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a projectile is fired from the surface of the earth with a velocity of `5ms^(-1)` and angle `theta` with the horizontal. Another projectile fired from another planet with a velocity of `3ms^(-1)` at the same angle follows a trajectory which is identical with the trajectory of the projectile fired from the earth.The value of the acceleration due to gravity on the planet is in `ms^(-2)` is given `(g=9.8 ms^(-2))`

A

3.5

B

5.9

C

16.3

D

110.8

Text Solution

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The correct Answer is:
To solve the problem, we will use the concept of projectile motion and the relationship between the maximum height of the projectiles fired from two different planets. ### Step-by-Step Solution: 1. **Understanding the Problem**: We have two projectiles: - Projectile 1 is fired from Earth with an initial velocity \( u_e = 5 \, \text{m/s} \) at an angle \( \theta \). - Projectile 2 is fired from another planet with an initial velocity \( u_p = 3 \, \text{m/s} \) at the same angle \( \theta \). Both projectiles follow identical trajectories. 2. **Height of Projectile Formula**: The maximum height \( H \) of a projectile is given by the formula: \[ H = \frac{u^2 \sin^2 \theta}{2g} \] where \( u \) is the initial velocity and \( g \) is the acceleration due to gravity. 3. **Height from Earth**: For the projectile fired from Earth: \[ H_e = \frac{u_e^2 \sin^2 \theta}{2g_e} \] where \( g_e = 9.8 \, \text{m/s}^2 \). 4. **Height from the Planet**: For the projectile fired from the other planet: \[ H_p = \frac{u_p^2 \sin^2 \theta}{2g_p} \] where \( g_p \) is the acceleration due to gravity on the planet. 5. **Setting the Heights Equal**: Since the trajectories are identical, we can set the heights equal: \[ H_e = H_p \] This gives us: \[ \frac{u_e^2 \sin^2 \theta}{2g_e} = \frac{u_p^2 \sin^2 \theta}{2g_p} \] 6. **Canceling Common Terms**: We can cancel \( \sin^2 \theta \) and \( 2 \) from both sides: \[ \frac{u_e^2}{g_e} = \frac{u_p^2}{g_p} \] 7. **Rearranging for \( g_p \)**: Rearranging the equation gives us: \[ g_p = \frac{u_p^2}{u_e^2} \cdot g_e \] 8. **Substituting Values**: Now, substituting the values: - \( u_p = 3 \, \text{m/s} \) - \( u_e = 5 \, \text{m/s} \) - \( g_e = 9.8 \, \text{m/s}^2 \) \[ g_p = \frac{3^2}{5^2} \cdot 9.8 \] \[ g_p = \frac{9}{25} \cdot 9.8 \] \[ g_p = 0.36 \cdot 9.8 \] \[ g_p = 3.528 \, \text{m/s}^2 \] 9. **Final Result**: Rounding off, we find: \[ g_p \approx 3.5 \, \text{m/s}^2 \] ### Final Answer: The value of the acceleration due to gravity on the planet is approximately \( 3.5 \, \text{m/s}^2 \). ---

To solve the problem, we will use the concept of projectile motion and the relationship between the maximum height of the projectiles fired from two different planets. ### Step-by-Step Solution: 1. **Understanding the Problem**: We have two projectiles: - Projectile 1 is fired from Earth with an initial velocity \( u_e = 5 \, \text{m/s} \) at an angle \( \theta \). - Projectile 2 is fired from another planet with an initial velocity \( u_p = 3 \, \text{m/s} \) at the same angle \( \theta \). ...
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