We are given the following equations:
\[ x = e^\theta \sin \theta \]
\[ y = e^{\theta} \cos \theta \]
Next, we differentiate both sides of the first equation with respect to \(\theta\):
\[ \frac{d}{d\theta}(x) = \frac{d}{d\theta}(e^{\theta} \sin \theta) \]
Using the product rule, we get:
\[ \frac{dx}{d\theta} = e^\theta \sin \theta + e^\theta \cos \theta \]
Now, we differentiate both sides of the second equation with respect to \(\theta\):
\[ \frac{d}{d\theta}(y) = \frac{d}{d\theta}(e^\theta \cos \theta) \]
Using the product rule, we get:
\[ \frac{dy}{d\theta} = e^\theta \cos \theta - e^\theta \sin \theta \]
Now, to find \(\frac{dy}{dx}\), we divide \(\frac{\frac{dy}{d\theta}}{\frac{dx}{d\theta}}\):
\[ \frac{dy}{dx} = \frac{\frac{dy}{d\theta}}{\frac{dx}{d\theta}} \]
Substituting the expressions for \(\frac{dy}{d\theta}\) and \(\frac{dx}{d\theta}\), we get:
\[ \frac{dy}{dx} = \frac{e^\theta \cos \theta - e^\theta \sin \theta}{e^\theta \sin \theta + e^\theta \cos \theta} \]
Next, we substitute the values of \(x\) and \(y\) at (1,1) into the equation to evaluate \(\frac{dy}{dx}\):
\[ x = e^\theta \sin \theta = 1 \]
\[ y = e^\theta \cos \theta = 1 \]
Dividing the second equation by the first equation, we get:
\[ \tan \theta = \frac{y}{x} = \frac{1}{1} = 1 \]
Simplifying the expression for \(\frac{dy}{dx}\) using trigonometric identities:
\[ \frac{dy}{dx} = \frac{\cos \theta - \sin \theta}{\sin \theta + \cos \theta} \]
Since \(\tan \theta = 1\), we substitute:
\[ \frac{\cos \theta - \sin \theta}{\sin \theta + \cos \theta} = \frac{\frac{1}{\sqrt{2}} - \frac{1}{\sqrt{2}}}{\frac{1}{\sqrt{2}} + \frac{1}{\sqrt{2}}} = \frac{0}{\sqrt{2}} = 0 \]
Therefore, at (1,1), \(\frac{dy}{dx}\) is equal to 0, which corresponds to option (A) 0.
We are given the parametric equations: \[ x = e^{\theta} \sin \theta, \quad y = e^{\theta} \cos \theta \] To find \(\frac{dy}{dx}\), use: \[ \frac{dy}{dx} = \frac{\frac{dy}{d\theta}}{\frac{dx}{d\theta}} \] Differentiate both: \[ \frac{dx}{d\theta} = \frac{d}{d\theta}(e^\theta \sin \theta) = e^\theta \sin \theta + e^\theta \cos \theta \] \[ \frac{dy}{d\theta} = \frac{d}{d\theta}(e^\theta \cos \theta) = e^\theta \cos \theta - e^\theta \sin \theta \] So, \[ \frac{dy}{dx} = \frac{e^\theta(\cos \theta - \sin \theta)}{e^\theta(\sin \theta + \cos \theta)} = \frac{\cos \theta - \sin \theta}{\sin \theta + \cos \theta} \] Now find the value of \( \theta \) that gives the point \( (1,1) \): From \( x = e^\theta \sin \theta = 1 \) and \( y = e^\theta \cos \theta = 1 \) Divide both: \[ \frac{x}{y} = \frac{\sin \theta}{\cos \theta} = \tan \theta = 1 \Rightarrow \theta = \frac{\pi}{4} \] Substitute \( \theta = \frac{\pi}{4} \) into the expression: \[ \frac{dy}{dx} = \frac{\cos \theta - \sin \theta}{\sin \theta + \cos \theta} = \frac{\frac{1}{\sqrt{2}} - \frac{1}{\sqrt{2}}}{\frac{1}{\sqrt{2}} + \frac{1}{\sqrt{2}}} = \frac{0}{\frac{2}{\sqrt{2}}} = 0 \] Hence, \(\left. \frac{dy}{dx} \right|_{(1,1)} = 0\)
We are given x = eθ sin θ and y = eθ cos θ. We need to find dy/dx at the point (1, 1).
First, let's find dx/dθ and dy/dθ:
\(\frac{dx}{d\theta} = \frac{d}{d\theta}(e^\theta \sin \theta) = e^\theta \sin \theta + e^\theta \cos \theta = e^\theta(\sin \theta + \cos \theta)\)
\(\frac{dy}{d\theta} = \frac{d}{d\theta}(e^\theta \cos \theta) = e^\theta \cos \theta - e^\theta \sin \theta = e^\theta(\cos \theta - \sin \theta)\)
Now, we can find dy/dx using the chain rule:
\(\frac{dy}{dx} = \frac{dy/d\theta}{dx/d\theta} = \frac{e^\theta(\cos \theta - \sin \theta)}{e^\theta(\sin \theta + \cos \theta)} = \frac{\cos \theta - \sin \theta}{\sin \theta + \cos \theta}\)
Next, we need to find the value of θ for which x = 1 and y = 1:
eθ sin θ = 1
eθ cos θ = 1
Dividing the two equations:
\(\frac{e^\theta \sin \theta}{e^\theta \cos \theta} = \frac{1}{1}\)
tan θ = 1
θ = \(\frac{\pi}{4}\) (since x and y are both positive)
Now, substitute θ = π/4 into the expression for dy/dx:
\(\frac{dy}{dx} \Big|_{\theta = \frac{\pi}{4}} = \frac{\cos(\frac{\pi}{4}) - \sin(\frac{\pi}{4})}{\sin(\frac{\pi}{4}) + \cos(\frac{\pi}{4})} = \frac{\frac{1}{\sqrt{2}} - \frac{1}{\sqrt{2}}}{\frac{1}{\sqrt{2}} + \frac{1}{\sqrt{2}}} = \frac{0}{\frac{2}{\sqrt{2}}} = 0\)
Therefore, \(\left. \frac{dy}{dx} \right|_{(1,1)} = 0\)
Answer: 0
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: