, as you scroll — highermaths.org highermaths.org read instead ›

Applications of forces

A ladder against a wall. How far up can he climb?

The ladder holds on its own. It holds with a man on the bottom rung. Yet somewhere up the ladder it will slip. Where, and why there?

scroll ↓

Four kinds of force

The smooth wall pushes straight out: SS. The rough ground pushes up with RR and grips with friction FF, towards the wall. Resolving:

R=20g+80g=100gF=S\begin{aligned} R &= 20g + 80g = 100g \\ F &= S \end{aligned}

The wall pushes harder

As he climbs, his weight turns the ladder about its foot more and more. Only the wall's push can balance that turning, so SS grows, and the foot needs more friction to match it. RR stays at 100g100g, so friction can be at most 0.4×100g=40g0.4 \times 100g = 40g.

On the point of slipping

At 2.71 m up the ladder, the foot needs all the friction the ground can give, 40g40g. The gauge is full: the ladder is on the point of slipping.

One step more

Any higher and the foot needs more than μR\mu R: it slides out and the ladder comes down the wall. A rougher floor, or a steeper ladder, would let him climb further.

Chapter 4

Resolve, take moments, respect the limit.

Particles pushed up rough slopes, rods held on rough ground, ladders on their own, connected particles over pulleys, strings that go slack, and twelve graded exam questions with full worked solutions are waiting.