Sigma Percentile
JEE Main 2021, 17 March Shift-I
LEVELJEE Main

Animated Solution for Physics - Rotational Motion: The angular speed of truck wheel is increased from to in . The number of revolutions by the truck engine during this time is ……… . (Assuming the acceleration to be uniform).

Enter Numerical Value:

Visualized Solution

\text{Visualizing the Rotating Wheel}

  • \text{Initial state: } \omega_0 = 900 \text{ rpm}
  • \text{Final state: } \omega = 2460 \text{ rpm}
  • \text{Time interval: } t = 26 \text{ s}

\text{Unit Conversion: rpm to rad/s}

  • \omega_0 = 900 \times \frac{2\pi}{60} = 30\pi \text{ rad/s}
  • \omega = 2460 \times \frac{2\pi}{60} = 82\pi \text{ rad/s}

\text{Kinematic Equations for Rotation}

  • \omega = \omega_0 + \alpha t
  • \theta = \omega_0 t + \frac{1}{2}\alpha t^2

\text{Calculating Angular Acceleration } (\alpha)

  • 82\pi = 30\pi + \alpha (26)
  • 52\pi = 26\alpha
  • \alpha = 2\pi \text{ rad/s}^2

\text{Calculating Angular Displacement } (\theta)

  • \theta = (30\pi)(26) + \frac{1}{2}(2\pi)(26)^2
  • \theta = 780\pi + \pi(676)
  • \theta = 1456\pi \text{ rad}

\text{Total Number of Revolutions } (n)

  • n = \frac{\theta}{2\pi}
  • n = \frac{1456\pi}{2\pi}
  • n = 728

\text{Alternative Approach}

  • \theta = \left(\frac{\omega_0 + \omega}{2}\right) t
  • n = \frac{\theta}{2\pi} = \left(\frac{f_0 + f}{2}\right) t
  • n = \left(\frac{\frac{900}{60} + \frac{2460}{60}}{2}\right) \times 26 = 728

The Sigma Insight: Kinematics of Rotational Motion

Solution Diagram

The Setup

Visualizing the Spinning Wheel
Imagine a massive truck wheel spinning on the highway. The driver steps on the gas, and the wheel's rotation speeds up from to over a span of .
We need to find out exactly how many times this wheel turned during this acceleration phase. This is a classic problem of kinematics of rotational motion, where the principles are identical to linear motion, just with a rotational twist!

Step 1

Taming the Units
Before we apply any physics equations, we must ensure our units are consistent. Standard SI units for angular velocity are radians per second ().
To convert revolutions per minute () to radians per second, we multiply by (since one revolution is radians) and divide by (to convert minutes to seconds).
Now our initial and final angular velocities are ready for action.

Step 2

Uncovering the Angular Acceleration
Since the problem states the acceleration is uniform, we can directly use the rotational equivalents of Newton's equations of motion. The first equation links angular velocities, acceleration, and time:
Let's plug our values into this equation to find the angular acceleration, .
Subtracting from both sides gives . Dividing by , we find that the angular acceleration is exactly:

Step 3

The Total Angular Displacement
Next, we need to find the total angle turned, , during this time. We use the second equation of rotational motion:
Substituting our known values:
Adding them up, the total angular displacement is:

The Final Stretch

Counting the Revolutions
We have the total angle in radians, but the question asks for the number of revolutions ().
Since one full revolution covers an angle of radians, we simply divide our total by .
The truck engine made exactly 728 revolutions during this time!

The Pro-Tip

The Average Velocity Shortcut
As a pro-tip, you could have solved this much faster! For uniform acceleration, the average angular velocity is simply the arithmetic mean of the initial and final velocities.
By converting the speeds to revolutions per second (), we get:
Their average is:
Multiplying this average velocity by the time () gives us the total revolutions directly:
Try this shortcut out, it's a massive time-saver for competitive exams!

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Comprehension Passage

The general motion of a rigid body can be considered to be a combination of (i) a motion of its centre of mass about an axis, and (ii) its motion about an instantaneous axis passing through the centre of mass. These axes need not be stationary. Consider, for example, a thin uniform disc welded (rigidly fixed) horizontally at its rim to a massless stick, as shown in the figure. When the disc-stick system is rotated about the origin on a horizontal frictionless plane with angular speed , the motion at any instant can be taken as a combination of (i) a rotation of the centre of mass of the disc about the Z-axis, and (ii) a rotation of the disc through an instantaneous vertical axis passing through its centre of mass (as is seen from the changed orientation of points and ). Both these motions have the same angular speed in this case. Now, consider two similar systems as shown in the figure : Case (a) the disc with its face vertical and parallel to x-z plane; Case (b) the disc with its face making an angle of with x-y plane and its horizontal diameter parallel to X-axis. In both the cases, the disc is welded at point , and the systems are rotated with constant angular speed about the Z-axis.
Question 1:

Which of the following statements regarding the angular speed about the instantaneous axis (passing through the centre of mass) is correct?

(A)
It is for both the cases
(B)
It is for case (a); and for case (b)
(C)
It is for case (a); and for case (b)
(D)
It is for both the cases
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Which of the following statements about the instantaneous axis (passing through the centre of mass) is correct?

(A)
It is vertical for both the cases (a) and (b)
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It is vertical for case (a); and is at to the x-z plane and lies in the plane of the disc for case (b)
(C)
It is horizontal for case (a); and is at to the x-z plane and is normal to the plane of the disc for case (b)
(D)
It is vertical for case (a); and is at to the x-z plane and is normal to the plane of the disc for case (b)
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Consider a disc rotating in the horizontal plane with a constant angular speed about its centre . The disc has a shaded region on one side of the diameter and an unshaded region on the other side as shown in the figure. When the disc is in the orientation as shown, two pebbles and are simultaneously projected at an angle towards . The velocity of projection is in the - plane and is same for both pebbles with respect to the disc. Assume that (i) they land back on the disc before the disc has completed rotation, (ii) their range is less than half the disc radius, and (iii) remains constant throughout. Then

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lands in the shaded region and in the unshaded region
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lands in the unshaded region and in the shaded region
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both and land in the unshaded region
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both and land in the shaded region
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A rigid uniform bar of length is slipping from its vertical position on a frictionless floor (as shown in the figure). At some instant of time, the angle made by the bar with the vertical is . Which of the following statements about its motion is/are correct?

* Multiple Correct Options
(A)
Instantaneous torque about the point in contact with the floor is proportional to
(B)
The trajectory of the point is parabola
(C)
The mid-point of the bar will fall vertically downward
(D)
When the bar makes an angle with the vertical, the displacement of its mid-point from the initial position is proportional to