Step 1: Given Data
We are given a triangle \( ABC \) with the following sides:
- \( AB = \sqrt{23} \)
- \( BC = 3 \)
- \( CA = 4 \)
We are asked to find the value of \( \frac{\cot A + \cot C}{\cot B} \).
Step 2: Applying the Cotangent Formula
The cotangent of an angle in a triangle can be expressed using the law of cosines and the sides of the triangle. Specifically:
\[
\frac{\cot A + \cot C}{\cot B} = \frac{\frac{\cos A}{\sin A} + \frac{\cos C}{\sin C}}{\frac{\cos B}{\sin B}}
\]
We can rewrite this expression using the formula for cosine in terms of the sides of the triangle:
\[
\frac{\cot A + \cot C}{\cot B} = \frac{\frac{b^2 + c^2 - a^2}{2bc} + \frac{a^2 + b^2 - c^2}{2ab}}{\frac{c^2 + a^2 - b^2}{2ac}}
\]
Step 3: Simplifying the Expression
Now, simplifying the above expression, we have:
\[
\frac{\cot A + \cot C}{\cot B} = \frac{\frac{b^2 + c^2 - a^2}{4\Delta} + \frac{a^2 + b^2 - c^2}{4\Delta}}{\frac{c^2 + a^2 - b^2}{4\Delta}}
\]
where \( \Delta \) is the area of the triangle.
Simplifying further, we get:
\[
\frac{\cot A + \cot C}{\cot B} = \frac{2b^2}{a^2 + c^2 - b^2}
\]
Step 4: Final Calculation
Substituting the given values of \( a = 3 \), \( b = 4 \), and \( c = \sqrt{23} \), we get:
\[
\frac{\cot A + \cot C}{\cot B} = \frac{2 \times 4^2}{3^2 + (\sqrt{23})^2 - 4^2}
\]
Simplifying the expression:
\[
= \frac{2 \times 16}{9 + 23 - 16}
\]
\[
= \frac{32}{16} = 2
\]
Final Answer:
The value of \( \frac{\cot A + \cot C}{\cot B} \) is \( 2 \).
The center of a disk of radius $ r $ and mass $ m $ is attached to a spring of spring constant $ k $, inside a ring of radius $ R>r $ as shown in the figure. The other end of the spring is attached on the periphery of the ring. Both the ring and the disk are in the same vertical plane. The disk can only roll along the inside periphery of the ring, without slipping. The spring can only be stretched or compressed along the periphery of the ring, following Hooke’s law. In equilibrium, the disk is at the bottom of the ring. Assuming small displacement of the disc, the time period of oscillation of center of mass of the disk is written as $ T = \frac{2\pi}{\omega} $. The correct expression for $ \omega $ is ( $ g $ is the acceleration due to gravity): 
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