We are given the parametric equations: \[ x = \cos(\theta) + \log \left( \tan \frac{\theta}{2} \right) \] \[ y = \sin(\theta) \] We need to find the points where \( \frac{dy}{dx} = 0 \). We know that: \[ \frac{dy}{dx} = \frac{\frac{dy}{d\theta}}{\frac{dx}{d\theta}} \] #### Step 1: Derivatives of \( x \) and \( y \) with respect to \( \theta \) The derivative of \( y = \sin(\theta) \) is: \[ \frac{dy}{d\theta} = \cos(\theta) \] The derivative of \( x = \cos(\theta) + \log \left( \tan \frac{\theta}{2} \right) \) is: \[ \frac{dx}{d\theta} = -\sin(\theta) + \frac{1}{2 \tan \frac{\theta}{2}} \] #### Step 2: Setting \( \frac{dy}{dx} = 0 \) For \( \frac{dy}{dx} = 0 \), we need \( \frac{dy}{d\theta} = 0 \), which occurs when \( \cos(\theta) = 0 \). This happens when: \[ \theta = \frac{\pi}{2} + n\pi, \quad n \in \mathbb{Z} \] Thus, the points for which \( \frac{dy}{dx} = 0 \) are at: \[ \theta = n\pi, \quad n \in \mathbb{Z} \]
The correct answer is (D) : \(θ=n\pi,n ∈z\).
Given \( x = \cos\theta + \log\left(\tan\left(\frac{\theta}{2}\right)\right) \) and \( y = \sin\theta \), we want to find the values of \( \theta \) for which \( \frac{dy}{dx} = 0 \).
First, we find \( \frac{dx}{d\theta} \) and \( \frac{dy}{d\theta} \):
\[ \frac{dx}{d\theta} = -\sin\theta + \frac{1}{\tan\left(\frac{\theta}{2}\right)} \cdot \sec^2\left(\frac{\theta}{2}\right) \cdot \frac{1}{2} = -\sin\theta + \frac{\cos\left(\frac{\theta}{2}\right)}{\sin\left(\frac{\theta}{2}\right)} \cdot \frac{1}{2 \cos^2\left(\frac{\theta}{2}\right)} = -\sin\theta + \frac{1}{\sin\theta} \]
\[ \frac{dx}{d\theta} = \frac{1 - \sin^2\theta}{\sin\theta} = \frac{\cos^2\theta}{\sin\theta} \]
\[ \frac{dy}{d\theta} = \cos\theta \]
Now, we find \( \frac{dy}{dx} \):
\[ \frac{dy}{dx} = \frac{\frac{dy}{d\theta}}{\frac{dx}{d\theta}} = \frac{\cos\theta}{\frac{\cos^2\theta}{\sin\theta}} = \frac{\sin\theta}{\cos\theta} = \tan\theta \]
We want to find when \( \frac{dy}{dx} = 0 \), so we need to solve \( \tan\theta = 0 \).
\[ \tan\theta = 0 \]
\(\tan\theta = 0\) when \( \theta = n\pi \), where \( n \) is an integer.
However, we need to consider the domain of the original parametric equations. Since \( \log\left(\tan\frac{\theta}{2}\right) \) is defined, we must have \( \tan\frac{\theta}{2} > 0 \). This means that:
\[ 0 < \frac{\theta}{2} < \frac{\pi}{2} \quad \text{or} \quad \pi < \frac{\theta}{2} < \frac{3\pi}{2}, \quad \text{etc.} \]
Thus, \( 2n\pi < \theta < (2n+1)\pi \), where \( n \) is an integer.
Therefore, the values of \( \theta \) for which \( \frac{dy}{dx} = 0 \) are given by \( \theta = n\pi \), \( n \in \mathbb{Z} \), with the additional constraint that \( 2n\pi < \theta < (2n+1)\pi \).
A wooden block of mass M lies on a rough floor. Another wooden block of the same mass is hanging from the point O through strings as shown in the figure. To achieve equilibrium, the coefficient of static friction between the block on the floor and the floor itself is
In an experiment to determine the figure of merit of a galvanometer by half deflection method, a student constructed the following circuit. He applied a resistance of \( 520 \, \Omega \) in \( R \). When \( K_1 \) is closed and \( K_2 \) is open, the deflection observed in the galvanometer is 20 div. When \( K_1 \) is also closed and a resistance of \( 90 \, \Omega \) is removed in \( S \), the deflection becomes 13 div. The resistance of galvanometer is nearly: