List-I | List-II | ||
---|---|---|---|
I | A and B are moving on a horizontal circle of radius 1 m with uniform angular speed ω = 1 rad s–1. The initial angular positions of A and B at time t = 0 are θ = 0 and θ = \(\frac{\pi}{2}\), respectively. ![]() | P | \(\frac{\sqrt{3}+1}{2}\) |
II | Projectiles A and B are fired (in the same vertical plane) at t = 0 and t = 0.1 s respectively,with the same speed \(v=\frac{5\pi}{\sqrt{2}}\)m s–1 and at 45° from the horizontal plane. The initial separation between A and B is large enough so that they do not collide,(g =10 m s -2 ). | Q | \(\frac{\sqrt{3}-1}{\sqrt{2}}\) |
III | Two harmonic oscillators A and B moving in the x direction according to \(x_A = x_0 sin\frac{t}{t_0}\) and \(x_B=x_0 sin(\frac{t}{t_0}+\frac{\pi}{2})\) respectively, starting from t = 0. Take x0 = 1 m, t0 = 1 s. | R | \(\sqrt{10}\) |
IV | Particle A is rotating in a horizontal circular path of radius 1 m on the xy plane, with constant angular speed ω = 1 rad s–1. Particle B is moving up at a constant speed 3 ms–1 in the vertical direction as shown in the figure. (Ignore gravity) | S | \(\sqrt{2}\) |
T | \(\sqrt{25\pi^{2}+1}\) |
I → R, II → T, III → P, IV → S
I → S, II → P, III → Q, IV → R
I → S, II → T, III → P, IV → R
I → T, II → P, III → R, IV → S
The initial angular position of A and B at time \( t = 0 \) is \( \theta_A = 0^\circ \) and \( \theta_B = 0^\circ \), respectively.
The relative velocity between the two particles can be determined by considering their tangential velocities. Given the same radius and angular speeds, the relative velocity would be the difference in their tangential speeds.
Using the relationship \( v = r \omega \), the relative velocity magnitude is \( \sqrt{2} \), matching with option R.
Since both projectiles are fired at the same speed and at the same angle, their relative velocity will be constant throughout the motion, which gives a magnitude of \( \sqrt{2} \).
This corresponds to option Q.
- For two harmonic oscillators with the same angular frequency \( \omega \) but different initial phases, their relative motion will result in a sinusoidal variation in their displacement, giving a maximum relative velocity of \( \sqrt{2} \).
This matches with option S.
Particle A is moving in a circular path with a constant speed \( v = 3 \, \text{m/s} \), and its relative velocity with respect to a reference point is calculated using angular velocity and position.
The relative velocity magnitude in this case is \( \sqrt{3} \), which corresponds to option K.
The correct match of options is:
The correct answer is Option C: (I) - R, (II) - Q, (III) - S, (IV) - K.
A string of length \( L \) is fixed at one end and carries a mass of \( M \) at the other end. The mass makes \( \frac{3}{\pi} \) rotations per second about the vertical axis passing through the end of the string as shown. The tension in the string is ________________ ML.
Let $ S $ denote the locus of the point of intersection of the pair of lines $$ 4x - 3y = 12\alpha,\quad 4\alpha x + 3\alpha y = 12, $$ where $ \alpha $ varies over the set of non-zero real numbers. Let $ T $ be the tangent to $ S $ passing through the points $ (p, 0) $ and $ (0, q) $, $ q > 0 $, and parallel to the line $ 4x - \frac{3}{\sqrt{2}} y = 0 $.
Then the value of $ pq $ is
Let $ y(x) $ be the solution of the differential equation $$ x^2 \frac{dy}{dx} + xy = x^2 + y^2, \quad x > \frac{1}{e}, $$ satisfying $ y(1) = 0 $. Then the value of $ 2 \cdot \frac{(y(e))^2}{y(e^2)} $ is ________.