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[QUICK DESCRIPTION] Physical quantities and models need to be dimensionally consistent. See also [[dimensional analysis]]. [PREREQUISITES] Calculus, basic algebra [EXAMPLE] From Newton's second law and basic assumptions, we might have derived the equation for a spring acting under gravity: [maths] m\frac{d^2 y}{dt^2} = -mg - ky [/maths] where $y(t)$ is the height of the mass, $m$ its mass, $k$ the spring constant of the spring, $g$ is the gravitational acceleration at the Earth's surface, and $t$ is (of course) time. Only quantities with the same dimensional units can be added. The dimensional units of a product is the product of the dimensional units: $[pq]=[p]\,[q]$. [GENERAL DISCUSSION] The quantity $g$ must have the units of acceleration. If we use $[q]$ to denote the physical units of a quantity $q$, then $[t]=T$ ($T$ representing the units of time), $[m]=M$ (representing the units of mass), and $[y]=L$ (representing the units of length). Thus the dimensional units of $g$ are $[g]=L T^{-2}$. The spring constant $k$ must have units $[k]=M T^{-2}$. If we are looking for the period of oscillation of the spring-mass system, then we need to look for something that has units $T$. Since $y(t)$ is an a priori unknown function of $t$, our period must depend only on the other quantities: $m$, $k$, $g$. Now $[m^\alpha k^\beta g^\gamma]=T$ means that $M^\alpha(M T^{-2})^\beta(L T^{-2})^\gamma=T$. Since $M$, $L$ and $T$ are independent units, this comes down to the equations for $M$: $\alpha+\beta=0$, for $L$: $\gamma=0$, and for $T$: $-2\beta-2\gamma=1$. This has the solution $\alpha=1/2$, $\beta=-1/2$ and $\gamma=0$. Thus we should be looking for a dimensionless multiple of $\sqrt{m/k}$. Indeed the period is $2\pi\sqrt{m/k}$.
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