1D Kinematics by Calculus
Most JEE motion problems are not constant-acceleration cookbook exercises. When a depends on t, on v or on x, you must use calculus: differentiation gives instantaneous rates, integration gives accumulated change.
Concept
For a particle on a line at position x(t):
- Velocity v=dtdx.
- Acceleration a=dtdv=dt2d2x.
- Chain rule trick: a=vdxdv, useful when a depends on x.
For constant acceleration, integrating gives the standard kinematics:
v=u+at,x=ut+21at2,v2=u2+2ax.
Displacement = ∫vdt; change of velocity = ∫adt; area under v-t graph = displacement; area under a-t graph = velocity change.
Derivation
Suppose a=−kv (linear drag). Then dtdv=−kv separates as
∫uvvdv=−k∫0tdt⇒v=ue−kt.
Position follows from another integration: x(t)=ku(1−e−kt). As t→∞, x→u/k (asymptotic stop).
If a depends on x, e.g. a=−ω2x (SHM), use vdv=adx:
∫vdv=∫−ω2xdx⇒v2=ω2(A2−x2).
JEE Worked Example
Q. A particle starts from rest with a(t)=6tm s−2. Find its velocity and position at t=4s.
Solution. v=∫0t6t′dt′=3t2. So v(4)=48m s−1.
x=∫0t3t′2dt′=t3. So x(4)=64m.
Traps
- Using v=u+at when a is variable.
- Confusing average velocity (Δx/Δt) with average speed (total distance/Δt).
- Forgetting initial conditions when integrating.
- Sign errors during deceleration; choose a fixed positive direction.
Key Takeaways
- v=dx/dt, a=dv/dt=vdv/dx.
- Area under v-t graph = displacement (signed).
- Pick the integration variable that matches the dependence of a.