A projectile is thrown at a speed V and at an angle with the horizontal. If the speed at its maximum height is \(\frac{V}{3}\),then the value of tan θ is:
\(\sqrt{3}\)
\(\frac{1}{\sqrt{3}}\)
2\(\sqrt{2}\)
3
3\(\sqrt{3}\)
Given:
Step 1: Analyze Velocity Components
At maximum height:
Thus, the speed at maximum height equals the horizontal component:
\[ v_x = \frac{V}{3} \]
Step 2: Relate to Initial Velocity
The horizontal component of the initial velocity is:
\[ v_x = V \cos \theta \]
From Step 1:
\[ V \cos \theta = \frac{V}{3} \]
Simplify:
\[ \cos \theta = \frac{1}{3} \]
Step 3: Find \(\tan \theta\)
Using the identity \( \sin^2 \theta + \cos^2 \theta = 1 \):
\[ \sin \theta = \sqrt{1 - \cos^2 \theta} = \sqrt{1 - \left(\frac{1}{3}\right)^2} = \sqrt{\frac{8}{9}} = \frac{2\sqrt{2}}{3} \]
Now, calculate \( \tan \theta \):
\[ \tan \theta = \frac{\sin \theta}{\cos \theta} = \frac{\frac{2\sqrt{2}}{3}}{\frac{1}{3}} = 2\sqrt{2} \]
Conclusion:
The value of \( \tan \theta \) is \( 2\sqrt{2} \).
Answer: \(\boxed{C}\)
Step 1: Recall the components of velocity in projectile motion.
In projectile motion, the velocity can be resolved into horizontal and vertical components:
At the maximum height, the vertical component of velocity becomes zero (\( V_y = 0 \)), and the total speed is equal to the horizontal component of velocity: \[ \text{Speed at maximum height} = V_x = V \cos\theta. \]
We are given that the speed at maximum height is \( \frac{V}{3} \). Therefore: \[ V \cos\theta = \frac{V}{3}. \]
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Step 2: Solve for \( \cos\theta \).
Divide both sides of the equation by \( V \) (assuming \( V \neq 0 \)): \[ \cos\theta = \frac{1}{3}. \]
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Step 3: Use the trigonometric identity to find \( \tan\theta \).
The relationship between \( \sin\theta \), \( \cos\theta \), and \( \tan\theta \) is given by: \[ \tan\theta = \frac{\sin\theta}{\cos\theta}. \]
Using the Pythagorean identity \( \sin^2\theta + \cos^2\theta = 1 \), we can solve for \( \sin\theta \): \[ \sin^2\theta = 1 - \cos^2\theta. \] Substitute \( \cos\theta = \frac{1}{3} \): \[ \sin^2\theta = 1 - \left(\frac{1}{3}\right)^2 = 1 - \frac{1}{9} = \frac{8}{9}. \] Take the square root: \[ \sin\theta = \sqrt{\frac{8}{9}} = \frac{2\sqrt{2}}{3}. \] Now calculate \( \tan\theta \): \[ \tan\theta = \frac{\sin\theta}{\cos\theta} = \frac{\frac{2\sqrt{2}}{3}}{\frac{1}{3}} = 2\sqrt{2}. \] ---
Final Answer: The value of \( \tan\theta \) is \( \mathbf{2\sqrt{2}} \), which corresponds to option \( \mathbf{(C)} \).
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: