Circular Motion – Concept Booster | Class 11 Physics CBSE

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Home Concept Boosters CBSE CBSE Class 11 Physics Laws of Motion (with Friction)

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How to Use This Page
Read each concept carefully, then check the formula, common mistake, and exam tip before moving to the next. This is Part 3 of Laws of Motion, focusing on the dynamics of Circular Motion for CBSE Class 11 Physics.

Key Concepts

Class 11 · Physics · Laws of Motion (Part 3)
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Circular Motion Dynamics

Forces that make things turn

Class 11 · Ch 4
1
Centripetal Force Formula
The net external force required to keep a body moving in a circular path. It is always directed towards the center of the circle. It is not a “new” force, but a role played by existing forces (like tension, gravity, or friction).
$$F_c = \frac{mv^2}{r} = m\omega^2 r$$
2
Centrifugal Force Formula
A pseudo force experienced only by an observer situated in a rotating (non-inertial) frame of reference. It is equal in magnitude to centripetal force but directed radially outwards.
$$F_{\text{pseudo}} = \frac{mv^2}{r} \text{ (Outwards)}$$
3
Car on a Level Circular Road Formula
When a car takes a turn on a flat road, the necessary centripetal force is provided entirely by the static friction between the tires and the road. The maximum safe speed depends on the coefficient of static friction $\mu_s$.
$$v_{\text{max}} = \sqrt{\mu_s r g}$$
4
Banking of Roads (Without Friction) Formula
Raising the outer edge of a curved road above the inner edge is called banking. At the “optimum speed”, the horizontal component of the Normal reaction provides the exact centripetal force needed, meaning absolutely zero friction is required.
$$v_{\text{optimum}} = \sqrt{rg \tan\theta} \quad \implies \quad \tan\theta = \frac{v^2}{rg}$$
5
Banking of Roads (With Friction) Formula
In reality, roads have friction. A banked road with friction allows for a wider range of safe speeds. The absolute maximum safe speed before skidding outwards is:
$$v_{\text{max}} = \sqrt{rg \left(\frac{\mu_s + \tan\theta}{1 – \mu_s \tan\theta}\right)}$$
6
Bending of a Cyclist Formula
A cyclist must lean inwards while taking a turn. The horizontal component of the normal reaction (from the ground pushing up along the tilted bicycle) provides the centripetal force.
$$\tan\theta = \frac{v^2}{rg} \quad \text{($\theta$ is angle with the vertical)}$$
7
Vertical Circular Motion (Mass on a String) Case Formulas
Motion under gravity in a vertical circle is non-uniform (speed changes). To complete a full circle without the string going slack, minimum velocities are required at specific points.
$$\text{Min Velocity at Bottom: } v_L = \sqrt{5gl}$$ $$\text{Min Velocity at Top: } v_H = \sqrt{gl}$$ $$\text{Velocity at Horizontal: } v_M = \sqrt{3gl}$$
8
Vertical Circular Motion (Mass on a Rigid Rod) Formula
Unlike a string, a rigid rod cannot go slack. Therefore, the velocity at the highest point can be exactly zero, and it will still fall through the circle.
$$\text{Min Velocity at Bottom: } v_L = \sqrt{4gl}$$

Concept Deep Dive

01

Why do we Bank Roads?

Never trust the weather
Core Concept
On a completely flat road, you rely 100% on static friction to take a turn. If it rains, snows, or oil spills on the road, $\mu_s$ drops drastically, and your $v_{\text{max}} = \sqrt{\mu_s rg}$ becomes dangerously low, causing you to skid off the road.

By 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.
02

The Myth of Centrifugal Force

Who is actually pushing you?
Crucial Concept
When a car turns left, you feel “thrown” to the right. You might think a “centrifugal force” is pushing you. It isn’t.

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

Mistake 1
Treating Centripetal Force as an Independent Force: Students often draw an FBD and include Gravity, Tension, AND Centripetal force. This is wrong. Centripetal force is just the name for the NET force toward the center. Write the equation as $\sum F_{\text{center}} = \frac{mv^2}{r}$. (e.g., $T – mg = \frac{mv^2}{r}$).
Mistake 2
Confusing the Cyclist’s Angle: In the formula $\tan\theta = \frac{v^2}{rg}$, $\theta$ is defined as the angle the cyclist makes with the Vertical. If a question gives you the angle the cyclist makes with the ground (the horizontal), you must use $(90^\circ – \theta)$ in the formula!
Mistake 3
Using the “String” formula for a “Rod”: To loop-the-loop, a mass on a string needs $v = \sqrt{5gl}$ at the bottom to prevent the string from going slack at the top. A mass attached to a stiff metal rod doesn’t have a slack problem, so it only needs $v = \sqrt{4gl}$ to make it over the top. Read the question carefully!

Exam Tips

Tip 1
The “6mg” Shortcut: For a mass $m$ tied to a string undergoing full vertical circular motion, the difference in tension between the lowest point and the highest point is always exactly $6mg$. ($T_{\text{bottom}} – T_{\text{top}} = 6mg$). This is a frequent direct MCQ question.
Tip 2
Conical Pendulum: A mass on a string moving in a horizontal circle forms a cone. The time period is $T = 2\pi\sqrt{\frac{L \cos\theta}{g}}$ where $L$ is string length and $\theta$ is the semi-vertical angle. Notice how similar it is to a simple pendulum formula!

Expected Exam Questions

SQ

Board Pattern Questions

Class 11 · Circular Motion · CBSE Exam
Class 11 · Physics
1
A cyclist speeding at $18 \text{ km/h}$ on a level road takes a sharp circular turn of radius $3 \text{ m}$ without reducing speed. The coefficient of static friction between the tires and the road is $0.1$. Will the cyclist slip while taking the turn? ($g = 9.8 \text{ m/s}^2$) [2 marks]
Answer Yes, the cyclist will slip. 📝
Explanation

First, 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.

2
Derive the expression for the maximum safe speed of a vehicle on a banked road with friction. [3 marks]
Answer Derivation required 📝
Explanation

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: $v_{\text{max}} = \sqrt{rg \left(\frac{\tan\theta + \mu_s}{1 – \mu_s \tan\theta}\right)}$.

3
A stone of mass $1 \text{ kg}$ tied to a light inextensible string of length $L = \frac{10}{3} \text{ m}$ is whirling in a circular path of radius $L$ in a vertical plane. If the ratio of the maximum tension to the minimum tension in the string is $4$, what is the speed of the stone at the highest point of the circle? ($g = 10 \text{ m/s}^2$) [3 marks]
Answer $v = 10 \text{ m/s}$ 📝
Explanation

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: $v_T^2 = 3 \times 10 \times (\frac{10}{3}) = 100 \implies v_T = 10 \text{ m/s}$.

Interactive Banking of Roads Simulator

Adjust the parameters to see how Normal and Friction forces keep the car on the road.

STATUS: SAFE

Min Safe Speed:
0.0 m/s
Optimum Speed:
0.0 m/s
Max Safe Speed:
0.0 m/s

*Center of curvature is to the left. At optimum speed, friction is zero. Above optimum, friction acts down the slope. Below optimum, friction acts up the slope.

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