Two projectiles are thrown same speed in such a way that their ranges are equal. If the time of flights for the two projectiles are `t_(1)` and `t_(2)` the value of `'t_(1)t_(2)'` in terms of range `'R'` and `'g'` is
Two projectiles are thrown same speed in such a way that their ranges are equal. If the time of flights for the two projectiles are `t_(1)` and `t_(2)` the value of `'t_(1)t_(2)'` in terms of range `'R'` and `'g'` is
A
`(R)/(g)`
B
`(2R)/(g)`
C
`(R)/(2g)`
D
`(R)/(4g)`
Text Solution
AI Generated Solution
The correct Answer is:
To solve the problem, we need to find the product of the time of flights \( t_1 \) and \( t_2 \) of two projectiles thrown with the same speed such that their ranges are equal. Let's denote the initial speed of the projectiles as \( u \), the range as \( R \), and the acceleration due to gravity as \( g \).
### Step-by-Step Solution:
1. **Understanding the Time of Flight**:
The time of flight \( t \) for a projectile launched at an angle \( \theta \) with an initial speed \( u \) is given by:
\[
t = \frac{2u \sin \theta}{g}
\]
Therefore, for the first projectile:
\[
t_1 = \frac{2u \sin \theta_1}{g}
\]
And for the second projectile:
\[
t_2 = \frac{2u \sin \theta_2}{g}
\]
2. **Finding the Product of Time of Flights**:
We can find the product \( t_1 t_2 \):
\[
t_1 t_2 = \left(\frac{2u \sin \theta_1}{g}\right) \left(\frac{2u \sin \theta_2}{g}\right) = \frac{4u^2 \sin \theta_1 \sin \theta_2}{g^2}
\]
3. **Using the Range Formula**:
The range \( R \) of a projectile is given by:
\[
R = \frac{u^2 \sin 2\theta}{g}
\]
For the two projectiles, since their ranges are equal, we can write:
\[
R = \frac{u^2 \sin 2\theta_1}{g} = \frac{u^2 \sin 2\theta_2}{g}
\]
4. **Relating Angles**:
Since the ranges are equal, the angles \( \theta_1 \) and \( \theta_2 \) must be complementary:
\[
\theta_2 = 90^\circ - \theta_1
\]
This means:
\[
\sin \theta_2 = \cos \theta_1
\]
5. **Substituting the Sine Values**:
Now substituting \( \sin \theta_2 \) into the product:
\[
t_1 t_2 = \frac{4u^2 \sin \theta_1 \cos \theta_1}{g^2}
\]
We can use the identity \( \sin \theta_1 \cos \theta_1 = \frac{1}{2} \sin 2\theta_1 \):
\[
t_1 t_2 = \frac{4u^2}{g^2} \cdot \frac{1}{2} \sin 2\theta_1 = \frac{2u^2 \sin 2\theta_1}{g^2}
\]
6. **Expressing in Terms of Range**:
From the range equation, we know:
\[
R = \frac{u^2 \sin 2\theta_1}{g}
\]
Thus, we can express \( \sin 2\theta_1 \) as:
\[
\sin 2\theta_1 = \frac{gR}{u^2}
\]
Substituting this back into our equation for \( t_1 t_2 \):
\[
t_1 t_2 = \frac{2u^2}{g^2} \cdot \frac{gR}{u^2} = \frac{2R}{g}
\]
### Final Answer:
The value of \( t_1 t_2 \) in terms of range \( R \) and \( g \) is:
\[
t_1 t_2 = \frac{2R}{g}
\]
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