e+1/2 \(e+\frac {1}{2}\)
\(-\frac {1}{2}\)
We begin by determining the integrating factor (IF):
ex: IF=e−∫t1+tdt=e−∫t+11+tdt=e−t+log(1+t)=1+te−t.
The sought-after solution can be expressed as y(IF)=∫Q⋅IFdt+C, where Q=11+t is derived from the given equation.
Thus, y(IF)=∫11+t⋅1+te−tdt+C,
=∫e−tdt+C,
=−e−t+C.
Given the initial condition y(0)=−1, we find:
−1⋅(1+0)=−e0+C,
−1=−1+C,
C=0.
Plugging the value of C back in, we have:
y(IF)=−e−t+0,
=−e−t.
Evaluating at t=1:
y(IF)=−e−1,
\(=-\frac {1}{e}\)
above is example. but here proves that : \(-\frac {1}{2}\)
Let $ y(x) $ be the solution of the differential equation $$ x^2 \frac{dy}{dx} + xy = x^2 + y^2, \quad x > \frac{1}{e}, $$ satisfying $ y(1) = 0 $. Then the value of $ 2 \cdot \frac{(y(e))^2}{y(e^2)} $ is ________.
The left and right compartments of a thermally isolated container of length $L$ are separated by a thermally conducting, movable piston of area $A$. The left and right compartments are filled with $\frac{3}{2}$ and 1 moles of an ideal gas, respectively. In the left compartment the piston is attached by a spring with spring constant $k$ and natural length $\frac{2L}{5}$. In thermodynamic equilibrium, the piston is at a distance $\frac{L}{2}$ from the left and right edges of the container as shown in the figure. Under the above conditions, if the pressure in the right compartment is $P = \frac{kL}{A} \alpha$, then the value of $\alpha$ is ____
Let $ S $ denote the locus of the point of intersection of the pair of lines $$ 4x - 3y = 12\alpha,\quad 4\alpha x + 3\alpha y = 12, $$ where $ \alpha $ varies over the set of non-zero real numbers. Let $ T $ be the tangent to $ S $ passing through the points $ (p, 0) $ and $ (0, q) $, $ q > 0 $, and parallel to the line $ 4x - \frac{3}{\sqrt{2}} y = 0 $.
Then the value of $ pq $ is
A differential equation is an equation that contains one or more functions with its derivatives. The derivatives of the function define the rate of change of a function at a point. It is mainly used in fields such as physics, engineering, biology and so on.
The first-order differential equation has a degree equal to 1. All the linear equations in the form of derivatives are in the first order. It has only the first derivative such as dy/dx, where x and y are the two variables and is represented as: dy/dx = f(x, y) = y’
The equation which includes second-order derivative is the second-order differential equation. It is represented as; d/dx(dy/dx) = d2y/dx2 = f”(x) = y”.
Differential equations can be divided into several types namely