To find the height of the projectile when its horizontal displacement is 20 m, we begin by understanding the path of a projectile. A projectile launched at angle \( \theta = 45^\circ \) with an initial velocity \( u \) achieves its range using the formula:
\[ R = \frac{u^2 \sin 2\theta}{g} \]
Given \( R = 50 \) m and \( \theta = 45^\circ \), the formula becomes:
\[ 50 = \frac{u^2 \sin 90^\circ}{g} \]
Since \( \sin 90^\circ = 1 \), it simplifies to:
\[ 50 = \frac{u^2}{g} \]
This implies:
\[ u^2 = 50g \]
Now, to find the height when horizontal displacement (x) is 20 m, the horizontal displacement equation is:
\[ x = u \cos\theta \cdot t \]
With \( \theta = 45^\circ \), \( \cos 45^\circ = \frac{1}{\sqrt{2}} \):
\[ 20 = \frac{u}{\sqrt{2}} \cdot t \]
Solving for \( t \), we get:
\[ t = \frac{20 \sqrt{2}}{u} \]
The vertical displacement \( y \) is given by:
\[ y = u \sin\theta \cdot t - \frac{1}{2} g t^2 \]
Substitute \( \sin 45^\circ = \frac{1}{\sqrt{2}} \) and \( t = \frac{20 \sqrt{2}}{u} \):
\[ y = \frac{u}{\sqrt{2}} \cdot \frac{20 \sqrt{2}}{u} - \frac{1}{2} g \left(\frac{20 \sqrt{2}}{u}\right)^2 \]
This simplifies to:
\[ y = 20 - \frac{1}{2} g \cdot \frac{800}{u^2} \]
Knowing \( u^2 = 50g \), the equation becomes:
\[ y = 20 - \frac{1}{2} \cdot \frac{800}{50} \]
Calculate:
\[ y = 20 - \frac{1}{2} \cdot 16 \]
\[ y = 20 - 8 \]
\[ y = 12 \text{ m} \]
Thus, the height of the projectile when its horizontal displacement is 20 m is \( 12 \) m.
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