Numerical Problems Based on Coefficient of Friction and Angle of Friction for Class 11 Physics

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Numerical Problems Based on Coefficient of Friction and Angle of Friction for Class 11 Physics

Numerical Problems on Newton’s Laws of Motion

Class 11 Physics · Laws of Motion
SQ

Friction Practice Set

Apply static/kinetic friction laws and kinematics
Ch 5 · Laws of Motion
1
A block of mass 1 kg lies on a horizontal surface in a truck. The coefficient of static friction between the block and the surface is 0.6. If the acceleration of the truck is $5\text{ ms}^{-2}$, calculate the frictional force acting on the block. [IIT]
Answer 5 N 📝
Detailed Solution

Mass of the block, $m = 1\text{ kg}$; Acceleration of the truck, $a = 5\text{ ms}^{-2}$; Coefficient of static friction, $\mu_s = 0.6$. Let $g = 9.8\text{ ms}^{-2}$.

First, find the maximum static frictional force (limiting friction) available:

$$f_{max} = \mu_s N = \mu_s mg = 0.6 \times 1 \times 9.8 = 5.88\text{ N}$$

Next, find the force required to accelerate the block along with the truck:

$$F_{required} = ma = 1 \times 5 = 5\text{ N}$$

Since the required force ($5\text{ N}$) is less than the maximum available static friction ($5.88\text{ N}$), the block does not slip. The actual frictional force simply matches the required force to prevent slipping.

$$f_{actual} = 5\text{ N}$$
2
A body weighing 20 kg just slides down a rough inclined plane that rises 5 m in every 13 m. What is the coefficient of friction?
Answer 0.4167 📝
Detailed Solution

When a body “just slides” down an inclined plane, the angle of inclination ($\theta$) is equal to the angle of repose. At this point, the coefficient of friction ($\mu$) is given by $\mu = \tan\theta$.

The phrase “rises 5 m in every 13 m” refers to the geometry of the incline: Perpendicular (rise) $= 5\text{ m}$, Hypotenuse (distance along incline) $= 13\text{ m}$.

$$\sin\theta = \frac{5}{13}$$

Using the Pythagorean theorem, the base of the triangle is $\sqrt{13^2 – 5^2} = \sqrt{169 – 25} = \sqrt{144} = 12\text{ m}$.

$$\tan\theta = \frac{\text{Perpendicular}}{\text{Base}} = \frac{5}{12}$$
$$\mu = \tan\theta = \frac{5}{12} \approx 0.4167$$
3
A scooter weighs 120 kgf. Brakes are applied so that wheels stop rolling and start skidding. Find the force of friction if the coefficient of friction is 0.4.
Answer 48 kgf 📝
Detailed Solution

Weight of the scooter, $W = 120\text{ kgf}$. The normal reaction ($N$) on a horizontal surface is equal to the weight.

$$N = 120\text{ kgf}$$

Coefficient of kinetic friction, $\mu = 0.4$. The force of friction ($f$) during skidding is:

$$f = \mu N = 0.4 \times 120 = 48\text{ kgf}$$
4
An automobile is moving on a horizontal road with a speed $v$. If the coefficient of friction between the tyres and road is $\mu$, show that the shortest distance in which the automobile can be stopped is $v^2 / 2\mu g$.
Answer Proof 📝
Detailed Solution

Initial velocity, $u = v$; Final velocity, $v_f = 0$ (since it stops).

The maximum retarding force is provided by friction: $F = -\mu N = -\mu mg$.

Using Newton’s second law, the deceleration ($a$) is:

$$ma = -\mu mg \implies a = -\mu g$$

Using the third equation of motion, $v_f^2 – u^2 = 2as$:

$$0^2 – v^2 = 2(-\mu g)s$$
$$-v^2 = -2\mu gs \implies s = \frac{v^2}{2\mu g}$$

This is the required shortest stopping distance.

5
Find the distance travelled by a body before coming to rest, if it is moving with a speed of $10\text{ ms}^{-1}$ and the coefficient of friction between the ground the body is 0.4.
Answer 12.75 m 📝
Detailed Solution

Initial velocity, $u = 10\text{ ms}^{-1}$; Coefficient of friction, $\mu = 0.4$; Final velocity, $v = 0$. Take $g = 9.8\text{ ms}^{-2}$.

Using the formula derived in the previous question ($s = u^2 / 2\mu g$):

$$s = \frac{10^2}{2 \times 0.4 \times 9.8} = \frac{100}{0.8 \times 9.8}$$
$$s = \frac{100}{7.84} \approx 12.755\text{ m} \approx 12.75\text{ m}$$
6
A motor car running at the rate of $7\text{ ms}^{-1}$ can be stopped by applying brakes in 10 m. Show that total resistance to the motion, when brakes are on, is one fourth of the weight of the car.
Answer Proof 📝
Detailed Solution

Initial velocity, $u = 7\text{ ms}^{-1}$; Final velocity, $v = 0$; Stopping distance, $s = 10\text{ m}$. Take $g = 9.8\text{ ms}^{-2}$.

