Physics Lab
JEE/Unit 2: Kinematics/1D Kinematics by Calculus

1D Kinematics by Calculus

Most JEE motion problems are not constant-acceleration cookbook exercises. When aa depends on tt, on vv or on xx, you must use calculus: differentiation gives instantaneous rates, integration gives accumulated change.

Concept

For a particle on a line at position x(t)x(t):

  • Velocity v=dxdtv = \dfrac{\mathrm{d}x}{\mathrm{d}t}.
  • Acceleration a=dvdt=d2xdt2a = \dfrac{\mathrm{d}v}{\mathrm{d}t} = \dfrac{\mathrm{d}^{2}x}{\mathrm{d}t^{2}}.
  • Chain rule trick: a=vdvdxa = v\dfrac{\mathrm{d}v}{\mathrm{d}x}, useful when aa depends on xx.

For constant acceleration, integrating gives the standard kinematics: v=u+at,x=ut+12at2,v2=u2+2ax.v = u + at,\qquad x = ut + \tfrac{1}{2}at^{2},\qquad v^{2} = u^{2} + 2ax.

Displacement = ∫v dt\int v\,\mathrm{d}t; change of velocity = ∫a dt\int a\,\mathrm{d}t; area under vv-tt graph = displacement; area under aa-tt graph = velocity change.

Derivation

Suppose a=−kva = -k v (linear drag). Then dvdt=−kv\dfrac{\mathrm{d}v}{\mathrm{d}t} = -k v separates as ∫uvdvv=−k∫0tdt⇒v=ue−kt.\int_{u}^{v} \frac{\mathrm{d}v}{v} = -k\int_{0}^{t}\mathrm{d}t \Rightarrow v = u e^{-k t}. Position follows from another integration: x(t)=uk(1−e−kt)x(t) = \dfrac{u}{k}(1 - e^{-k t}). As t→∞t\to\infty, x→u/kx\to u/k (asymptotic stop).

If aa depends on xx, e.g. a=−ω2xa = -\omega^{2} x (SHM), use v dv=a dxv\,\mathrm{d}v = a\,\mathrm{d}x: ∫v dv=∫−ω2x dx⇒v2=ω2(A2−x2).\int v\,\mathrm{d}v = \int -\omega^{2} x\,\mathrm{d}x \Rightarrow v^{2} = \omega^{2}(A^{2} - x^{2}).

JEE Worked Example

Q. A particle starts from rest with a(t)=6t m s−2a(t) = 6t\,\text{m s}^{-2}. Find its velocity and position at t=4 st = 4\,\text{s}.

Solution. v=∫0t6t′ dt′=3t2v = \int_{0}^{t} 6t'\,\mathrm{d}t' = 3 t^{2}. So v(4)=48 m s−1v(4) = 48\,\text{m s}^{-1}.

x=∫0t3t′2 dt′=t3x = \int_{0}^{t} 3 t'^{2}\,\mathrm{d}t' = t^{3}. So x(4)=64 mx(4) = 64\,\text{m}.

Traps

  • Using v=u+atv = u + at when aa is variable.
  • Confusing average velocity (Δx/Δt\Delta x/\Delta t) with average speed (total distance/Δt\Delta t).
  • Forgetting initial conditions when integrating.
  • Sign errors during deceleration; choose a fixed positive direction.

Key Takeaways

  • v=dx/dtv = \mathrm{d}x/\mathrm{d}t, a=dv/dt=v dv/dxa = \mathrm{d}v/\mathrm{d}t = v\,\mathrm{d}v/\mathrm{d}x.
  • Area under vv-tt graph == displacement (signed).
  • Pick the integration variable that matches the dependence of aa.

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