$\therefore[\text{ML}^2\text{T}^3\text{I}^{-1}]=[\text{ML}^2\text{T}^{-3}\text{I}^{-2}][\text{I}]$
$\Rightarrow\text{V = IR}$
16 questions · self-marked practice — reveal the answer and mark yourself.
$\therefore[\text{ML}^2\text{T}^3\text{I}^{-1}]=[\text{ML}^2\text{T}^{-3}\text{I}^{-2}][\text{I}]$
$\Rightarrow\text{V = IR}$
Electric dipole moment $\text{P = qI = [IT]}\times[\text{L] = [LTI}]$
Magnetic dipole moment $\text{M = IA}=[\text{I][L}^2]=[\text{L}^2\text{I}]$
$\text{h}=\frac{\text{E}}{\text{v}}=\frac{[\text{ML}^2\text{T}^{-2}]}{[\text{T}^{-1}]}[\text{ML}^2\text{T}^{-1}]$
$\text{F = qE, F = qvB,}$ and $\text{B}=\frac{\mu_0\text{I}}{2\pi\alpha};$
where F is force, q is charge, v is speed, I is current, and a is distance.Electric field $\text{E}=\frac{\text{F}}{\text{q}}=\frac{\text{MLT}^{-2}}{[\text{lT}]}=[\text{MLT}^{-3}\text{l}^{-2}]$
Magnetic field $\text{B}=\frac{\text{F}}{\text{qv}}=\frac{\text{MLT}^{-2}}{[\text{lT}][\text{LT}^{-1}]}=[\text{MT}^{-2}\text{l}^{-1}]$
Magnetic permeability $\mu_0=\frac{\text{B}\times2\pi\text{a}}{\text{l}}=\frac{[\text{MT}^{-2}\text{l}^{-1}]\times[\text{L}]}{[\text{l}]}=[\text{MLT}^{-2}\text{l}^{-2}]$
Using the lunar year, Earth's year and distance between earth and moon.
Linear momentum: $\text{mv}=[\text{MLT}^{-1}]$
Frequency: $\frac{1}{\text{T}}=[\text{M}^0\text{L}^0\text{T}^{-1}]$
Pressure: $\frac{\text{Force}}{\text{Area}}=\frac{[\text{MLT}^{-2}]}{\text{[L}^2]}=[\text{ML}^{-1}\text{T}^{-2}]$
$\text{Q = mc(T}_2-\text{T}_1),\text{l}_{\text{t}}=\text{l}_0[1+\alpha(\text{T}_2-\text{T}_1)]$ and $\text{PV = nRT}.$
Specific heat capacity $=\text{C}=\frac{\text{Q}}{\text{m}\triangle\text{T}}=\frac{\text{ML}^2\text{T}^{-2}}{[\text{M}][\text{k}]}=[\text{L}^2\text{T}^{-2}\text{K}^{-1}]$
Coefficient of linear expansion $=\alpha=\frac{\text{L}_{1}-\text{L}_{2}}{\text{L}_0\triangle\text{T}}=\frac{[\text{L}]}{[\text{L}][\text{R}]}=[\text{k}^{-1}]$
Gas constant $=\text{R}=\frac{\text{PV}}{\text{nT}}=\frac{[\text{ML}^{-1}\text{T}^{-2}][\text{L}^3]}{[(\text{mol})][\text{k}]}=[\text{ML}^2\text{T}^{-2}\text{k}^{-1}(\text{mol})^{-1}]$
$\omega=\frac{\theta_2-\theta_1}{\text{t}_2-\text{t}_1},\alpha=\frac{\omega_2-\omega_1}{\text{t}_2-\text{t}_1},\tau=\text{F.r}$ and $\text{I = mr}^2.$
The symbols have standard meanings.
Angular speed $\omega=\frac{\theta}{\text{t}}=[\text{M}^0\text{L}^0\text{T}^{-1}]$
Angular acceleration $\alpha=\frac{\omega}{\text{t}}=\frac{\text{M}^0\text{L}^0\text{T}^{-1}}{\text{T}}=[\text{M}^0\text{L}^0\text{T}^{-2}]$
Torque $\tau=\text{Fr}=[\text{MLT}^{-2}][\text{L] = [ML}^2\text{T}^{-2}]$
Moment of inertia $=\text{Mr}^2=[\text{M}][\text{L}^2]=[\text{ML}^2\text{T}^0]$
$\therefore$ l = ct.
$\text{Density}=\frac{\text{m}}{\text{V}}=\frac{\big(\frac{\text{force}}{\text{acceleration}}\big)}{\text{Volume}}\\=\frac{\big[\frac{\text{F}}{\text{LT}}^{-2}\big]}{[\text{L}^{2}]}=\frac{\text{F}}{\text{L}^4\text{T}^{-2}}=[\text{FL}^{-4}\text{T}^{2}]$
$\text{Pressure}=\frac{\text{F}}{\text{A}}=\frac{\text{F}}{\text{L}^2}=[\text{FL}^{-2}]$
$\text{Momentum = mv (Force I acceleration)}\times\text{Velocity}\\=\Big[\frac{\text{F}}{\text{LT}^{-2}}\Big]\times[\text{LT}^{-1}]=[\text{FT}]$
$\text{Energy}=\frac{1}{2}\text{mv}^2=\frac{\text{Force}}{\text{acceleration}}\times\text{(velocty)}^2$
$=\Big[\frac{\text{F}}{\text{LT}^{-2}}\Big]\times[\text{LT}^{-1}]^2=\Big[\frac{\text{F}}{\text{LT}^{-2}}\Big]\times[\text{L}^2\text{T}^{-2}]=[\text{FL}]$