To solve the given differential equation:
\[ x \cos\left(\frac{y}{x}\right) \frac{dy}{dx} = y \cos\left(\frac{y}{x}\right) + x \]
We note that it is in a format that can be addressed by assuming a substitution:
Let \( z = \frac{y}{x} \). This gives \( y = zx \) and differentiating with respect to \( x \), we have:
\(\frac{dy}{dx} = z + x \frac{dz}{dx}\)
Substitute in the differential equation:
\[ x \cos(z) (z + x \frac{dz}{dx}) = zx \cos(z) + x \]
On simplifying, we get:
\[ xz \cos(z) + x^2 \cos(z) \frac{dz}{dx} = zx \cos(z) + x \]
Cancel terms and simplify:
\[ x^2 \cos(z) \frac{dz}{dx} = x(1 - z \cos(z)) \]
Which simplifies to:
\[ \frac{dz}{dx} = \frac{1 - z \cos(z)}{x \cos(z)} \]
Let's separate the variables and integrate:
\[ \int \frac{\cos(z)}{1 - z \cos(z)} \, dz = \int \frac{1}{x} \, dx \]
On the right side, integrate:
\[ \int \frac{1}{x} \, dx = \log_e |x| + C \]
Let's consider the solution format provided in the question:
\[ \sin\left(\frac{y}{x}\right) = \log_e |x| + \frac{\alpha}{2} \]
At point \( x = 1, y = \frac{\pi}{3} \), substituting these values gives:
\[ \sin\left(\frac{\pi}{3}\right) = \log_e |1| + \frac{\alpha}{2} \]
Since \(\sin\left(\frac{\pi}{3}\right) = \frac{\sqrt{3}}{2}\) and \(\log_e |1| = 0\), we have:
\[ \frac{\sqrt{3}}{2} = 0 + \frac{\alpha}{2} \]
This implies:
\[ \alpha = \sqrt{3} \]
Thus, \(\alpha^2 = (\sqrt{3})^2 = 3\).
Therefore, the correct answer is 3.
Starting with the differential equation:
\(x \cos \left( \frac{y}{x} \right) \frac{dy}{dx} = y \cos \left( \frac{y}{x} \right) + x\)
Step 1. Divide both sides by \( x^2 \cos \left( \frac{y}{x} \right) \):
\(\cos \left( \frac{y}{x} \right) \left( \frac{y}{x} \frac{dy}{dx} - \frac{y}{x^2} \right) = \frac{1}{x}\)
Step 2. Let \( \frac{y}{x} = t \), then \( y = tx \) and \( \frac{dy}{dx} = t + x \frac{dt}{dx} \), substituting into the equation:
\(\cos t \left( \frac{dt}{dx} \right) = \frac{1}{x}\)
Step 3. Integrate both sides:
\(\sin t = \ln |x| + c\)
\(\sin \frac{y}{x} = \ln |x| + c\)
Step 4. Using the initial condition \( y(1) = \frac{\sqrt{3}}{2} \), we find \( c = \frac{\sqrt{3}}{2} \).
Thus, \( \alpha = \sqrt{3} \implies \alpha^2 = 3\)
The Correct Answer is: 3
A settling chamber is used for the removal of discrete particulate matter from air with the following conditions. Horizontal velocity of air = 0.2 m/s; Temperature of air stream = 77°C; Specific gravity of particle to be removed = 2.65; Chamber length = 12 m; Chamber height = 2 m; Viscosity of air at 77°C = 2.1 × 10\(^{-5}\) kg/m·s; Acceleration due to gravity (g) = 9.81 m/s²; Density of air at 77°C = 1.0 kg/m³; Assume the density of water as 1000 kg/m³ and Laminar condition exists in the chamber.
The minimum size of particle that will be removed with 100% efficiency in the settling chamber (in $\mu$m is .......... (round off to one decimal place).
Consider an A.P. $a_1,a_2,\ldots,a_n$; $a_1>0$. If $a_2-a_1=-\dfrac{3}{4}$, $a_n=\dfrac{1}{4}a_1$, and \[ \sum_{i=1}^{n} a_i=\frac{525}{2}, \] then $\sum_{i=1}^{17} a_i$ is equal to
