Circular Motion of motorcyclist

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SUMMARY

A 50kg motorcyclist on a 100kg bike can navigate a curve with a radius of 30m at a speed of 20 m/s, as the required centripetal force of 2000N matches the maximum frictional force available. If the motorcyclist accelerates beyond 20 m/s, the required centripetal force will exceed 2000N, resulting in a skid. Conversely, if the motorcyclist decelerates, she will require additional friction to slow down, which also surpasses the 2000N limit, leading to a skid. The bike leans at an angle determined by the balance of gravitational and centripetal forces, and a banked curve would reduce the reliance on friction, enhancing safety.

PREREQUISITES
  • Understanding of centripetal force and its calculation (F_c = mv²/r)
  • Knowledge of frictional forces and their limits in motion
  • Basic principles of kinetic energy and work-energy theorem
  • Familiarity with the concept of banking in circular motion
NEXT STEPS
  • Study the effects of banking on circular motion and its impact on frictional forces
  • Learn about the relationship between speed, radius, and centripetal force in circular motion
  • Explore the physics of skidding and the factors that contribute to loss of traction
  • Investigate the dynamics of motorcycle handling during acceleration and deceleration
USEFUL FOR

Physics students, motorcycle enthusiasts, and safety engineers interested in understanding the dynamics of circular motion and friction in vehicular control.

danago
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A 50kg motorcyclist on a 100kg bike enters a tight curve of radius 30m at a speed of 20ms-1. The maximum frictional force the surface can provide is 2000N before the bike will skid uncontrollably.

  • Will she make the curve safely?
  • What will happen if she speeds up while on the curve?
  • What would happen if she tried to slow down while on the curve?
  • At what angle to the vertical does she lean her bike while rounding the corner?
  • Why would this curve be safer if it was banked?

-------------------------------------------

a)
[tex]F_c=\frac{mv^2}{r}=\frac{150(20^2)}{30}=2000N[/tex]

The centripetal force required to move in that circular path is 2000N, which is supplied by the friction, so she will JUST be able to travel that path.

b) If she speeds up, the centripetal force required to continue on that path exceeds 2000N, which cannot be supplied by the friction, so she will therefore skid out of control.

c) If she slows to below 20m/s, then the centripetal force required will be less than 2000N. The maximum friction from the ground is 2000, so she should still be able to maintain her circular path. Apparently, according to the answers, she will skid if she goes lower than 20m/s. Why is this? The answer says "Slowing down requires extra friction; she will skid"


Parts a and b I am ok with, but I am a little confused with part c. Any help would be great.

Thanks,
Dan.
 
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Consider what has to happen to reduce the bike's speed. Kinetic energy must be lost through W=Fd between the tyres and the road. At the point where the bike is traveling 20ms-1 and requires additional friction to slow down, this will exceed the 2000N limit and the skid will occur.
 
You could also look at the acceleration needed to change speeds. Since F=ma then a force is needed.
 

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