Verify the ranges for the projectiles in Figure 3.41 (a) for $\mathit{\theta }\mathbf{=}\mathbf{45}\mathbf{°}$and the given initial velocities.

The horizontal range is the distance between a projectile's point of projection and its point of impact. By adjusting the projectile's initial velocity and projection angle, one may alter the projectile's horizontal range of motion.

The expression for the horizontal range is,

$R=\frac{u^2\sin \left(2\theta \right)}{g}$ ....(1.1)

Here is the horizontal range, is the angle of projection, and is the acceleration due to gravity.

• The angle of projection is,$\theta =45.0°$.
• The initial velocity of projection $30\text{m/s}$.
• The range of projectile for $30\text{m/s}$is $91.8\text{m}$.
• The initial velocity of projection $40\text{m/s}$.
• The range of projectile for $40\text{m/s}$is $163\text{m}$.
• The initial velocity of the projectile $50\text{m/s}$.
• The range of projectile for $50\text{m/s}$is $255\text{m/s}$.

When the initial velocity is $30\text{m/s}$, and the angle of projection is $45°$, the horizontal range can be calculated using equation (1.1).

Substitute the value in equation 1.1, and we get,

$\begin{array}{rcl}R& =& \frac{{\left(30\text{m/s}\right)}^2\times \sin \left(2\times 45°\right)}{\left(9.8{\text{m/s}}^{\text{2}}\right)}\\ & =& 91.8\text{m}\\ & & \end{array}$

Hence, when the initial velocity is $30\text{m/s}$, the range of the projectile is $91.8\text{m}$.

When the initial velocity is $40\text{m/s}$, and the angle of projection is $45°$, the horizontal range can be calculated using equation (1.1).

Substitute the value in equation 1.1, and we get,

$\begin{array}{rcl}R& =& \frac{{\left(40\text{m/s}\right)}^2\times \sin \left(2\times 45°\right)}{\left(9.8{\text{m/s}}^2\right)}\\ & \approx & \text{163}\text{m}\\ & & \end{array}$

Hence, when the initial velocity is $40\text{m/s}$, the range of the projectile is $\text{163 m}$.

When the initial velocity is$50\text{m}/\text{s}$, and the angle of projection is $45°$, the horizontal range can be calculated using equation (1.1).

Substitute the value in equation 1.1, and we get,

$\begin{array}{rcl}R& =& \frac{{\left(50\text{m/s}\right)}^2\times \sin \left(2\times 45°\right)}{\left(9.8{\text{m/s}}^2\right)}\\ & \approx & \text{255}\text{m}\\ & & \end{array}$

Hence, when the initial velocity is , the range of the projectile is .