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Draw a Diagram Showing All Components of Forces Acting on a Vehicle Moving on a Curved Banked Road. - Physics

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Draw a diagram showing all components of forces acting on a vehicle moving on a curved banked road. 

Draw a neat labelled diagram showing the various forces and their components acting on a vehicle moving along curved banked road

Solution

  • Motion of a car on a banked road:

For the vehicle to go round the curved track at a reasonable speed without skidding, the greater centripetal force is managed for it by raising the outer edge of the track a little above the inner edge. It is called banking of circular tracks.

Consider a vehicle of weight Mg, moving round a curved path of radius r, with a speed v, on a road banked through angleθ.

The vehicle is under the action of the following forces:

  • The weight Mg acting vertically downwards

  • The reaction R of the ground to the vehicle, acting along the normal to the banked road OA in the upward direction

The vertical component R cos θ of the normal reaction R will balance the weight of the vehicle and the horizontal component R sin θ will provide the necessary centripetal force to the vehicle. Thus,

R cosθ = Mg …(i)

R sinθ = `(Mv^2)/r` .......(ii) 

On dividing equation (ii) by equation (i), we get

`(R sin theta)/(R cos theta) = (Mv^2//r)/Mg`

`tan theta = v^2/(rg)`

As the vehicle moves along the circular banked road OA, the force of friction between the road and the tyres of the vehicle, F = μR, acts in the direction AO.

The frictional force can be resolved into two components:

  • μ R sinθ in the downward direction

  • μ R cosθ in the inward direction

Since there is no motion along the vertical,

R cos θ = Mg + μ R sinθ ……. (iii)

Let vmax be the maximum permissible speed of the vehicle. The centripetal force is now provided by the components R sinθ and μ Mg cosθ, i.e.,

R sin θ + μ R cosθ = `(Mv_max  ^2)/r` .....(iv)

From equation(iii),we have

Mg = R cosθ (1−μ tanθ)…(v)

Again from equation (iv), we have 

`(Mv_max  ^2)/r`

= R cosθ (μ + tanθ) …(vi)

On dividing equation (iv) by (v), we have

`(v_max ^2)/(gr) = (µ + tan theta)/(1 - tan theta)`

`=> v_max = [(g r (µ  + tan theta)/(1 - µ tan theta)]^(1//2)`

Maximum optimum speed depends on:
1) Radius of the curved path,
2) Coefficient of friction
3) angle on inclination
Regards

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Solution Draw a Diagram Showing All Components of Forces Acting on a Vehicle Moving on a Curved Banked Road. Concept: Banking of Roads.
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