Motion in a straight line — the kinematic equations that define it, and the traps that cost marks on them.
NCERT Class 11 Physics Chapter 2 (page 1) defines the framework: an object moving along a straight line has its position described by a single coordinate. Displacement is the change in that coordinate (a signed quantity), while distance is the total path length (always non-negative). This distinction between vector displacement and scalar distance is the root of half the traps in this topic.
The three kinematic equations (NCERT Chapter 2, pages 4–6) apply strictly when acceleration is constant:
- v = v₀ + at
- x − x₀ = v₀t + ½at²
- v² = v₀² + 2a(x − x₀)
A high-frequency trap: applying these equations when acceleration varies with time or position. If a problem states acceleration changes, you must integrate — the kinematic equations are off-limits.
Galileo's odd-number rule. For an object starting from rest under constant acceleration, distances covered in successive equal time intervals follow the ratio 1 : 3 : 5 : 7 : … A common mistake is writing 1 : 2 : 3 : 4 (linear), which ignores that displacement grows as t².
Non-zero initial velocity. When a problem says an object is "thrown downward" or "projected with speed u," that u must appear in the equation. Writing v² = 2gh instead of v² = u² + 2gh drops the u² term and produces a wrong answer — a distractor that appears regularly in NEET papers.
Implicit-function kinematics. When time is given as a function of position (e.g., t = x² + x), don't try to algebraically invert for x(t). Differentiate directly: v = dx/dt = 1/(dt/dx), then use the chain rule a = v(dv/dx) for acceleration.
The v² insight. Under uniform deceleration, kinetic energy (proportional to v²) drops linearly with distance. Speed itself does not. Treating the speed ratio as the distance ratio is a trap that costs marks in multi-stage deceleration problems.