Uniform Circular Motion — Question 2

Section 6-4 · Physics pages 834–835

Question 2 A level turn imposes a speed bound through friction Take g = 10 m/s2. A vehicle modeled as a particle follows a level circular road of radius 40 m at constant speed. Static tire-road friction is the only horizontal force. Its coefficient is 0.40; ignore aerodynamic forces and rollover. O fs Plan view; tire-road static friction supplies the horizontal inward resultant. (a) Derive the maximum speed without sliding. (b) Find the fraction of the available friction used at 10 m/s. (c) If the coefficient drops to 0.10, find the new maximum speed and the minimum radius at 10 m/s.
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Question 2 - Solution A level turn imposes a speed bound through friction O fs (a) Apply the radial demand to the friction bound. Vertical balance gives N = mg. The static-friction bound must cover the radial demand: mv2 r ≤µsN = µsmg. vmax = √µsgr = √ .40(10)(40) = 4 √ 10 = 12.649 m/s . Mass cancels in this particle model. (b) Compare required and available magnitudes. At 10 m/s, compare the required force with its capacity: factual fs,max = mv2/r µsmg = 100 160 = .625 = 62.5% . The actual static friction is below its maximum. (c) Recompute the capacity. With µs = .10, vmax = √ .10(10)(40) = 2 √ 10 = 6.325 m/s . Maintaining 10 m/s instead requires r ≥v2 µsg = 100 .10(10) = 100 m .

Question 2

A level turn imposes a speed bound through friction

Take g=10g=10 m/s2^2. A vehicle modeled as a particle follows a level circular road of radius 40 m at constant speed. Static tire-road friction is the only horizontal force. Its coefficient is 0.40; ignore aerodynamic forces and rollover.

Diagram shown in the original SVG worksheet.

  1. Derive the maximum speed without sliding.

  2. Find the fraction of the available friction used at 10 m/s.

  3. If the coefficient drops to 0.10, find the new maximum speed and the minimum radius at 10 m/s.

Question 2 - Solution

A level turn imposes a speed bound through friction

Diagram shown in the original SVG worksheet.

(a) Apply the radial demand to the friction bound.

Vertical balance gives N=mgN=mg. The static-friction bound must cover the radial demand: mv2r≤μsN=μsmg.\frac{mv^2}{r}\leq\mu_sN=\mu_smg. vmax=μsgr=.40(10)(40)=410=12.649m/s.\boxed{v_{\max}=\sqrt{\mu_sgr}=\sqrt{.40(10)(40)}=4\sqrt{10}=12.649\ \mathrm{m/s}}. Mass cancels in this particle model.

(b) Compare required and available magnitudes.

At 10 m/s, compare the required force with its capacity: factualfs,max=mv2/rμsmg=100160=.625=62.5%.\boxed{\frac{f_{\mathrm{actual}}}{f_{s,\max}}=\frac{mv^2/r}{\mu_smg}=\frac{100}{160}=.625=62.5\%}. The actual static friction is below its maximum.

(c) Recompute the capacity.

With μs=.10\mu_s=.10, vmax=.10(10)(40)=210=6.325m/s.\boxed{v_{\max}=\sqrt{.10(10)(40)}=2\sqrt{10}=6.325\ \mathrm{m/s}}. Maintaining 10 m/s instead requires r≥v2μsg=100.10(10)=100m.\boxed{r\geq\frac{v^2}{\mu_sg}=\frac{100}{.10(10)}=100\ \mathrm m}.