Correct answer Carries: 4.
Wrong Answer Carries: -1.
A particle starts from rest with an acceleration of \( (4 \hat{i} + 3 \hat{j}) \, \text{m/s}^2 \). What is its displacement magnitude after \( 2 \, \text{s} \)?
Displacement \( \mathbf{r} = \frac{1}{2} \mathbf{a} t^2 \) (since \( \mathbf{v}_0 = 0 \)).
Given: \( \mathbf{a} = 4 \hat{i} + 3 \hat{j}, t = 2 \, \text{s} \).
\( \mathbf{r} = \frac{1}{2} (4 \hat{i} + 3 \hat{j}) \times 2^2 = 2 (4 \hat{i} + 3 \hat{j}) = 8 \hat{i} + 6 \hat{j} \, \text{m} \).
Magnitude \( |\mathbf{r}| = \sqrt{8^2 + 6^2} = \sqrt{64 + 36} = \sqrt{100} = 10 \, \text{m} \).
For a projectile launched at an angle, what is true about the horizontal and vertical motions?
The horizontal and vertical motions in projectile motion are independent of each other. The horizontal motion is uniform (constant velocity), while the vertical motion is uniformly accelerated due to gravity, allowing separate analysis of each component.
A particle’s position is given by \( x = 2t^2 + 3t \) and \( y = t^2 - 2t \) (in meters and seconds). What is the magnitude of its velocity at \( t = 2 \, \text{s} \)?
Velocity: \( v_x = \frac{dx}{dt} = 4t + 3, v_y = \frac{dy}{dt} = 2t - 2 \).
At \( t = 2 \, \text{s} \): \( v_x = 4 \times 2 + 3 = 11 \, \text{m/s}, v_y = 2 \times 2 - 2 = 2 \, \text{m/s} \).
Speed \( v = \sqrt{v_x^2 + v_y^2} = \sqrt{11^2 + 2^2} = \sqrt{121 + 4} = \sqrt{125} \approx 11.18 \, \text{m/s} \).
In projectile motion, what is conserved throughout the trajectory if air resistance is negligible?
With negligible air resistance, the total mechanical energy (kinetic + potential) is conserved in projectile motion. Energy transforms between kinetic and potential forms, but the sum remains constant as gravity is a conservative force.
A ball is thrown horizontally at \( 6 \, \text{m/s} \) from a height of \( 4.9 \, \text{m} \). What is its horizontal range? (Take \( g = 9.8 \, \text{m/s}^2 \))
Time to fall: \( h = \frac{1}{2} g t^2 \Rightarrow 4.9 = \frac{1}{2} \times 9.8 \times t^2 \Rightarrow 4.9 = 4.9 t^2 \Rightarrow t^2 = 1 \Rightarrow t = 1 \, \text{s} \).
Horizontal range \( R = v_x t = 6 \times 1 = 6 \, \text{m} \).
A particle moves in a circular path of radius \( 3 \, \text{m} \) with a speed of \( 6 \, \text{m/s} \). What is its angular speed?
Angular speed \( \omega = \frac{v}{R} \).
Given: \( v = 6 \, \text{m/s}, R = 3 \, \text{m} \).
\( \omega = \frac{6}{3} = 2 \, \text{rad/s} \).
What is the primary factor affecting the time of flight of a projectile launched from level ground?
The time of flight of a projectile depends on the initial vertical velocity component (\( v_0 \sin \theta_0 \)) and gravity (\( g \)), as given by \( T_f = \frac{2 v_0 \sin \theta_0}{g} \). The vertical component determines how long the projectile stays in the air.
A stone is dropped from a cliff 45 m high with an initial horizontal speed of 15 m/s. What is its speed on hitting the ground? (Take g = 10 m/s²)
Horizontal velocity: v_x = 15 m/s (constant).
Vertical velocity: v_y = √(2gh) = √(2 × 10 × 45) = √900 = 30 m/s.
Speed v = √(v_x² + v_y²) = √(15² + 30²) = √(225 + 900) = √1125 ≈ 33.54 m/s.
What is the physical significance of the time of flight being zero for a projectile?
A time of flight of zero occurs when the initial vertical velocity component (\( v_0 \sin \theta_0 \)) is zero, meaning the projectile is launched horizontally (\( \theta_0 = 0^\circ \)) from ground level, resulting in no vertical displacement and immediate landing.
A particle moves in a circle of radius \( 1.5 \, \text{m} \) with a speed of \( 3 \, \text{m/s} \). What is its centripetal acceleration?
Centripetal acceleration \( a_c = \frac{v^2}{R} \).
Given: \( v = 3 \, \text{m/s}, R = 1.5 \, \text{m} \).
\( a_c = \frac{3^2}{1.5} = \frac{9}{1.5} = 6 \, \text{m/s}^2 \).
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