To find the angular acceleration \( \alpha \), we use the relation between torque \( \tau \), moment of inertia \( I \), and angular acceleration:
\[\tau = I \cdot \alpha\]
The torque \( \tau \) is given by the product of the applied force \( F \) and the radius \( r \) of the disk:
\[\tau = F \cdot r\]
Substitute the given values: \( F = 15 \, \text{N} \), \( r = 0.1 \, \text{m} \), and \( I = 0.02 \, \text{kg} \cdot \text{m}^2 \).
Calculate the torque:
\[\tau = 15 \, \text{N} \times 0.1 \, \text{m} = 1.5 \, \text{Nm}\]
Now, substitute \( \tau \) into the first equation to solve for \( \alpha \):
\[1.5 = 0.02 \cdot \alpha\]
Solve for \( \alpha \):
\[\alpha = \frac{1.5}{0.02} = 75 \, \text{rad/s}^2\]
The angular acceleration \( \alpha \) is 75 rad/s\(^2\).
Two circular discs of radius \(10\) cm each are joined at their centres by a rod, as shown in the figure. The length of the rod is \(30\) cm and its mass is \(600\) g. The mass of each disc is also \(600\) g. If the applied torque between the two discs is \(43\times10^{-7}\) dyne·cm, then the angular acceleration of the system about the given axis \(AB\) is ________ rad s\(^{-2}\).

Two point charges 2q and q are placed at vertex A and centre of face CDEF of the cube as shown in figure. The electric flux passing through the cube is : 
Suppose there is a uniform circular disc of mass M kg and radius r m shown in figure. The shaded regions are cut out from the disc. The moment of inertia of the remainder about the axis A of the disc is given by $\frac{x{256} Mr^2$. The value of x is ___.
Consider the following statements: Statement I: \( 5 + 8 = 12 \) or 11 is a prime. Statement II: Sun is a planet or 9 is a prime.
Which of the following is true?
The value of \[ \int \sin(\log x) \, dx + \int \cos(\log x) \, dx \] is equal to
The value of \[ \lim_{x \to \infty} \left( e^x + e^{-x} - e^x \right) \] is equal to