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2.4-2.5

Equations of motion and gravity

Your guide: Sir HamzaBelieves every formula has a story, and units never lie.

Equations of motion and gravity

A cricket ball is thrown up. It slows, stops, and falls. Its motion follows three short equations.

Let us learn them and when to use each.

1 · Three equations for uniform acceleration

The book gives three equations. They hold only when acceleration is constant.

v_f = vᵢ + at (Eq. 2.11).

S = vᵢt + ½at2 (Eq. 2.14).

2aS = v_f2 − vᵢ2 (Eq. 2.16).

The book derives them two ways: by algebra and by graph. The graph is a velocity-time line. The area under it is S.

2 · How to choose

List what you know. Find what is missing. Pick the equation without the missing one.

No S? Use v_f = vᵢ + at. No v_f? Use S = vᵢt + ½at2. No t? Use 2aS = v_f2 − vᵢ2.

Book Example 2.2: vᵢ = 10 m s−1, a = 2 m s−2, t = 5 s gives v_f = 20 m s−1.

Book Example 2.3 gives S = 76 m.

Book Example 2.4: change units first. 300 km/h = 83.33 m s−1. Then a = 7.72 m s−2 and S = 450 m.

3 · Motion under gravity

A falling body has constant acceleration g = 9.8 m s−2 (the book's value).

So use the same three equations. Replace a by g, and S by h.

Going up, g is negative. Going down, it is positive.

Book Example 2.5 gives t = 3.34 s, v_f = 32.7 m s−1 and h = 54.56 m. The last uses the rounded 32.7.

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Notes, short questions and MCQs

Read the full notes: key terms, model answers and MCQs with answers

Equations of motion and gravity

A cricket ball is thrown up. It slows, stops, and falls. Its motion follows three short equations.

Let us learn them and when to use each.

1 · Three equations for uniform acceleration

The book gives three equations. They hold only when acceleration is constant.

v_f = vᵢ + at (Eq. 2.11).

S = vᵢt + ½at2 (Eq. 2.14).

2aS = v_f2 − vᵢ2 (Eq. 2.16).

The book derives them two ways: by algebra and by graph. The graph is a velocity-time line. The area under it is S.

2 · How to choose

List what you know. Find what is missing. Pick the equation without the missing one.

No S? Use v_f = vᵢ + at. No v_f? Use S = vᵢt + ½at2. No t? Use 2aS = v_f2 − vᵢ2.

Book Example 2.2: vᵢ = 10 m s−1, a = 2 m s−2, t = 5 s gives v_f = 20 m s−1.

Book Example 2.3 gives S = 76 m.

Book Example 2.4: change units first. 300 km/h = 83.33 m s−1. Then a = 7.72 m s−2 and S = 450 m.

3 · Motion under gravity

A falling body has constant acceleration g = 9.8 m s−2 (the book's value).

So use the same three equations. Replace a by g, and S by h.

Going up, g is negative. Going down, it is positive.

Book Example 2.5 gives t = 3.34 s, v_f = 32.7 m s−1 and h = 54.56 m. The last uses the rounded 32.7.

Key terms

Uniform acceleration
Velocity changes by equal amounts in equal times.
g
Acceleration due to gravity, 9.8 m s−2 in the book.

Short questions with model answers

  1. Q1. A body falls from rest for 2 s. Find v_f with g = 9.8.

      vᵢ = 0, so v_f = 0 + 9.8 × 2 = 19.6 m s−1.

    Common mistakes

    • ✗ “Use a = 9.8 always for gravity, even going up.”

      ✓ Going up, g acts against motion. Use −9.8.

    • ✗ “Use the three equations for any motion.”

      ✓ Only when acceleration is constant.

    MCQs

    1. 1. Which equation has no t?

      1. (a) v_f = vᵢ + at
      2. (b) S = vᵢt + ½at2
      3. (c) 2aS = v_f2 − vᵢ2
      4. (d) None
      Show answer

      (c) Eq. 2.16 has a, S, v_f, vᵢ only.

    2. 2. A car starts from rest. a = 2 m s−2, t = 5 s. S is:

      1. (a) 25 m
      2. (b) 50 m
      3. (c) 10 m
      4. (d) 5 m
      Show answer

      (a) S = ½ × 2 × 25 = 25.

    3. 3. The book's value of g is:

      1. (a) 9.8 m s−2
      2. (b) 98 m s−2
      3. (c) 0.98 m s−2
      4. (d) 8.9 m s−2
      Show answer

      (a) Section 2.5 uses g = 9.8 m s−2.

    4. 4. The area under a velocity-time graph gives:

      1. (a) Acceleration
      2. (b) Displacement
      3. (c) Force
      4. (d) Mass
      Show answer

      (b) The book uses this area to get S.

    Quick revision

    • v_f = vᵢ + at, S = vᵢt + ½at2, 2aS = v_f2 − vᵢ2.
    • For gravity, a = g = 9.8 m s−2.

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