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).
Let $ P_n = \alpha^n + \beta^n $, $ n \in \mathbb{N} $. If $ P_{10} = 123,\ P_9 = 76,\ P_8 = 47 $ and $ P_1 = 1 $, then the quadratic equation having roots $ \alpha $ and $ \frac{1}{\beta} $ is:
For $ \alpha, \beta, \gamma \in \mathbb{R} $, if $$ \lim_{x \to 0} \frac{x^2 \sin \alpha x + (\gamma - 1)e^{x^2} - 3}{\sin 2x - \beta x} = 3, $$ then $ \beta + \gamma - \alpha $ is equal to:
The maximum speed of a boat in still water is 27 km/h. Now this boat is moving downstream in a river flowing at 9 km/h. A man in the boat throws a ball vertically upwards with speed of 10 m/s. Range of the ball as observed by an observer at rest on the river bank is _________ cm. (Take \( g = 10 \, {m/s}^2 \)).