We are given the differential equation:
\[\frac{dy}{dx} = 2x(x + y)^3 - x(x + y) - 1\]
Let \( x + y = t \). Therefore, we have:
\[\frac{dt}{dx} = 2xt^3 - xt - 1\]
This simplifies to:
\[\frac{dt}{dx} = t^2 \quad \text{and} \quad \frac{dt}{dx} = x^2 \text{ for } x = 0\]
Now solve the equation:
\[\int \frac{dz}{2(2z - z)} = \int x dx\]
After solving:
\[\ln \left( \frac{z - 1}{z} \right) = x^2 + k\]
Thus, \( z = \frac{1}{2 - \sqrt{e}} \).
Given the differential equation \( \frac{dy}{dx} = 2x(x + y)^3 - x(x + y) - 1 \) with \( y(0) = 1 \), we need to find \( \left( \frac{1}{\sqrt{2}} + y\left(\frac{1}{\sqrt{2}}\right) \right)^2 \).
When a differential equation involves \( x+y \) repeatedly, a substitution \( t = x + y \) can simplify it. Then \( \frac{dt}{dx} = 1 + \frac{dy}{dx} \), which can be used to transform the equation into a separable or simpler form.
Step 1: Substitute \( t = x + y \). Then \( \frac{dt}{dx} = 1 + \frac{dy}{dx} \).
From the given equation:
\[ \frac{dy}{dx} = 2x t^3 - x t - 1 \]
So:
\[ \frac{dt}{dx} = 1 + \left( 2x t^3 - x t - 1 \right) = 2x t^3 - x t \] \[ \frac{dt}{dx} = x t (2 t^2 - 1) \]
Step 2: Separate variables and integrate.
\[ \frac{dt}{t(2 t^2 - 1)} = x \, dx \]
Factor the denominator: \( 2 t^2 - 1 = 2\left(t^2 - \frac12\right) \).
Use partial fractions for \( \frac{1}{t(2 t^2 - 1)} \).
Let \( \frac{1}{t(2 t^2 - 1)} = \frac{A}{t} + \frac{B t + C}{2 t^2 - 1} \).
Multiply through by \( t(2 t^2 - 1) \):
\[ 1 = A(2 t^2 - 1) + (B t + C) t = 2A t^2 - A + B t^2 + C t \] \[ 1 = (2A + B) t^2 + C t - A \]
Comparing coefficients:
\( 2A + B = 0 \) … (1)
\( C = 0 \) … (2)
\( -A = 1 \Rightarrow A = -1 \) … (3)
From (1): \( 2(-1) + B = 0 \Rightarrow B = 2 \).
Thus:
\[ \frac{1}{t(2 t^2 - 1)} = -\frac{1}{t} + \frac{2 t}{2 t^2 - 1} \]
Step 3: Integrate both sides.
\[ \int \left( -\frac{1}{t} + \frac{2 t}{2 t^2 - 1} \right) dt = \int x \, dx \] \[ - \ln |t| + \frac12 \ln |2 t^2 - 1| = \frac{x^2}{2} + C \]
Rewriting:
\[ \ln \left| \frac{\sqrt{2 t^2 - 1}}{t} \right| = \frac{x^2}{2} + C \] \[ \frac{\sqrt{2 t^2 - 1}}{t} = K e^{x^2 / 2}, \quad K = \pm e^C \]
Step 4: Use initial condition \( y(0) = 1 \) ⇒ \( t(0) = 0 + 1 = 1 \).
\[ \frac{\sqrt{2 (1)^2 - 1}}{1} = K e^{0} \Rightarrow \frac{\sqrt{1}}{1} = K \Rightarrow K = 1 \]
So:
\[ \frac{\sqrt{2 t^2 - 1}}{t} = e^{x^2 / 2} \] \[ \sqrt{2 t^2 - 1} = t e^{x^2 / 2} \]
Step 5: Square both sides:
\[ 2 t^2 - 1 = t^2 e^{x^2} \] \[ 2 t^2 - t^2 e^{x^2} = 1 \] \[ t^2 (2 - e^{x^2}) = 1 \] \[ t^2 = \frac{1}{2 - e^{x^2}} \]
Recall \( t = x + y \).
Step 6: Evaluate \( \left( \frac{1}{\sqrt{2}} + y\left(\frac{1}{\sqrt{2}}\right) \right)^2 \).
Let \( x_0 = \frac{1}{\sqrt{2}} \), then \( t_0 = x_0 + y(x_0) \).
\[ t_0^2 = \frac{1}{2 - e^{x_0^2}} = \frac{1}{2 - e^{1/2}} \]
So:
\[ \left( \frac{1}{\sqrt{2}} + y\left(\frac{1}{\sqrt{2}}\right) \right)^2 = t_0^2 = \frac{1}{2 - \sqrt{e}} \]
Therefore, the required value is \( \mathbf{\frac{1}{2 - \sqrt{e}}} \).
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,