Kinematics Previous Year Questions — JEE Main Physics

38 past-year Kinematics questions from JEE Main (Physics).

Q15 (2025)

A sportsman runs around a circular track of radius $r$ such that he traverses the path ABAB. The distance travelled and displacement, respectively, are {{IMG1}}
  1. $2\mathrm{r}, 3\pi \mathrm{r}$
  2. $3\pi \mathbf{r},\pi \mathbf{r}$
  3. $\pi \mathrm{r}, 3\mathrm{r}$
  4. $3\pi \mathrm{r}, 2\mathrm{r}$
### Related Formula 1. Distance: Total actual path length covered. 2. Displacement: Shortest straight-line distance connecting the initial and final position. 3. Circumference of a complete circle = $2\pi r$ 4. Semicircular arc length = $\pi r$ ### Core Logic The trajectory is defined by the sequence of points $A \to B \to A \to B$: 1. **Distance Travelled:** - Segment 1 ($A \to B$): Semicircular path of length $\pi r$ - Segment 2 ($B \to A$): Semicircular path of length $\pi r$ - Segment 3 ($A \to B$): Semicircular path of length $\pi r$ - Total distance: $$\text{Distance} = \pi r + \pi r + \pi r = 3\pi r$$ 2. **Displacement:** - Initial position: $A$ - Final position: $B$ - Since points $A$ and $B$ represent diametrically opposite positions on the circle, the shortest distance between them is equal to the diameter of the circle: $$\text{Displacement} = 2r$$ ### Step 1: Write result The actual distance travelled is $3\pi r$ and the magnitude of displacement is $2r$. ### Pattern Recognition Sees: Circular kinematics path tracing. Trap: Accidentally substituting straight chords for the distance arcs, or assuming the loop returns fully to A (which would yield a zero displacement). Shortcut: The path ends at B. Since 3 half-loops are made, distance = $3 \times \pi r = 3\pi r$. The direct path from start A to end B is just the diameter $2r$. ### Evaluation Rubric / Model Answer null ### Chapter Mix Class 11 Physics: Motion in a Straight Line

Q81 (2025)

A river is flowing from west to east direction with speed of $9\mathrm{~km~h}^{-1}$. If a boat capable of moving at a maximum speed of $27\mathrm{~km~h}^{-1}$ in still water, crosses the river in half a minute, while moving with maximum speed at an angle of $150^{\circ}$ to direction of river flow, then the width of the river is:
  1. $300\mathrm{~m}$
  2. $112.5\mathrm{~m}$
  3. $75\mathrm{~m}$
  4. $112.5\times \sqrt{3}\mathrm{~m}$
### Related Formula $$v_{\perp} = v_{br} \sin\theta$$ $$w = v_{\perp} \cdot t$$ ### Core Logic Let the West-to-East river flow direction be along the positive $x$-axis. The boat's velocity relative to water is $v_{br} = 27\mathrm{~km/h}$ at an angle of $150^{\circ}$ with respect to the river flow (which is $30^{\circ}$ upstream from the perpendicular crossing line). To find the width of the river, we only need the component of the boat's velocity perpendicular to the river bank ($y$-axis): $$v_{\perp} = v_{br} \sin(150^{\circ}) = 27 \sin(150^{\circ}) = 27 \times \frac{1}{2} = 13.5\mathrm{~km/h}$$ Convert this velocity to SI units: $$v_{\perp} = 13.5 \times \frac{5}{18}\mathrm{~m/s} = 3.75\mathrm{~m/s}$$ Given the crossing time is half a minute ($t = 30\mathrm{~s}$): $$w = v_{\perp} \cdot t = 3.75 \times 30 = 112.5\mathrm{~m}$$ ### Step 1: Final Conclusion The width of the river is $112.5\mathrm{~m}$. ### Pattern Recognition In river-boat crossing problems, river velocity ($v_r$) only causes drift along the bank; it has zero impact on crossing time or the crossing width calculations when the angle is defined relative to the flow. Use the vertical velocity component exclusively. ### Evaluation Rubric / Model Answer null ### Chapter Mix Class 11 Physics: Kinematics

Q25 (2025)

