Question #60162

18. A turn of radius 20 m is banked for the vehicles going
at a speed of 36 km/h. If the coefficient of static friction
between the road and the tyre is 0.4, what are the
possible speeds of a vehicle so that it neither slips down
nor skids up ?
1

Expert's answer

2016-05-30T10:40:03-0400

Answer on Question #60162, Physics / Mechanics | Relativity

18. A turn of radius 20m20\mathrm{m} is banked for the vehicles going at a speed of 36km/h36\mathrm{km/h} . If the coefficient of static friction between the road and the tyre is 0.4, what are the possible speeds of a vehicle so that it neither slips down nor skids up?

Solution:

Given:


v=36kmhr=10m/s,r=20m,μs=0.4\begin{array}{l} v = 3 6 \frac {k m}{h r} = 1 0 m / s, \\ r = 2 0 m, \\ \mu_ {s} = 0. 4 \\ \end{array}


The road is banked with an angle,


θ=tan1(v2rg)=tan1(1022010)=26.57\theta = \tan^ {- 1} \left(\frac {v ^ {2}}{r g}\right) = \tan^ {- 1} \left(\frac {1 0 ^ {2}}{2 0 * 1 0}\right) = 2 6. 5 7 {}^ {\circ}


When the car travels at max speed it slips upward



Force equations at maximum speed v\mathbf{v} , at threshold of sliding up incline


Fx=mv2r=Nsinθ+μsNcosθFy=0=NcosθμsNsinθmg\begin{array}{l} \sum F _ {x} = \frac {m v ^ {2}}{r} = N \sin \theta + \mu_ {s} N \cos \theta \\ \sum F _ {y} = 0 = N \cos \theta - \mu_ {s} N \sin \theta - m g \\ \end{array}


Solving the pair of equations for the maximum speed v\mathbf{v} gives:


vmax=rg(sinθ+μscosθ)cosθμssinθv _ {m a x} = \sqrt {\frac {r g (\sin \theta + \mu_ {s} \cos \theta)}{\cos \theta - \mu_ {s} \sin \theta}}vmax=2010(sin26.57+0.4cos26.57)cos26.570.4sin26.57=15ms=153.6kmhr=54kmhrv _ {m a x} = \sqrt {\frac {2 0 \cdot 1 0 \cdot (\sin 2 6 . 5 7 {}^ {\circ} + 0 . 4 \cdot \cos 2 6 . 5 7 {}^ {\circ})}{\cos 2 6 . 5 7 {}^ {\circ} - 0 . 4 \cdot \sin 2 6 . 5 7 {}^ {\circ}}} = 1 5 \frac {m}{s} = 1 5 \cdot 3. 6 \frac {k m}{h r} = 5 4 \frac {k m}{h r}


For the case of sliding down


Fx=mv2r=NsinθμsNcosθ\sum F _ {x} = \frac {m v ^ {2}}{r} = N \sin \theta - \mu_ {s} N \cos \thetaFy=0=Ncosθ+μsNsinθmg\sum F _ {y} = 0 = N \cos \theta + \mu_ {s} N \sin \theta - m g


Solving the pair of equations for the minimum speed vv gives:


vmin=rg(sinθμscosθ)cosθ+μssinθv _ {m i n} = \sqrt {\frac {r g (\sin \theta - \mu_ {s} \cos \theta)}{\cos \theta + \mu_ {s} \sin \theta}}vmin=2010(sin26.570.4cos26.57)cos26.57+0.4sin26.57=4.085ms=4.0853.6kmhr=14.7kmhrv _ {m i n} = \sqrt {\frac {2 0 \cdot 1 0 \cdot (\sin 2 6 . 5 7 {}^ {\circ} - 0 . 4 \cdot \cos 2 6 . 5 7 {}^ {\circ})}{\cos 2 6 . 5 7 {}^ {\circ} + 0 . 4 \cdot \sin 2 6 . 5 7 {}^ {\circ}}} = 4. 0 8 5 \frac {m}{s} = 4. 0 8 5 \cdot 3. 6 \frac {k m}{h r} = 1 4. 7 \frac {k m}{h r}


Answer: vmin=14.7kmhrv_{min} = 14.7 \frac{km}{hr} , vmax=54kmhrv_{max} = 54 \frac{km}{hr} .

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