First, find the retardation ($a$) using $v^2 – u^2 = 2as$:

$$0^2 – 7^2 = 2a(10) \implies -49 = 20a \implies a = -2.45\text{ ms}^{-2}$$

The magnitude of the retarding force (resistance), $F = m|a| = m(2.45)$.

The weight of the car, $W = mg = m(9.8)$.

Now, find the ratio of the resistance to the weight:

$$\frac{F}{W} = \frac{m(2.45)}{m(9.8)} = \frac{2.45}{9.8} = \frac{1}{4}$$
$$F = \frac{1}{4}W$$

Hence proved.

7
Find the power of an engine which can maintain a speed of $50\text{ ms}^{-1}$ for a train of mass $3 \times 10^5\text{ kg}$ on a rough line. The coefficient of friction is 0.05. Take $g = 10\text{ ms}^{-2}$.
Answer 7500 kW 📝
Detailed Solution

Mass, $m = 3 \times 10^5\text{ kg}$; Constant speed, $v = 50\text{ ms}^{-1}$; Coefficient of friction, $\mu = 0.05$.

To maintain a constant speed, the forward force applied by the engine must exactly balance the frictional resistance ($f$).

$$F = f = \mu mg = 0.05 \times (3 \times 10^5) \times 10$$
$$F = 0.5 \times 3 \times 10^5 = 1.5 \times 10^5\text{ N}$$

Power ($P$) is the product of force and velocity:

$$P = F \times v = (1.5 \times 10^5) \times 50 = 75 \times 10^5\text{ W}$$
$$P = 7,500,000\text{ W} = 7500\text{ kW}$$
8
A train weighing 1000 quintals is running on a level road with a uniform speed of $72\text{ km h}^{-1}$. If the frictional resistance amounts to 50 g wt per quintal, find power in watt. Take $g = 9.8\text{ ms}^{-2}$.
Answer 9800 W 📝
Detailed Solution

Speed, $v = 72\text{ km h}^{-1} = 72 \times \frac{5}{18} = 20\text{ ms}^{-1}$.

Frictional resistance = $50\text{ g wt}$ per quintal.
Total weight = $1000\text{ quintals}$.

Total frictional force ($F$) = $1000 \times 50\text{ g wt} = 50,000\text{ g wt}$.

Convert grams weight to kilograms weight, then to Newtons:

$$F = \frac{50,000}{1000}\text{ kgf} = 50\text{ kgf}$$
$$F = 50 \times 9.8 = 490\text{ N}$$

Power ($P$) required to maintain the uniform speed:

$$P = F \times v = 490 \times 20 = 9800\text{ W}$$
9
An automobile of mass $m$ starts from rest and accelerates at a maximum rate possible without slipping on a road with $\mu_s = 0.5$. If only the rear wheels are driven and half the weight of the automobile is supported on these wheels, how much time is required to reach a speed of $100\text{ kmh}^{-1}$?
Answer 11.3 s 📝
Detailed Solution

Let $m$ be the mass of the car. The normal reaction on the driven rear wheels is $N_{rear} = \frac{1}{2}mg$.

The maximum forward force without slipping is the maximum static friction on the driven wheels:

$$f_{max} = \mu_s N_{rear} = 0.5 \times \frac{mg}{2} = 0.25mg$$

The maximum acceleration ($a$) of the entire car is given by $f_{max} = ma$:

$$ma = 0.25mg \implies a = 0.25g = 0.25 \times 9.8 = 2.45\text{ ms}^{-2}$$

Target velocity, $v = 100\text{ kmh}^{-1} = 100 \times \frac{5}{18} = 27.78\text{ ms}^{-1}$. Initial velocity $u = 0$.

$$v = u + at \implies 27.78 = 0 + 2.45t$$
$$t = \frac{27.78}{2.45} \approx 11.33\text{ s} \approx 11.3\text{ s}$$
10
A suitcase is gently dropped on a conveyor belt moving at $3\text{ ms}^{-1}$. If the coefficient of friction between the belt and the suitcase is 0.5, how far will the suitcase move on the belt before coming to rest?
Answer 0.92 m 📝
Detailed Solution

The phrase “move on the belt before coming to rest” implies finding the relative slipping distance until the suitcase shares the belt’s speed.

Relative to the belt, the suitcase has an initial velocity $u_{rel} = -3\text{ ms}^{-1}$ (moving backwards). It comes to rest relative to the belt, so $v_{rel} = 0$.

The forward friction from the belt provides an acceleration to the suitcase relative to the ground ($a = \mu g = 0.5 \times 9.8 = 4.9\text{ ms}^{-2}$). Relative to the belt, this is a retardation ($a_{rel} = 4.9\text{ ms}^{-2}$ in the positive direction to cancel the negative velocity).

Using the third equation of motion for relative variables ($v_{rel}^2 – u_{rel}^2 = 2a_{rel}s_{rel}$):

$$0^2 – (-3)^2 = 2(4.9) \times (-s_{rel})$$

(Note: Treating the slip direction as negative, distance magnitude is $s_{rel}$)

$$-9 = -9.8 s_{rel} \implies s_{rel} = \frac{9}{9.8} \approx 0.918\text{ m} \approx 0.92\text{ m}$$

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