Motion in a Plane — Exam Practice
Practice questions in CBSE, NEET, and JEE Main style covering vector addition, projectile motion, and uniform circular motion.
1CBSE Board Exam Style
At the highest point, the vertical velocity component is momentarily zero, leaving only the horizontal component — velocity is horizontal. Acceleration (g) is always vertical, downward. So velocity is exactly perpendicular to acceleration at that instant.
Vertical motion: initial vertical velocity = u sinθ, acceleration = −g. The projectile returns to the launch height when net vertical displacement is zero:
0 = (u sinθ)t − ½gt² → t[u sinθ − ½gt] = 0.
The nonzero solution: t = 2u sinθ / g.
(a) R = (horizontal velocity) × (time of flight) = (u cosθ)(2u sinθ/g) = u²(2 sinθ cosθ)/g = u² sin(2θ)/g.
Since sin(2θ) has a maximum value of 1 at 2θ = 90° (θ = 45°), range is maximum at exactly 45°.
(b) R = u²sin(2θ)/g = (400 × sin60°)/10 = (400 × 0.866)/10 ≈ 34.6 m.
2NEET Style (Single-Correct MCQ)
R = √(A²+A²+2A²cos120°) = √(2A² − A²) = √(A²) = A.
ac = v²/r = ω²r, always directed toward the centre of the circular path.
H = u²sin²θ/(2g) — depends only on u sinθ, the vertical (launch-angle-dependent) component of velocity.
Relative velocity of rain with respect to the observer: vrain,observer = vrain − vobserver, computed as a full vector subtraction, not just scalar speeds.
3JEE Main Style
A + B = 4î + 2ĵ. Magnitude = √(4² + 2²) = √20 ≈ 4.47.
R = u²sin(2θ)/g. Since sin(2θ) = sin(180°−2θ) = sin(2(90°−θ)), angles θ and (90°−θ) give identical range, though different time of flight and maximum height.
ac = v²/r = 16/2 = 8 m/s².

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