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Initial velocity u = 100 m/s

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3 parts
a

5 s\text{5 s}

b

125 m\text{125 m}

c

866 m\text{866 m}

Step-by-step solution

6 steps

Here are the calculations for the projectile motion problem.

Given:
Initial velocity u=100 m/su = 100 \, \text{m/s}
Angle of projection θ=30∘\theta = 30^\circ
Acceleration due to gravity g=10 m/s2g = 10 \, \text{m/s}^2

Part a· 2 steps

The time at which the ball reaches the highest point (tmaxt_{max})

  1. Use the formula for the time to reach maximum height.

    The vertical component of velocity at the highest point is 0.

    tmax=usin⁡θgt_{max} = \frac{u \sin \theta}{g}
  2. Substitute the given values into the formula.

    tmax=100 m/s×sin⁡(30∘)10 m/s2t_{max} = \frac{100 \, \text{m/s} \times \sin(30^\circ)}{10 \, \text{m/s}^2} tmax=100 m/s×0.510 m/s2t_{max} = \frac{100 \, \text{m/s} \times 0.5}{10 \, \text{m/s}^2} tmax=50 m/s10 m/s2t_{max} = \frac{50 \, \text{m/s}}{10 \, \text{m/s}^2} tmax=5 st_{max} = 5 \, \text{s}

    The time to reach the highest point is 5 s\boxed{\text{5 s}}.

Part b

125 m\text{125 m}

The maximum height reached (HmaxH_{max})

  1. Use the formula for the maximum height.

    Hmax=u2sin⁡2θ2gH_{max} = \frac{u^2 \sin^2 \theta}{2g}
  2. Substitute the given values into the formula.

    Hmax=(100 m/s)2×(sin⁡(30∘))22×10 m/s2H_{max} = \frac{(100 \, \text{m/s})^2 \times (\sin(30^\circ))^2}{2 \times 10 \, \text{m/s}^2} Hmax=10000 m2/s2×(0.5)220 m/s2H_{max} = \frac{10000 \, \text{m}^2/\text{s}^2 \times (0.5)^2}{20 \, \text{m/s}^2} Hmax=10000 m2/s2×0.2520 m/s2H_{max} = \frac{10000 \, \text{m}^2/\text{s}^2 \times 0.25}{20 \, \text{m/s}^2} Hmax=2500 m2/s220 m/s2H_{max} = \frac{2500 \, \text{m}^2/\text{s}^2}{20 \, \text{m/s}^2} Hmax=125 mH_{max} = 125 \, \text{m}

    The maximum height reached is 125 m\boxed{\text{125 m}}.

Part c

866 m\text{866 m}

The horizontal range of the ball (RR)

  1. Use the formula for the horizontal range.

    R=u2sin⁡(2θ)gR = \frac{u^2 \sin(2\theta)}{g}
  2. Substitute the given values into the formula.

    R=(100 m/s)2×sin⁡(2×30∘)10 m/s2R = \frac{(100 \, \text{m/s})^2 \times \sin(2 \times 30^\circ)}{10 \, \text{m/s}^2} R=10000 m2/s2×sin⁡(60∘)10 m/s2R = \frac{10000 \, \text{m}^2/\text{s}^2 \times \sin(60^\circ)}{10 \, \text{m/s}^2} R=10000 m2/s2×3210 m/s2R = \frac{10000 \, \text{m}^2/\text{s}^2 \times \frac{\sqrt{3}}{2}}{10 \, \text{m/s}^2} R=10000 m2/s2×0.86602510 m/s2R = \frac{10000 \, \text{m}^2/\text{s}^2 \times 0.866025}{10 \, \text{m/s}^2} R=1000 m×0.866025R = 1000 \, \text{m} \times 0.866025 R≈866.025 mR \approx 866.025 \, \text{m}

    The horizontal range of the ball is 866 m\boxed{\text{866 m}}.

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