10 J
40 J
20 J
20√2 J
20√3 J
Given:
Step 1: Resolve Initial Velocity
At the highest point, the vertical velocity component is zero, and only the horizontal component remains:
\[ v_x = v_0 \cos \theta \]
Step 2: Relate Initial KE to Final KE
Initial KE: \( K_0 = \frac{1}{2} m v_0^2 = 40 \, \text{J} \).
KE at highest point: \( K_{\text{top}} = \frac{1}{2} m v_x^2 = \frac{1}{2} m (v_0 \cos 60^\circ)^2 \).
Since \( \cos 60^\circ = 0.5 \):
\[ K_{\text{top}} = K_0 \cos^2 60^\circ = 40 \times (0.5)^2 = 10 \, \text{J} \]
Conclusion:
The kinetic energy at the highest point is 10 J.
Answer: \(\boxed{A}\)
1. Analyze the projectile motion:
At the highest point of its trajectory, the projectile's vertical velocity component is zero. However, the horizontal velocity component remains constant throughout the motion (assuming no air resistance).
2. Relate kinetic energy to velocity components:
The initial kinetic energy (KEi) is given by:
\[KE_i = \frac{1}{2}mv_i^2 = 40 \, J\]
where \(v_i\) is the initial velocity.
The velocity can be resolved into horizontal (\(v_{ix}\)) and vertical (\(v_{iy}\)) components:
\[v_{ix} = v_i \cos(60^\circ) = \frac{1}{2}v_i\]
\[v_{iy} = v_i \sin(60^\circ) = \frac{\sqrt{3}}{2}v_i\]
3. Calculate the kinetic energy at the highest point:
At the highest point, the vertical velocity is zero (\(v_y = 0\)), and the horizontal velocity remains unchanged (\(v_x = v_{ix} = \frac{1}{2}v_i\)). The kinetic energy at the highest point (KEh) is:
\[KE_h = \frac{1}{2}mv_x^2 = \frac{1}{2}m(\frac{1}{2}v_i)^2 = \frac{1}{4}(\frac{1}{2}mv_i^2) = \frac{1}{4}KE_i\]
4. Substitute the initial kinetic energy:
\[KE_h = \frac{1}{4}(40 \, J) = 10 \, J\]
y = a sin(βx + γt)wherex and t represent displacement and time, respectively. Then, the dimensional formula for β— γis:
If \( 2 \) is a solution of the inequality \( \frac{x-a}{a-2x}<-3 \), then \( a \) must lie in the interval:
A projectile is an object set in flight by applying an external force. The projectile may be thrown up vertically or at an angle to the horizontal. It may be dropped from a position of rest. The only force acting on the projectile during its motion along the flight path is the gravitational force and it is in motion due to its own inertia.
Examples of projectile are: a ball hit by a bat, bullet fired from a gun, shell launched from a launcher, bomb dropped from a plane, etc. It must be noted that a rocket or a missile cannot be considered as a projectile as they are propelled by power.
When a particle is thrown obliquely near the earth’s surface, it moves along a curved path under constant acceleration that is directed towards the centre of the earth (we assume that the particle remains close to the surface of the earth). The path of such a particle is called a projectile and the motion is called projectile motion or trajectory motion.
In a Projectile Motion, there are two simultaneous independent rectilinear motions:
Acceleration in the horizontal projectile motion and vertical projectile motion of a particle: When a particle is projected in the air with some speed, the only force acting on it during its time in the air is the acceleration due to gravity (g). This acceleration acts vertically downward. There is no acceleration in the horizontal direction, which means that the velocity of the particle in the horizontal direction remains constant.
The types of Projectile Motion Formula are: