Calculating Deceleration of Man on Bicycle with Air Resistance

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SUMMARY

The discussion focuses on calculating the deceleration of a man on a bicycle, weighing 100 kg, who is free-wheeling at a speed of 15 m/s down a 10% gradient. When he applies a braking force of 84 N, the challenge arises from the air resistance, which is proportional to the square of the speed. The key issue is the unknown constant k in the air resistance equation, leading to a need for alternative methods to determine deceleration without this constant.

PREREQUISITES
  • Understanding of Newton's laws of motion
  • Familiarity with forces acting on objects in motion
  • Knowledge of air resistance and its mathematical representation
  • Basic algebra for solving equations
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  • Research methods for estimating air resistance without the constant k
  • Study the impact of braking forces on deceleration in physics
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This discussion is beneficial for physics students, educators, and anyone interested in understanding the dynamics of motion involving forces, particularly in scenarios involving air resistance and braking mechanics.

furor celtica
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Homework Statement


A man on a bicycle, of total mass 100 kg, is free-wheeling at a constant speed of 15ms^-1 down a hill with a gradient 10% (i.e. sin^-1(0.10)). He wants to slow down to a safer speed, so he applies the brake lightly to produce a constant braking force of 84 N. The air resistance is proportional to the square of the speed.
a. Calculate the deceleration when he first applies the brake.

Homework Equations


The Attempt at a Solution


Several other questions follow.
Anyway the problem is the air resistance: in this model I know v^2 but I don’t know the constant k as in kv^2! I know how to solve these problems with k but without it I’m lost. Is there a way to work around the air resistance, i.e. without using k?
 
Last edited:
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As he is freewheeling at constant speed initially, we know that there is no resultant force on him. (No acceleration) This means that the air resistance must be exactly balanced by the component of the weight (man + cycle) down the slope.
 

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