A person travelling on a straight line moves with a uniform velocity $v_1$ for a distance $x$ and with a uniform velocity $v_2$ for the next $\frac{3}{2}x$ distance. The average velocity in this motion is $\frac{50}{7}\mathrm{~m/s}$. If $v_1$ is $5\mathrm{~m/s}$ then $v_2 = $ ____ $\mathrm{m/s}$.
### Related Formula $$v_{\text{avg}} = \frac{\text{Total Distance}}{\text{Total Time}}$$ ### Core Logic Let's find the time taken for each section of the motion: - First section of distance $x$ with velocity $v_1 = 5\mathrm{~m/s}$: $$t_1 = \frac{x}{v_1} = \frac{x}{5}$$ - Second section of distance $\frac{3}{2}x$ with velocity $v_2$: $$t_2 = \frac{3x/2}{v_2} = \frac{3x}{2v_2}$$ Total distance is: $$d_{\text{total}} = x + \frac{3}{2}x = \frac{5}{2}x$$ Average velocity is: $$v_{\text{avg}} = \frac{d_{\text{total}}}{t_1 + t_2} = \frac{\frac{5}{2}x}{\frac{x}{5} + \frac{3x}{2v_2}}$$ We are given $v_{\text{avg}} = \frac{50}{7}\mathrm{~m/s}$. Equating the two values (noting $x$ cancels out): $$\frac{50}{7} = \frac{\frac{5}{2}}{\frac{1}{5} + \frac{3}{2v_2}}$$ Divide both sides by 5: $$\frac{10}{7} = \frac{\frac{1}{2}}{\frac{1}{5} + \frac{3}{2v_2}} \implies 10 \left(\frac{1}{5} + \frac{3}{2v_2}\right) = \frac{7}{2}$$ $$2 + \frac{15}{v_2} = 3.5 \implies \frac{15}{v_2} = 1.5 \implies v_2 = \frac{15}{1.5} = 10\mathrm{~m/s}$$ ### Step 1: Final Conclusion The velocity $v_2$ is $10\mathrm{~m/s}$. ### Pattern Recognition Never take simple arithmetic averages of velocities! Average velocity must always be calculated as $\frac{\text{Total Distance}}{\text{Total Time}}$. Because total distance and time intervals are proportional to $x$, $x$ cleanly cancels out. ### Evaluation Rubric / Model Answer null ### Chapter Mix Class 11 Physics: Kinematics

Q11 (2025)

A particle is projected with velocity $u$ so that its horizontal range is three times the maximum height attained by it. The horizontal range of the projectile is given as $\frac{nu^2}{25g}$ , where value of $n$ is: (Given ' $g$' is the acceleration due to gravity).
  1. 6
  2. 18
  3. 12
  4. 24
### Related Formula For a projectile with launch speed $u$ and angle $\theta$: - Horizontal Range: $$R = \frac{u^2 \sin(2\theta)}{g} = \frac{2 u^2 \sin\theta \cos\theta}{g}$$ - Maximum Height: $$H = \frac{u^2 \sin^2\theta}{2g}$$ The general ratio linking range and maximum height is: $$\tan\theta = \frac{4H}{R}$$ ### Core Logic Given state: $$R = 3H \Rightarrow \frac{H}{R} = \frac{1}{3}$$ ### Step 1: Determine the projection angle ($\theta$) Substitute the ratio into the relation: $$\tan\theta = 4 \left(\frac{H}{R}\right) = 4 \left(\frac{1}{3}\right) = \frac{4}{3}$$ This is a standard Pythagorean triangle angle: $$\sin\theta = \frac{4}{5}, \quad \cos\theta = \frac{3}{5}$$ ### Step 2: Compute the horizontal range ($R$) $$R = \frac{2 u^2 \sin\theta \cos\theta}{g}$$ $$R = \frac{2 u^2 \left(\frac{4}{5}\right) \left(\frac{3}{5}\right)}{g} = \frac{24 u^2}{25 g}$$ Comparing this with the given format $\frac{nu^2}{25g}$: $n = 24$ ### Pattern Recognition The relation $\tan\theta = 4H/R$ is an essential identity in projectile dynamics. Whenever $R = k H$, then $\tan\theta = 4/k$. Recognizing standard angles like $\tan\theta = 4/3$ or $3/4$ directly yields trigonometric values immediately. ### Evaluation Rubric / Model Answer null ### Chapter Mix Class 11 Physics: Motion in a Plane

Q14 (2025)

A particle moves along the x-axis and has its displacement x varying with time t according to the equation $x=c_{0}(t^{2}-2)+c(t-2)^{2}$ where $c_{0}$ and c are constants of appropriate dimensions. Then, which of the following statements is correct?
  1. the acceleration of the particle is $2c_{0}$
  2. the acceleration of the particle is 2c
  3. the initial velocity of the particle is 4c
  4. the acceleration of the particle is $2(c+c_{0})$
### Related Formula In rectilinear kinematics: - Velocity: $$v = \frac{dx}{dt}$$ - Acceleration: $$a = \frac{dv}{dt} = \frac{d^2x}{dt^2}$$$ ### Core Logic Given position-time function: $$x(t) = c_0 (t^2 - 2) + c (t - 2)^2$$ ### Step 1: Differentiate once to get velocity ($v$) $$v = \frac{dx}{dt} = \frac{d}{dt}\left[c_0(t^2 - 2)\right] + \frac{d}{dt}\left[c(t-2)^2\right]$$ $$v = c_0 (2t) + c \cdot 2(t-2) = 2 c_0 t + 2 c(t - 2)$$ ### Step 2: Differentiate again to get acceleration ($a$) $$a = \frac{dv}{dt} = \frac{d}{dt}\left[2 c_0 t + 2 c(t - 2)\right]$$ $$a = 2 c_0 + 2 c = 2(c + c_0)$$ This shows acceleration is constant and equals $2(c + c_0)$, matching Statement (4). ### Pattern Recognition Whenever a position function is a pure quadratic polynomial in $t$, the acceleration is constant and equal to $2 \times$ the coefficient of the $t^2$ term. Rewriting $x(t)$: $$x(t) = (c_0 + c)t^2 - 4ct + (4c - 2c_0)$$ The coefficient of $t^2$ is $(c_0 + c)$. Thus, acceleration is $2(c_0 + c)$ directly. ### Evaluation Rubric / Model Answer null ### Chapter Mix Class 11 Physics: Motion in a Straight Line
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