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Questions 3-22 · Q15

Q.The road in the example 14 above is constructed as per the requirements. The coefficient of static friction between the tyres of a vehicle and this road is 0.8. Will there be any lower speed limit? By how much can the upper speed limit exceed in this case?
[!NOTE]
The book says “the example 14” — it refers to question 14 of this exercise (the racing-track design).

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From question 14, this road has r = 72 m and tan⁡θ=5\tan\theta=5; here μs=0.8\mu_s=0.8. Since tan⁡θ=5>μs=0.8\tan\theta=5>\mu_s=0.8, the lower speed limit is genuinely nonzero (a road banked steeply enough relative to its friction can still slide DOWN at too low a speed): vmin=rg tan⁡θ−μs1+μstan⁡θ=72×10×5−0.81+0.8×5=720×4.25=604.8≈24.59 m/s≈88.5 km/hv_{min}=\sqrt{rg\,\frac{\tan\theta-\mu_s}{1+\mu_s\tan\theta}}=\sqrt{72\times10\times\frac{5-0.8}{1+0.8\times5}}=\sqrt{720\times\frac{4.2}{5}}=\sqrt{604.8}\approx24.59\text{ m/s}\approx88.5\text{ km/h} For the upper limit, vmax=rg tan⁡θ+μs1−μstan⁡θv_{max}=\sqrt{rg\,\frac{\tan\theta+\mu_s}{1-\mu_s\tan\theta}} requires the denominator 1−μstan⁡θ=1−(0.8)(5)=1−4=−31-\mu_s\tan\theta=1-(0.8)(5)=1-4=-3, which is NEGATIVE -- meaning there is no finite value of vmaxv_{max} that satisfies the limiting-friction condition; physically, once μstan⁡θ>1\mu_s\tan\theta>1 (equivalently μs>cot⁡θ\mu_s>\cot\theta), friction acting down the slope is always more than sufficient to prevent outward skidding at ANY speed, however large. This condition is guaranteed here beca …

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