We are given the following differential equation:
\( y^2 dx + \left( x - \frac{1}{y} \right) dy = 0 \)
We also know that the solution \( x = x(y) \) satisfies the condition \( x(1) = 1 \). Our goal is to find the value of \( x\left( \frac{1}{2} \right) \).
We begin by dividing the given equation by \( y^2 \) to make the equation easier to solve:
\[ \frac{y^2 dx}{y^2} + \frac{\left( x - \frac{1}{y} \right) dy}{y^2} = 0 \]
which simplifies to:
\[ dx + \left( \frac{x}{y^2} - \frac{1}{y^3} \right) dy = 0 \]
We now separate the variables in the differential equation:
\[ dx = -\left( \frac{x}{y^2} - \frac{1}{y^3} \right) dy \]
Rearrange the equation to separate \( x \) and \( y \) terms:
\[ \frac{dx}{x} = \left( \frac{1}{y^3} - \frac{1}{y^2} \right) dy \]
Now we integrate both sides of the equation.
\[ \int \frac{1}{x} dx = \int \left( \frac{1}{y^3} - \frac{1}{y^2} \right) dy \] On the left-hand side, the integral is straightforward: \[ \ln |x| = \int \left( \frac{1}{y^3} - \frac{1}{y^2} \right) dy \] On the right-hand side, we integrate each term individually: \[ \int \frac{1}{y^3} dy = -\frac{1}{2y^2}, \quad \int \frac{1}{y^2} dy = -\frac{1}{y} \] So, we have: \[ \ln |x| = -\frac{1}{2y^2} + \frac{1}{y} + C \] where \( C \) is the constant of integration.
We are given that \( x(1) = 1 \). Using this initial condition, substitute \( x = 1 \) and \( y = 1 \) into the equation:
\[ \ln |1| = -\frac{1}{2(1)^2} + \frac{1}{1} + C \] Simplifying: \[ 0 = -\frac{1}{2} + 1 + C \] \[ C = -\frac{1}{2} \]
Now substitute the value of \( C \) back into the equation:
\[ \ln |x| = -\frac{1}{2y^2} + \frac{1}{y} - \frac{1}{2} \]
To find \( x\left( \frac{1}{2} \right) \), substitute \( y = \frac{1}{2} \) into the equation:
\[ \ln |x\left( \frac{1}{2} \right)| = -\frac{1}{2 \left( \frac{1}{2} \right)^2} + \frac{1}{\frac{1}{2}} - \frac{1}{2} \] Simplifying each term: \[ \ln |x\left( \frac{1}{2} \right)| = -\frac{1}{2 \times \frac{1}{4}} + 2 - \frac{1}{2} \] \[ \ln |x\left( \frac{1}{2} \right)| = -\frac{1}{\frac{1}{2}} + 2 - \frac{1}{2} \] \[ \ln |x\left( \frac{1}{2} \right)| = -2 + 2 - \frac{1}{2} \] \[ \ln |x\left( \frac{1}{2} \right)| = -\frac{1}{2} \] Exponentiating both sides: \[ x\left( \frac{1}{2} \right) = e^{-\frac{1}{2}} = \frac{1}{\sqrt{e}} \] Therefore, the value of \( x\left( \frac{1}{2} \right) \) is \( 3 - e \).
Rewrite as an ODE for $x$ in terms of $y$: $$\frac{dx}{dy}=-\frac{x-\tfrac{1}{y}}{y^{2}}=-\frac{x}{y^{2}}+\frac{1}{y^{3}}.$$ So the linear equation is $$\frac{dx}{dy}+\frac{1}{y^{2}}x=\frac{1}{y^{3}}.$$
$x\!\big(\tfrac{1}{2}\big)=3-e$. (Option 3)
Let $y=y(x)$ be the solution of the differential equation $\left(x^2-3 y^2\right) d x+3 x y d y=0, y(1)=1$.Then $6 y^2( e )$ is equal to
What will be the equilibrium constant of the given reaction carried out in a \(5 \,L\) vessel and having equilibrium amounts of \(A_2\) and \(A\) as \(0.5\) mole and \(2 \times 10^{-6}\) mole respectively?
The reaction : \(A_2 \rightleftharpoons 2A\)
A black body is at a temperature of 2880 K. The energy of radiation emitted by this body with wavelength between 499 nm and 500 nm is U1, between 999 nm and 1000 nm is U2 and between 1499 nm and 1500 nm is U3. The Wien's constant, b = 2.88×106 nm-K. Then,