A wheel of radius $ 0.2 \, \text{m} $ rotates freely about its center when a string that is wrapped over its rim is pulled by a force of $ 10 \, \text{N} $. The established torque produces an angular acceleration of $ 2 \, \text{rad/s}^2 $. Moment of inertia of the wheel is............. kg m².
To determine the moment of inertia (I) of the wheel, we start by using the relationship between torque (τ), moment of inertia (I), and angular acceleration (α). The equation is:
\( \tau = I \cdot \alpha \)
Given the force applied (F) and the radius (r) of the wheel, the torque can be calculated as:
\( \tau = F \cdot r \)
Substituting the given values, we have:
\( \tau = 10 \, \text{N} \times 0.2 \, \text{m} = 2 \, \text{Nm} \)
Next, use this torque in the relation \( \tau = I \cdot \alpha \) to solve for the moment of inertia (I):
\( I = \frac{\tau}{\alpha} = \frac{2 \, \text{Nm}}{2 \, \text{rad/s}^2} = 1 \, \text{kg m}^2 \)
Thus, the moment of inertia of the wheel is \( 1 \, \text{kg m}^2 \). This result fits exactly within the given range (1, 1).
We are given:
We need to find the moment of inertia (I) of the wheel.
The torque (\( \tau \)) produced by a force \( F \) applied tangentially at radius \( r \) is:
\[ \tau = F \times r \]
Also, the relation between torque, moment of inertia, and angular acceleration is:
\[ \tau = I \alpha \]
Therefore, the moment of inertia can be calculated as:
\[ I = \frac{\tau}{\alpha} = \frac{F r}{\alpha} \]
Step 1: Calculate the torque produced by the applied force.
\[ \tau = F \times r = 10 \times 0.2 = 2 \, \text{Nm} \]
Step 2: Use the relation between torque and angular acceleration to find \( I \):
\[ I = \frac{\tau}{\alpha} = \frac{2}{2} = 1 \, \text{kgm}^2 \]
The moment of inertia of the wheel is:
\[ \boxed{I = 1 \, \text{kgm}^2} \]
A tube of length 1m is filled completely with an ideal liquid of mass 2M, and closed at both ends. The tube is rotated uniformly in horizontal plane about one of its ends. If the force exerted by the liquid at the other end is \( F \) and the angular velocity of the tube is \( \omega \), then the value of \( \alpha \) is ______ in SI units.
If $ \theta \in [-2\pi,\ 2\pi] $, then the number of solutions of $$ 2\sqrt{2} \cos^2\theta + (2 - \sqrt{6}) \cos\theta - \sqrt{3} = 0 $$ is:
A thin transparent film with refractive index 1.4 is held on a circular ring of radius 1.8 cm. The fluid in the film evaporates such that transmission through the film at wavelength 560 nm goes to a minimum every 12 seconds. Assuming that the film is flat on its two sides, the rate of evaporation is:
The major product (A) formed in the following reaction sequence is
