Table of Contents
Key Concepts
Circular Motion Dynamics
Forces that make things turn
Concept Deep Dive
Why do we Bank Roads?
Never trust the weatherBy banking (tilting) the road, we force the Normal Reaction ($N$) to tilt. Now, a horizontal component of the normal force ($N \sin\theta$) pushes you towards the center of the curve! Because gravity and the solid road surface are always reliable (unlike friction), banking guarantees a safe turning speed regardless of the weather.
The Myth of Centrifugal Force
Who is actually pushing you?According to Newton’s First Law (Inertia), your body just wants to keep moving in a straight line. It is the car that is suddenly accelerating to the left into your path! The door of the car bumps into you and pushes you to the left (providing your centripetal force). Centrifugal force is just an illusion (a pseudo-force) invented to make Newton’s laws work inside a rotating, non-inertial frame of reference.
Compare & Contrast
✗ Horizontal Circular Motion
- Motion occurs in a horizontal plane.
- Gravity acts perpendicular to the motion and does not affect the speed.
- Speed remains constant (Uniform Circular Motion).
- Tension in a string remains constant throughout the circle.
✓ Vertical Circular Motion
- Motion occurs in a vertical plane.
- Gravity acts along the plane of motion, accelerating the body down and decelerating it up.
- Speed is variable (Non-Uniform Circular Motion).
- Tension is maximum at the bottom and minimum at the top.
Common Mistakes to Avoid
Exam Tips
Expected Exam Questions
Board Pattern Questions
Class 11 · Circular Motion · CBSE ExamFirst, convert speed to m/s: $v = 18 \times \frac{5}{18} = 5 \text{ m/s}$.
The maximum safe speed on an unbanked road is given by $v_{\text{max}} = \sqrt{\mu_s r g}$.
$v_{\text{max}} = \sqrt{0.1 \times 3 \times 9.8} = \sqrt{2.94} \approx 1.71 \text{ m/s}$.
Since the cyclist’s speed ($5 \text{ m/s}$) is much greater than the maximum safe speed ($1.71 \text{ m/s}$), the required centripetal force exceeds the available friction, and the cyclist will skid outwards and slip.
1. Draw the FBD of the car. Normal force $N$ acts perpendicular to the banked surface (angle $\theta$). Weight $mg$ acts downwards. Limiting friction $f_s$ acts down the slope to prevent the car from skidding outwards.
2. Resolve forces vertically: $N \cos\theta = mg + f_s \sin\theta$.
Since $f_s = \mu_s N$, we get $N(\cos\theta – \mu_s \sin\theta) = mg$. (Equation 1)
3. Resolve forces horizontally (towards the center): $N \sin\theta + f_s \cos\theta = \frac{mv_{\text{max}}^2}{r}$.
Substituting $f_s = \mu_s N$: $N(\sin\theta + \mu_s \cos\theta) = \frac{mv_{\text{max}}^2}{r}$. (Equation 2)
4. Divide Eq 2 by Eq 1: $\frac{\sin\theta + \mu_s \cos\theta}{\cos\theta – \mu_s \sin\theta} = \frac{v_{\text{max}}^2}{rg}$.
Divide numerator and denominator by $\cos\theta$ to get: $v_{\text{max}} = \sqrt{rg \left(\frac{\tan\theta + \mu_s}{1 – \mu_s \tan\theta}\right)}$.
Let $v_B$ be velocity at bottom and $v_T$ be velocity at top.
Tension at bottom (Max): $T_{\text{max}} = \frac{mv_B^2}{L} + mg$
Tension at top (Min): $T_{\text{min}} = \frac{mv_T^2}{L} – mg$
By conservation of energy: $\frac{1}{2}mv_B^2 = \frac{1}{2}mv_T^2 + mg(2L) \implies v_B^2 = v_T^2 + 4gL$.
Given $T_{\text{max}} / T_{\text{min}} = 4 \implies T_{\text{max}} = 4 T_{\text{min}}$.
$\frac{m(v_T^2 + 4gL)}{L} + mg = 4 \left( \frac{mv_T^2}{L} – mg \right)$
Divide by $m$ and multiply by $L$: $(v_T^2 + 4gL) + gL = 4v_T^2 – 4gL$
$v_T^2 + 5gL = 4v_T^2 – 4gL \implies 3v_T^2 = 9gL \implies v_T^2 = 3gL$.
Substitute values: $v_T^2 = 3 \times 10 \times (\frac{10}{3}) = 100 \implies v_T = 10 \text{ m/s}$.
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