c2l=l_0\sqrt{1-\frac{v^2}{c^2}}
Length contraction
λ=hp=hmv=h2m KE=h2mqV\lambda=\frac{h}{p}=\frac{h}{mv}=\frac{h}{\sqrt{2m\,\mathrm{KE}}}=\frac{h}{\sqrt{2mqV}}
de Broglie wavelength
E=hf=hcλE=hf=\frac{hc}{\lambda}
Photon energy
P=n(hft)=nhcλtP=n\left(\frac{hf}{t}\right)=\frac{nhc}{\lambda t}
Power of n photons
E(eV)=12400λ(A˚)=1240λ(nm)E(\mathrm{eV})=\frac{12400}{\lambda(\mathring{\mathrm{A}})}=\frac{1240}{\lambda(\mathrm{nm})}
Photon energy from wavelength
Δλ=hm0c(1−cos⁡θ)\Delta\lambda=\frac{h}{m_0c}(1-\cos\theta)
Compton shift
ϕ=hf0=hcλ0\phi=hf_0=\frac{hc}{\lambda_0}
Work function
hf=ϕ+12mvmax2hf=\phi+\frac{1}{2}mv_{\mathrm{max}}^2
eV0=hf−ϕeV_0=hf-\phi
Einstein photoelectric equation
vmax=6×105V0v_{\mathrm{max}}=6\times10^5\sqrt{V_0}
Maximum photoelectron speed from stopping potential

Unit VI · Fluid dynamics

Fluid dynamics

FormulaUse
Q=ΔVΔt=AvQ=\frac{\Delta V}{\Delta t}=Av
Volume flow rate
m˙=ΔmΔt=ρAv\dot{m}=\frac{\Delta m}{\Delta t}=\rho Av
Mass flow rate
A1v1=A2v2A_1v_1=A_2v_2
Q1=Q2Q_1=Q_2
Continuity equation
Re=ρvDμ\mathrm{Re}=\frac{\rho vD}{\mu}
Reynolds number
F=6πμrvF=6\pi\mu rv
Stokes’ law
P=ρghP=\rho gh
Fluid pressure at depth h
vt=2gr2ρ9μv_t=\frac{2gr^2\rho}{9\mu}
Terminal velocity of a small sphere
P+12ρv2+ρgh=constantP+\frac{1}{2}\rho v^2+\rho gh=\text{constant}
Bernoulli equation
vefflux=2ghv_{\mathrm{efflux}}=\sqrt{2gh}
Efflux speed (Torricelli)
Q=πr4ΔP8ηLQ=\frac{\pi r^4\Delta P}{8\eta L}
Poiseuille’s law

Unit VII · Waves & oscillations

Stationary waves & Doppler effect

FormulaUse
λn=2Ln\lambda_n=\frac{2L}{n}
fn=nv2L=nf1f_n=\frac{nv}{2L}=nf_1
String fixed at both ends
f1=12LFμf_1=\frac{1}{2L}\sqrt{\frac{F}{\mu}}
Fundamental frequency of a string
Open pipe:λn=2Ln\text{Open pipe:}\quad\lambda_n=\frac{2L}{n}
fn=nv2Lf_n=\frac{nv}{2L}
Open air column
Closed pipe:λn=4Ln\text{Closed pipe:}\quad\lambda_n=\frac{4L}{n}
fn=nv4L,n oddf_n=\frac{nv}{4L},\quad n\text{ odd}
Closed air column
v′=v±vwv'=v\pm v_w
Speed of sound with/against wind
fa=f0(v±vov∓vs)f_a=f_0\left(\frac{v\pm v_o}{v\mp v_s}\right)
General Doppler formula (choose signs for approach)
Δλλ0=vsc\frac{\Delta\lambda}{\lambda_0}=\frac{v_s}{c}
Doppler shift for light at low speeds

