Q7.
For the situation depicted in Fig. 7.19, calculate the mechanical energy of the ball just before it hits the ground and show that even at this position, it is mgh.
Answer
Just before it reaches C the ball has no potential energy left and kinetic energy mgh, so its mechanical energy is still mgh.
The object is released from rest at A, at height h. Take the ground (C) as h = 0.
Height at C: h′ = 0, so potential energy = mg × 0 = 0 J
Speed at C — using v2 = u2 + 2gh with u = 0:
v2 = 0 + 2gh = 2gh
Kinetic energy at C:
K = ½mv2 = ½ × m × 2gh = mgh
Mechanical energy at C = K + U = mgh + 0 = mgh ✔
Height at C: h′ = 0, so potential energy = mg × 0 = 0 J
Speed at C — using v2 = u2 + 2gh with u = 0:
v2 = 0 + 2gh = 2gh
Kinetic energy at C:
K = ½mv2 = ½ × m × 2gh = mgh
Mechanical energy at C = K + U = mgh + 0 = mgh ✔
Compare this with the two positions the chapter already worked out:
| Point | Potential energy | Kinetic energy | Mechanical energy |
|---|---|---|---|
| A (t = 0, height h) | mgh | 0 | mgh |
| B (time t, height h – ½gt2) | mgh – ½mg2t2 | ½mg2t2 | mgh |
| C (ground, height 0) | 0 | mgh | mgh |
Why it happens: gravity is the only force doing work here. Whatever potential energy the ball loses by falling, it gains back exactly as kinetic energy. The store simply changes its label, so the total never moves off mgh. This is the conservation of mechanical energy.
Check it yourself: take m = 0.5 kg, h = 5 m, g = 10 m s–2. At A: U = 0.5 × 10 × 5 = 25 J. At C: v = √(2 × 10 × 5) = 10 m s–1, so K = ½ × 0.5 × 100 = 25 J. Same number.