Question:

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: 

Updated On: Apr 27, 2025
  • \(\sqrt{3}\)

  • \(\frac{1}{\sqrt{3}}\)

  • 2\(\sqrt{2}\)

  • 3

  • 3\(\sqrt{3}\)

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The Correct Option is C

Approach Solution - 1

Given:

  • Initial speed of projectile: \( V \)
  • Launch angle: \( \theta \)
  • Speed at maximum height: \( \frac{V}{3} \)

Step 1: Analyze Velocity Components

At maximum height:

  • Vertical velocity component (\( v_y \)) becomes 0.
  • Horizontal velocity component (\( v_x \)) remains constant throughout the flight.

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: \(\boxed{C}\)

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Approach Solution -2

Step 1: Recall the components of velocity in projectile motion.

In projectile motion, the velocity can be resolved into horizontal and vertical components:

  • The horizontal component of velocity is \( V_x = V \cos\theta \), which remains constant throughout the motion because there is no horizontal acceleration.
  • The vertical component of velocity is \( V_y = V \sin\theta \), which changes due to gravity.

 

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: \[ V \cos\theta = \frac{V}{3}. \]

---

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 \( \mathbf{(C)} \).

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Concepts Used:

Projectile Motion

Projectile

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.

Trajectory path/ projectile motion

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:

  1. Along the x-axis: uniform velocity, responsible for the horizontal (forward) motion of the particle.
  2. Along y-axis: uniform acceleration, responsible for the vertical (downwards) motion of the particle.

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: 

  • Horizontal Distance – x = Vx0t
  • Horizontal Velocity – Vx = Vx0
  • Vertical Distance, y – Vy0t – ½ gt2
  • Vertical Velocity, Vy – Vy0 – gt