3000 m
2800 m
2000 m
1000 m
Given:
\(u = 280\ ms^{-1}\)
\(\theta = 30\degree\)
\(g-9.8 \ ms^{-2}\)
The maximum height attained by the bullet,
\(H_{max}=\frac{u^2sin^2\theta}{2g}\)
\(H_{max}=\frac{(280)^2\times(sin30^{\circ})^2}{2(9.8)}\)
\(H_{max}=1000\,m\)
So, the correct option is (D): \(1000\ m\)
To find the maximum height attained by the bullet, we can use the fact that at the highest point of its trajectory, the vertical component of the bullet's velocity will be zero. This is because, at this point, the bullet will have reached its maximum height and will momentarily stop before starting to fall back down.
First, we need to find the initial vertical and horizontal components of the velocity of the bullet. We can use trigonometry to do this:
Initial vertical velocity, \(v_y = 280 sin 30° = 140 \ m/s\)
Initial horizontal velocity, \(vx = 280 cos 30° = 242.4\ m/s\)
Next, we can use the fact that the maximum height attained by the bullet is equal to the vertical displacement of the bullet from its initial position. We can use the kinematic equation:
\(y = y_0 + v_yt - \frac{1}{2gt^2}\)
Where \(y_0\) is the initial vertical position (which we can take to be zero), t is the time taken to reach maximum height, and g is the acceleration due to gravity.
At the maximum height, \(v_y = 0,\) so we can rearrange the equation to solve for t:
\(t =\)\(\frac{v_y}{g}\)
Substituting in the values we have:
t = \(\frac{140}{9.8}\) = 14.29 s (to two decimal places)
Now we can use this value of t to find the maximum height:
\(y = y_0 + v_yt - \frac 12gt^2 y = 0 + 140(14.29) - \frac 12(9.8)(14.29)^2 y = 999.86 m\) (to two decimal places)
Therefore, the maximum height attained by the bullet is approximately 999.86 meters, equivalent to \(1000\ m\).
Car P is heading east with a speed V and car Q is heading north with a speed \(\sqrt{3}\). What is the velocity of car Q with respect to car P?
List I | List II | ||
---|---|---|---|
A | Mesozoic Era | I | Lower invertebrates |
B | Proterozoic Era | II | Fish & Amphibia |
C | Cenozoic Era | III | Birds & Reptiles |
D | Paleozoic Era | IV | Mammals |
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: