183_notes:examples:sledding

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A little girl is riding her sled on a hill. If she starts a distance d up the hill, which makes an angle θ with the horizontal, how far will she travel along the flat snowy ground?

Facts

Child on incline of θ.

The total mass of the sled and child = m.

There's a small bit of friction between the rails of the sled and the snow = (μ_k).

Slope length = L

Initial state: at rest, at height above horizontal

Final state: at rest on horizontal

Lacking

How far will she travel along the flat?

Approximations & Assumptions

Coefficient for kinetic friction for flat + incline is the same.

No wind resistance.

Representations

System: Sled + Kid + Earth

Surroundings: Snow

ΔEsystem=Wsurroundings

ΔK+ΔUg=Wfriction

Solution

ΔEsystem=Wsurroundings

ΔK+ΔUg=Wfriction

no change ΔK=0

ΔUg=WfrictionWfriction?

Here, we pause because we have two different regions to consider.

The frictional force is different in the two regions so we must consider the work they do separately.

ΔUg=W1+W2

ΔUg=f1Δr1+f2Δr2

r2 is what we care about. (position change along flat part)

What's f1 and f2?

Fx=f1mgsinθ=ma1 don't need this because f1=μkN

Fy=Nmgcosθ=0

mgcosθ=N

f1=μkmgcosθ

Fx=f2=ma2f2=μkN=μkmg

Fy=Nmg=0

Again because not using kinematics we don't need accelerations.

ΔUg=f1Δr1+f2Δr2

In the previous equation f1Δr1W1<0 and f2Δr2W2<0 because f's are opposite to Δr's

ΔUg=(μkmgcosθ)d(μkmg)x

+mg(yfyi)=μkmgdcosθμkmgx

yfyi=μk(dcosθ+x)

What is yfyi in terms of what we know?

yfyi=dsinθ

dsinθ=μk(dcosθ+x)

dcosθ+x=dμksinθ

x=dμksinθdcosθ

x=d(sinθμkcosθμk)

[x]=m

[d]=m

All other quantities are unitless.

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  • Last modified: 2014/10/11 06:58
  • by pwirving