Core 2 Chapter 6: Projectile Motion

HKDSE Physics – Projectile Motion

HKDSE Physics Core
Chapter 6: Projectile Motion | 拋體運動

Billy Sir’s Smart Notes: Master 2D Motion, Trajectories, and the Monkey-Hunter Experiment.
由中大物理系碩士 Billy Sir 編寫,助你極速掌握二維運動、軌跡計算及馬騮與獵人實驗。

1. Definition of Projectile Motion | 拋體運動定義

Projectile motion is the motion of an object thrown or projected into the air, subject to only the acceleration of gravity. 拋體運動是指物體被拋入空中後,僅在重力加速度作用下的運動。

🔑 The Golden Rule of Projectiles | 拋體運動黃金法則

The horizontal and vertical motions are completely independent of each other! (水平和垂直方向的運動是完全獨立的!)

  • Horizontal (x-axis): Uniform motion. Velocity is constant (\( a_x = 0 \)). (水平:勻速運動,加速度為零)
  • Vertical (y-axis): Uniformly accelerated motion (Free fall). Acceleration is due to gravity (\( a_y = g \)). (垂直:勻加速運動/自由落體,加速度為重力加速度)

2. Horizontal Projection | 水平拋出

When an object is projected horizontally, its initial vertical velocity is zero (\( u_y = 0 \)). It is essentially a combination of a ball moving uniformly in the horizontal direction and a ball in vertical free fall. 當物體被水平拋出時,其初始垂直速度為零。它本質上是水平勻速運動和垂直自由落體的結合。

Illustration: Dropped Ball vs. Horizontally Projected Ball

Dropped (Free Fall) Projected

Notice that both balls are at the same vertical height at any given time \( t \). (注意:在任何給定時間,兩球的垂直高度完全相同。)

3. Projection at an Angle | 傾斜拋出

When a ball is projected with an initial velocity \( u \) at an angle \( \theta \) to the horizontal, we resolve the velocity into two components: (當球以初速 \( u \) 及仰角 \( \theta \) 拋出時,我們將速度分解為兩個分量:)

  • \( u_x = u \cos \theta \) (Constant throughout the flight)
  • \( u_y = u \sin \theta \) (Changes due to gravity)

🧮 Key Calculations | 核心計算公式

1. Time of Flight (\( T \)): The total time the projectile is in the air. (飛行總時間)

$$ T = \frac{2u \sin \theta}{g} $$

2. Maximum Height (\( H \)): Reached when vertical velocity \( v_y = 0 \). (最大高度)

$$ H = \frac{u^2 \sin^2 \theta}{2g} $$

3. Horizontal Range (\( R \)): The total horizontal distance traveled. (水平射程)

$$ R = \frac{u^2 \sin 2\theta}{g} $$

🎯 Maximizing Range & Complementary Angles | 最大射程與互餘角

Which angle gives the farthest range?
The maximum horizontal range occurs when \( \sin 2\theta = 1 \), which means \( 2\theta = 90^\circ \). Therefore, the optimal angle is \( \theta = 45^\circ \). (當角度為 45° 時,水平射程最遠。)

Which two angles land at the same point?
Any two complementary angles (angles that add up to \( 90^\circ \), such as \( 30^\circ \) and \( 60^\circ \)) will result in the exact same horizontal range, assuming the same initial speed. (任何兩個互餘的角度,如 30° 和 60°,將落在同一點。)

θ = 60° θ = 30° Same Range

4. Energy Changes (PE & KE) | 能量轉換 (勢能與動能)

Assuming air resistance is negligible, the total mechanical energy is conserved throughout the flight. (假設空氣阻力可忽略,整個飛行過程中的總機械能守恆。)

Position (位置) Kinetic Energy (KE) Potential Energy (PE)
Going Up (上升時) Decreases (減少) Increases (增加)
Maximum Height (最高點) Minimum (Not Zero!)
Because \( v_x \) still exists. \( KE = \frac{1}{2}m(u \cos \theta)^2 \)
Maximum
Going Down (下降時) Increases (增加) Decreases (減少)

5. The Monkey and Hunter Experiment | 馬騮與獵人實驗

A classic physics thought experiment: A hunter aims a dart gun directly at a monkey hanging from a tree branch. The exact moment the gun is fired, the monkey lets go and falls freely. Will the dart hit the monkey? (獵人瞄準樹上的馬騮開槍,開槍的瞬間馬騮鬆手自由下落。飛鏢會擊中馬騮嗎?)

🐒 The Result | 結果

Yes, the dart will always hit the monkey! (Assuming the dart reaches the monkey’s horizontal position before hitting the ground). (是的,飛鏢一定會擊中馬騮!)

🧠 The Physics Explanation | 物理原理解釋

Gravity acts on both the dart and the monkey equally. If there were no gravity, the dart would travel in a straight line and hit the monkey (who would remain stationary in the air). Because of gravity, both the dart and the monkey fall at the exact same rate (\( \frac{1}{2}gt^2 \)) relative to their gravity-free positions. Since they fall by the same vertical distance in the same amount of time, their paths will intersect! (重力對飛鏢和馬騮的作用是相同的。兩者在相同時間內下落的垂直距離完全相等,因此必定相撞!)

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