Circular Motion: Common Mistakes and Fixes (4)

easy 2 min read

Question

A car of mass m=1000m = 1000 kg moves at v=20v = 20 m/s on a horizontal circular track of radius r=50r = 50 m. Find the centripetal force needed and the minimum coefficient of friction between tyres and road. Take g=10g = 10 m/s2^2.

Solution — Step by Step

Fc=mv2r=1000×40050=8000 NF_c = \frac{m v^2}{r} = \frac{1000 \times 400}{50} = 8000 \text{ N}

On a flat horizontal track, only static friction can provide the centripetal force. So fs=Fc=8000f_s = F_c = 8000 N.

The maximum static friction is μsN=μsmg\mu_s N = \mu_s m g. For the car not to slip:

μsmgmv2r    μsv2rg\mu_s m g \geq \frac{m v^2}{r} \implies \mu_s \geq \frac{v^2}{r g}

μs,min=40050×10=0.8\mu_{s,\min} = \frac{400}{50 \times 10} = 0.8

Final answers: Fc=8000F_c = 8000 N, μs,min=0.8\mu_{s,\min} = 0.8.

Why This Works

Centripetal force is not a new kind of force — it’s the net inward force from whatever real forces (friction, tension, gravity, normal) are acting. On a flat road, friction is the only horizontal force, so it must equal mv2/rm v^2 / r.

Notice that mass cancels out of the friction condition: μs,min=v2/(rg)\mu_{s,\min} = v^2/(rg). Heavier cars need the same coefficient — they have more inertia but also more weight.

Alternative Method

For a banked road at angle θ\theta, gravity helps — the optimum (no friction needed) banking angle is tanθ=v2/(rg)\tan\theta = v^2/(rg). With banking, μs\mu_s requirement drops sharply. JEE often combines flat and banked versions.

Students sometimes write “centripetal force = friction + something else.” On a flat road there’s no other inward force. Don’t invent forces — only what’s physically there can provide the centripetal pull.

Common Mistake

A persistent error: treating centripetal force as an additional force in the FBD alongside friction, gravity, and normal. It isn’t. Centripetal force is the NAME we give to the net radial force. Drawing it as a separate arrow leads to double counting.

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