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DC Pandey Solutions Circular Motion- 1 - DC Pandey Solutions for NEET Physics

Introductory Exercise 7.1

Q.1. Is the acceleration of a particle in uniform circular motion constant or variable?
Ans. 
Variable

In uniform circular motion the magnitude of acceleration Introductory Exercise 7.1 does not changewhile its direction (being always towards the centre of the circular path) changes.

Q.2. Is it necessary to express all angles in radian while using the equation ω = ω0 + αt?
Ans.
No

If ω0 and ω are in rad s-1 the value of a must be in rad s-2. But, if ω0 and ω are in degree s-1 the value of a must also be in degree s-2. Thus, it is not necessary to express all angles in radian. One way change rad into degree using π rad = 180°.

Q.3. Which of the following quantities may remain constant during the motion of an object along a curved path?
(i) Velocity
(ii) Speed
(iii) Acceleration
(iv ) Magnitude of acceleration
Ans.
speed, acceleration, the magnitude of acceleration.

During motion of an object along a curved path the speed and magnitude of its radial acceleration may remain constant. Due to change in direction of motion the velocity of the object will change even if its speed is constant. Further, the acceleration will also change even if the speed is constant.

Q.4. A particle moves in a circle of radius 1.0 cm with a speed given by v = 2 t where v is in cm/s and t in seconds.
(a ) Find the radial acceleration of the particle at t = 1 s.
(b) Find the tangential acceleration at t = 1 s.
(c) Find the magnitude of net acceleration at t = 1 s.
Ans. 
(a) 4.0 cms-2  (b) 2.0 cms-2 (c) 2√5 cms-2

(i) Radial acceleration (αc)
Introductory Exercise 7.1
(ii) Tangential acceleration (αT )
Introductory Exercise 7.1
(iii) Magnitude of net acceleration
Introductory Exercise 7.1 

Q.5. A particle is moving with a constant speed in a circular path. Find the ratio of average velocity to its instantaneous velocity when the particle describes an angle Introductory Exercise 7.1
Ans. 
Introductory Exercise 7.1

Introductory Exercise 7.1

Introductory Exercise 7.1
Introductory Exercise 7.1
Introductory Exercise 7.1

Q.6. A particle is moving with a constant angular acceleration of 4 rad/sin a circular path. At time t =0, particle was at rest. Find the time at which the magnitudes of centripetal acceleration and tangential acceleration are equal.
Ans: 1/2 s

ωt = 0 + 4t
Centripetal acceleration = tangential acceleration
Introductory Exercise 7.1

Introductory Exercise 7.2

Q.1. Is a body in uniform circular motion in equilibrium?

Ans. In uniform circular motion of a body the body is never in equilibrium as only one force (centripetal) acts on the body which forces the perform circular motion.

Q.2. Find the maximum speed at which a truck can safely travel without toppling over, on a curve of radius 250 m. The height of the centre of gravity of the truck above the ground is 1.5 m and the distance between the wheels is 1.5 m, the truck being horizontal.

Ans. Introductory Exercise 7.2
= 35 ms-1
Introductory Exercise 7.2

Q.3. (a) How many revolutions per minute must the apparatus shown in figure make about a vertical axis so that the cord makes an angle of 45° with the vertical?
(b) What is the tension in the cord then. Given, l = √2 m, a = 20 cm and m = 5.0 kg?

Introductory Exercise 7.2
Ans.

Introductory Exercise 7.2
Introductory Exercise 7.2
Introductory Exercise 7.2
Introductory Exercise 7.2
Introductory Exercise 7.2
Introductory Exercise 7.2
Introductory Exercise 7.2

Q.4. A car moves at a constant speed on a straight but hilly road. One section has a crest and dip of the same 250 m radius.
(a) As the car passes over the crest the normal force on the car is one half the 16 kN weight of the car. What will be the normal force on the car as its passes through the bottom of the dip?
(b) What is the greatest speed at which the car can move without leaving the road at the top of the hill?
(c) Moving at a speed found in part (b) what will be the normal force on the car as it moves through the bottom of the dip? (Take g = 10 m/s2)
Ans.