Unit I · Vectors & equilibrium

Vectors

FormulaUse
∣r⃗∣=a2+b2|\vec{r}|=\sqrt{a^2+b^2}
∣r⃗∣=a2+b2+c2|\vec{r}|=\sqrt{a^2+b^2+c^2}
Magnitude in 2D / 3D
r⃗=aı^+bȷ^  (+ck^)\vec{r}=a\hat{\imath}+b\hat{\jmath}\;(+c\hat{k})
Position vector
Rx=Rcos⁡θR_x=R\cos\theta
Ry=Rsin⁡θR_y=R\sin\theta
Rectangular components
R=Rx2+Ry2R=\sqrt{R_x^2+R_y^2}
θ=tan⁡−1(RyRx)\theta=\tan^{-1}\left(\frac{R_y}{R_x}\right)
Resultant magnitude and direction
R=A2+B2+2ABcos⁡θR=\sqrt{A^2+B^2+2AB\cos\theta}
Law of cosines for vector resultant
A⃗⋅B⃗=ABcos⁡θ=AxBx+AyBy+AzBz\vec{A}\cdot\vec{B}=AB\cos\theta=A_xB_x+A_yB_y+A_zB_z
Dot product
A⃗×B⃗=ABsin⁡θ n^\vec{A}\times\vec{B}=AB\sin\theta\,\hat{n}
Cross product

Unit II · Force & motion

Kinematics, momentum & horizontal projectiles

FormulaUse
v⃗av=Δd⃗Δt\vec{v}_{\mathrm{av}}=\frac{\Delta\vec{d}}{\Delta t}
v=ΔSΔtv=\frac{\Delta S}{\Delta t}
aav=ΔvΔta_{\mathrm{av}}=\frac{\Delta v}{\Delta t}
Velocity, speed and acceleration
vf=vi+atv_f=v_i+at
S=vit+12at2S=v_it+\frac{1}{2}at^2
vf2−vi2=2aSv_f^2-v_i^2=2aS
Equations of motion
F⃗=ma⃗=Δp⃗Δt\vec{F}=m\vec{a}=\frac{\Delta\vec{p}}{\Delta t}
J⃗=F⃗Δt=Δp⃗\vec{J}=\vec{F}\Delta t=\Delta\vec{p}
Newton’s second law and impulse
p⃗=mv⃗\vec{p}=m\vec{v}
m1u1+m2u2=m1v1+m2v2m_1u_1+m_2u_2=m_1v_1+m_2v_2
Momentum and its conservation
Ffriction=μsNF_{\mathrm{friction}}=\mu_s N
Limiting static friction
U=mghU=mgh
gravitational potential=gh\text{gravitational potential}=gh
Gravitational potential energy / potential
vfx=viv_{fx}=v_i
vfy=gtv_{fy}=gt
vf=vfx2+vfy2v_f=\sqrt{v_{fx}^2+v_{fy}^2}
Horizontal projectile motion
θ=tan⁡−1(vfyvfx)\theta=\tan^{-1}\left(\frac{v_{fy}}{v_{fx}}\right)
R=vtR=vt
Direction and range of horizontal projectile

Unit III · Work & energy

Work, energy & power

FormulaUse
W=Fdcos⁡θW=Fd\cos\theta
W=τωW=\tau\omega
Work in linear / rotational motion
W=PΔVW=P\Delta V
Pressure–volume work
Wspring=12kx2W_{\mathrm{spring}}=\frac{1}{2}kx^2
Einductor=12LI2E_{\mathrm{inductor}}=\frac{1}{2}LI^2
Stored energy in spring / inductor
KE=12mv2=12pv=p22m\mathrm{KE}=\frac{1}{2}mv^2=\frac{1}{2}pv=\frac{p^2}{2m}
Kinetic energy forms
Fd=12m(vf2−vi2)Fd=\frac{1}{2}m(v_f^2-v_i^2)
Fd=mg(h2−h1)Fd=mg(h_2-h_1)
Work–energy principle
v=2ghv=\sqrt{2gh}
Speed after falling through height h in vacuum
U=−GMmrU=-\frac{GMm}{r}
Vgrav=−GMrV_{\mathrm{grav}}=-\frac{GM}{r}
Gravitational potential energy / potential
P=Wt=Fvcos⁡θ=τωP=\frac{W}{t}=Fv\cos\theta=\tau\omega
Power
η=outputinput×100\eta=\frac{\text{output}}{\text{input}}\times100
Efficiency

