Exams › NEET › Physics › Motion in a Plane
115 questions with worked solutions.
Answer: Displacement with respect to ground is zero after 2.66 and displacement with respect to ground is \( 12 \mathrm{m} \) after \( 4 s \)
The block starts at 2 m/s while the belt moves oppositely at 4 m/s, so the block must change velocity by 6 m/s in 4 s, giving constant acceleration. Using that motion, the block’s ground displacement becomes zero at about 2.66 s and equals 12 m after 4 s, matching the given correct statement.
Answer: 80
Terminal velocity occurs when downward acceleration is exactly balanced by air resistance, so the effective acceleration is zero. Using a = g - kv^2 and setting a = 0 gives v = sqrt(g/k), which evaluates to 80 m/s.
Q3. In the two dimensional motions:
Answer: \( y-x \) graph gives actual path of particle
The actual path of a particle in two-dimensional motion is its trajectory in the plane, which is described by the relation between x and y. A y-x graph shows this spatial curve directly, while x-t and y-t graphs only show how each coordinate varies with time.
Answer: equal vertical ranges but different horizontal ranges
Both observers measure the same vertical motion because gravity is unchanged and the train’s horizontal motion does not affect vertical acceleration. Their horizontal ranges differ because observer B sees the ball’s horizontal velocity as the sum of the throw and the train’s motion, while observer A does not.
Answer: 5 N
When two forces act at 90°, their resultant is found using the Pythagorean theorem. So the magnitude is \(\sqrt{3^2+4^2}=5\) N.
Answer: III only
A projectile in ideal motion has constant acceleration due to gravity, which points straight down at all times. Its velocity must be tangent to the parabolic path, so only the diagram matching both conditions can be correct.
Answer: Along a parabola with acceleration 'g"
In the ground frame, the stone has an initial horizontal velocity equal to the train’s speed at the moment of release, while its vertical motion is governed only by gravity. Since horizontal acceleration is zero and vertical acceleration is g, the path is a parabola with acceleration g.
Answer: \( 700 m \)
Displacement depends only on initial and final positions. The car starts and ends at opposite ends of a semicircle, so the straight-line separation is the diameter, which is twice the radius.
Q9. For the shown graph the slope of graph from point \( A \) to point \( B: \)
Answer: First increases then decreases
The graph’s slope is not constant; as you move from A toward the middle, the curve becomes steeper, so the slope increases. After that, it flattens again, so the slope decreases, giving the pattern “first increases then decreases.”
Answer: \( 36 \mathrm{cm} / \mathrm{sec} \)
Instantaneous velocity is the time derivative of position. For x = a + bt^2, v = dx/dt = 2bt, so at t = 3 s with b = 3 cm/s², v = 2·3·3 = 36 cm/s.
Answer: \( v=4 g t \)
For the same falling distance, time is inversely related to the square root of gravity, and final speed is proportional to the square root of gravity. Comparing the cases for 2g and 8g gives a speed difference tied to the time difference, leading to v = 4gt.
Answer: 90°
The condition that the magnitude of the sum of two vectors equals the magnitude of their difference implies that the dot product of the vectors is zero. This happens when the angle between the vectors is 90°.
Answer: \( t = \frac{\pi}{\omega} \)
Two vectors are orthogonal if their dot product is zero. The dot product of \( \mathbf{A} \) and \( \mathbf{B} \) is \( \cos \omega t \cos \frac{\omega t}{2} + \sin \omega t \sin \frac{\omega t}{2} = \cos \left( \omega t - \frac{\omega t}{2} \right) = \cos \frac{\omega t}{2} \). For orthogonality, \( \cos \frac{\omega t}{2} = 0 \), which gives \( \frac{\omega t}{2} = \frac{\pi}{2} \), or \( t = \frac{\pi}{\omega} \).
Answer: \( \mathbf{B} \times \mathbf{C} \)
Since \( \mathbf{A} \cdot \mathbf{B} = 0 \) and \( \mathbf{A} \cdot \mathbf{C} = 0 \), \( \mathbf{A} \) is perpendicular to both \( \mathbf{B} \) and \( \mathbf{C} \). The cross product \( \mathbf{B} \times \mathbf{C} \) is perpendicular to both \( \mathbf{B} \) and \( \mathbf{C} \), and hence is parallel to \( \mathbf{A} \).
Answer: decreases with increasing length of the string
The minimum speed required to rotate a stone in a vertical circle is given by v = √(gL), where g is the acceleration due to gravity and L is the length of the string. This shows that the minimum speed decreases as the length of the string increases.
Answer: 4
The shortest path occurs when the boat's velocity is directed perpendicular to the riverbank. The boat's speed in still water is 5 km/hr, and it takes 15 minutes (0.25 hours) to cross 1 km. Thus, the boat's effective speed perpendicular to the river is 1/0.25 = 4 km/hr. Using Pythagoras' theorem, the river's velocity is √(5² - 4²) = √9 = 3 km/hr.
Answer: 0.43 m/s
To swim directly across the river, the swimmer's velocity component perpendicular to the river flow must cancel the river's velocity. Using trigonometry, the river's speed is calculated as 0.5 × sin(120°) = 0.43 m/s.
Answer: 2 m/s
The linear velocity (v) in circular motion is given by v = rω, where r is the radius and ω is the angular velocity. Substituting r = 0.2 m and ω = 10 rad/s, we get v = 0.2 × 10 = 2 m/s.
Answer: 3.92 m/s
The maximum tension in the string is given as 25 N. Using the formula for centripetal force, T = mv²/r, where T is the tension, m is the mass, v is the speed, and r is the radius of the circle, we solve for v: v = √(T * r / m). Substituting T = 25 N, r = 1.96 m, and m = 0.25 kg, we get v = √(25 * 1.96 / 0.25) = 3.92 m/s.
Q20. When a body moves with a constant speed along a circle
Answer: no work is done on it
When a body moves with constant speed along a circle, its velocity changes direction continuously, so there is acceleration (centripetal). However, no work is done because the force is perpendicular to the displacement at every point.