Introductory Exercise 7.2
(a) At rest :Required CPF = Introductory Exercise 7.2
Introductory Exercise 7.2...(i)
At dip :
Required CPF = N' - w
Introductory Exercise 7.2...(ii)
Comparing Eqs. (i) and (ii),
Introductory Exercise 7.2
Introductory Exercise 7.2
= 24 kN
(b) At crest on increasing the speed (v), the value of N will decrease and for maximum value of v the of N will be just zero.
Thus, Introductory Exercise 7.2
Introductory Exercise 7.2
Introductory Exercise 7.2
(c) At dip :
Introductory Exercise 7.2
= w + mg
= 2w = 32 kN

Q.5. A car driver going at speed v suddenly finds a wide wall at a distance r. Should he apply brakes or turn the car in a circle of radius r to avoid hitting the wall.
Ans. 
Case I. If the driver turns the vehicle

Introductory Exercise 7.2
Introductory Exercise 7.2
[where v1 = maximum speed of vehicle]
Introductory Exercise 7.2
Case II. If the driver tries to stop the vehicle by applying breaks.
Maximum retardation = μg
Introductory Exercise 7.2
As v2 > v1, driver should apply breaks to stop the vehicle rather than taking turn.

Q.6. Show that the angle made by the string with the vertical in a conical pendulum is given by cos θ = Introductory Exercise 7.2 where L is the length of the string and ω is the angular speed.
Ans. 
In the answer to question 3(a) if we replace θ  by Φ

Introductory Exercise 7.2
If θ is the angle made by the string with the vertical
Introductory Exercise 7.2

The document DC Pandey Solutions: Circular Motion- 1 is a part of the NEET Course DC Pandey Solutions for NEET Physics.
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FAQs on DC Pandey Solutions: Circular Motion- 1

1. What is centripetal force and why do objects need it to move in circles?
Ans. Centripetal force is the inward-directed force required to keep an object moving along a circular path at constant speed. Without it, objects would move in straight lines due to inertia. This force continuously changes the direction of velocity, not its magnitude, causing circular motion. Common sources include tension, friction, gravity, and normal force depending on the scenario.
2. How do I find the relationship between angular velocity and linear velocity in circular motion problems?
Ans. Linear velocity and angular velocity are connected by the equation v = ωr, where v is linear velocity, ω is angular velocity, and r is the radius of the circular path. Linear velocity represents how fast an object covers distance along the circle's edge, while angular velocity measures how quickly it rotates around the centre. This relationship helps solve DC Pandey problems involving rotating bodies and orbital motion.
3. Why does a car need more friction on curved roads compared to straight roads?
Ans. Curved roads demand friction to provide centripetal acceleration toward the centre, keeping the vehicle on its circular path. On straight roads, friction only opposes motion. During turning, friction must supply the necessary centripetal force; if insufficient, the car skids outward. Banking roads reduces this friction requirement by adding an inward-tilted component, improving safety on highways and sharp turns.
4. What's the difference between uniform circular motion and non-uniform circular motion?
Ans. Uniform circular motion occurs when an object moves at constant speed along a circular path, requiring only centripetal acceleration toward the centre. Non-uniform circular motion involves changing speed, requiring both centripetal acceleration (inward) and tangential acceleration (along the path). Tangential acceleration changes the object's speed while centripetal acceleration adjusts its direction, making non-uniform motion more complex in NEET physics problems.
5. How do I calculate the normal force when an object moves in a vertical circle?
Ans. For vertical circular motion, apply Newton's second law along the radial direction. At the highest point, normal force and weight combine to provide centripetal force: N + mg = mv²/r. At the lowest point, normal force minus weight supplies centripetal acceleration: N - mg = mv²/r. The normal force varies throughout the circle; it's maximum at the bottom and minimum at the top, critical for understanding tension and contact forces.
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