Q1.
Remove both the ends from a pen so that the refill can slide freely through the barrel (Fig. 7.40). Fix the pen cap to the side of the barrel and attach a rubber band to the clip of the cap. Connect the free end of the rubber band to the refill using a safety pin. Stretch and release the rubber band. The refill shoots out, showing the conversion of elastic potential energy into kinetic energy. Repeat with different amounts of stretch, and observe how the distance travelled changes. Is there a relationship between the stretch and the distance travelled?
Answer
Yes. The farther you stretch the band, the farther the refill flies — and the distance grows much faster than the stretch does, roughly as the square of the extension.
How to do the experiment properly
- Mark the barrel in centimetres so you can pull the refill back by a measured amount x each time.
- Fire the refill horizontally from the same height and from the same launch spot every time — tape the pen to the edge of a table.
- Measure the horizontal distance R from the table edge to where the refill first lands.
- Take three shots at each stretch and use the average, to reduce the error.
| Stretch x (cm) | Distance R (cm) — sample readings | R ÷ x | R ÷ x² |
|---|---|---|---|
| 2 | 40 | 20 | 10 |
| 3 | 90 | 30 | 10 |
| 4 | 160 | 40 | 10 |
Why R goes as x2
Elastic potential energy stored in the stretched band grows as the square of the extension: U ∝ x2
All of it becomes kinetic energy of the refill: ½mv2 = U ∝ x2
so v2 ∝ x2, i.e. v ∝ x
For a horizontal launch from a fixed height, the time of flight t is the same every shot,
so for a horizontal launch off a table the time of flight t is fixed and R = v × t ∝ v ∝ x
but for a launch at an angle the projectile formula gives R ∝ v2 ∝ x2
Elastic potential energy stored in the stretched band grows as the square of the extension: U ∝ x2
All of it becomes kinetic energy of the refill: ½mv2 = U ∝ x2
so v2 ∝ x2, i.e. v ∝ x
For a horizontal launch from a fixed height, the time of flight t is the same every shot,
so for a horizontal launch off a table the time of flight t is fixed and R = v × t ∝ v ∝ x
but for a launch at an angle the projectile formula gives R ∝ v2 ∝ x2
What to expect in your own data: if you fire horizontally off a table, R rises in proportion to x. If you fire at an angle across the floor, R rises roughly as x². Either way, doubling the stretch more than doubles the reach — and a graph of R against x² (or against x) that comes out as a straight line is the proof.
Safety: never aim the refill at anyone's face, and wear spectacles if you have them. Fire along the floor or into a cardboard box.