Unit XV · Atomic spectra

Bohr model & atomic spectra

FormulaUse
rn=n2a0Zr_n=\frac{n^2a_0}{Z}
Radius of nth Bohr orbit for hydrogen-like atom
En=−13.6Z2n2 eVE_n=-\frac{13.6Z^2}{n^2}\,\mathrm{eV}
Energy of nth Bohr orbit
vn=2.18×106Zn m s−1v_n=2.18\times10^6\frac{Z}{n}\,\mathrm{m\,s^{-1}}
Electron speed in nth orbit
Ln=nh2πL_n=\frac{nh}{2\pi}
Angular momentum quantisation
KE=ke22rn\mathrm{KE}=\frac{ke^2}{2r_n}
PE=−ke2rn\mathrm{PE}=-\frac{ke^2}{r_n}
TE=−ke22rn\mathrm{TE}=-\frac{ke^2}{2r_n}
Energy relations in Bohr orbit
f∝Z2n3f\propto\frac{Z^2}{n^3}
T∝n3Z2T\propto\frac{n^3}{Z^2}
Orbital frequency and period trends
νˉ=RH(1p2−1n2)\bar{\nu}=R_H\left(\frac{1}{p^2}-\frac{1}{n^2}\right)
Rydberg wavenumber relation
λlimit=p2RH\lambda_{\mathrm{limit}}=\frac{p^2}{R_H}
Series-limit wavelength
Nmax=(n−p+1)(n−p)2N_{\mathrm{max}}=\frac{(n-p+1)(n-p)}{2}
Maximum transitions between two orbits

Unit IX · Current electricity

Current electricity

FormulaUse
I=ΔQΔt=neΔtI=\frac{\Delta Q}{\Delta t}=\frac{ne}{\Delta t}
I=feI=fe
Electric current
vd=InAev_d=\frac{I}{nAe}
Drift velocity
V=IRV=IR
R=ρLAR=\frac{\rho L}{A}
G=σALG=\frac{\sigma A}{L}
Ohm’s law, resistance and conductance
R=ρL2V=ρVA2R=\frac{\rho L^2}{V}=\frac{\rho V}{A^2}
Resistance forms using volume
Rt=R0(1+αΔT)R_t=R_0(1+\alpha\Delta T)
ρt=ρ0(1+αΔT)\rho_t=\rho_0(1+\alpha\Delta T)
Temperature dependence
P=IV=V2R=I2RP=IV=\frac{V^2}{R}=I^2R
Electric power
Eheat=V2tR=I2RtE_{\mathrm{heat}}=\frac{V^2t}{R}=I^2Rt
Electrical energy / heat
Rseries=R1+R2+⋯R_{\mathrm{series}}=R_1+R_2+\cdots
1Rparallel=1R1+1R2+⋯\frac{1}{R_{\mathrm{parallel}}}=\frac{1}{R_1}+\frac{1}{R_2}+\cdots
Equivalent resistance
Vn=V(RnRtotal)V_n=V\left(\frac{R_n}{R_{\mathrm{total}}}\right)
In=I(ReqRn)I_n=I\left(\frac{R_{\mathrm{eq}}}{R_n}\right)
Voltage divider and current divider
Eseries=E1+E2+⋯E_{\mathrm{series}}=E_1+E_2+\cdots
rseries=r1+r2+⋯r_{\mathrm{series}}=r_1+r_2+\cdots
Cells in series