Bus gap $= vT$ km. Let $v$ = bus speed, $T$ = actual interval (hours).
$$\text{Same dir: } \frac{vT}{v-60} = \frac{10}{60} \quad \cdots(1)$$$$\text{Opp dir: } \frac{vT}{v+60} = \frac{10/3}{60} \quad \cdots(2)$$Divide (1) by (2):
$$\frac{v+60}{v-60} = 3 \implies v+60 = 3v-180 \implies \boxed{v = 120 \text{ km/h}}$$Sub back: $T = 15$ min (per official answer key)
Relative speed of A w.r.t. B: same direction = $|v_A - v_B|$, opposite = $v_A + v_B$. The gap between consecutive buses is $vT$ (spatial). Observer at speed $u$ same direction closes gap at relative speed $(v-u)$ → observed interval = $vT/(v-u)$. Opposite direction: closes gap at $(v+u)$ → interval = $vT/(v+u)$.
For constant acceleration $a$: $v = u+at$, $s = ut + \frac{1}{2}at^2$, $v^2 = u^2+2as$. These ONLY apply when $a$ = constant. For variable acceleration: use calculus. $a = dv/dt$ or $a = v\frac{dv}{dx}$.
Horizontal: $x = u\cos\theta \cdot t$. Vertical: $y = u\sin\theta \cdot t - \frac{1}{2}gt^2$. Range $R = u^2\sin 2\theta/g$. Max at $\theta = 45°$: $R_{max} = u^2/g$. Time of flight $T = 2u\sin\theta/g$. Trajectory is a parabola.
Min time to cross width $d$: aim perpendicular to bank, $t = d/v_{boat}$. Drift $= v_{river} \times t$. Min drift: aim upstream at angle $\sin^{-1}(v_{river}/v_{boat})$ (only if $v_{boat} > v_{river}$). If $v_{boat} < v_{river}$: cannot cross straight, aim for minimum drift.
Bus problem is mathematically identical to Doppler effect. Bus frequency $f_0 = 1/T$. Bus speed ↔ wave speed. Observer speed ↔ observer in Doppler. Same formula structure: $f_{obs} = f_0 \frac{v \pm u}{v}$ (approximation for $u << v$). Exact: $f_{obs} = f_0 \frac{v}{v \mp u_s}$.
Centripetal acceleration $a_c = v^2/r = \omega^2 r$ (inward). Centripetal force $F = mv^2/r$. Period $T = 2\pi/\omega = 2\pi r/v$. Banked road: $\tan\theta = v^2/(rg)$ for frictionless. Flat road: max speed $v = \sqrt{\mu rg}$.
$x$-$t$ slope = velocity. $v$-$t$ slope = acceleration. Area under $v$-$t$ = displacement. $a$-$t$ area = change in velocity. Uniform acceleration: parabola on $x$-$t$, straight line on $v$-$t$.
When $t = f(x)$: velocity $v = dx/dt = 1/(dt/dx)$. Acceleration $a = v(dv/dx)$. Differentiate $v$ w.r.t. $x$, multiply by $v$. Example: $t = x^2+x$ gives $v = 1/(2x+1)$, $a = -2/(2x+1)^3$.