We are given:
\[ \frac{dy}{dx} = (x + y)^2 \] Let us use substitution. Let:
\[ z = x + y \quad \Rightarrow \quad \frac{dz}{dx} = 1 + \frac{dy}{dx} \] Since \(\frac{dy}{dx} = (x + y)^2 = z^2\), we get: \[ \frac{dz}{dx} = 1 + z^2 \] Now separate the variables: \[ \frac{1}{1 + z^2} \, dz = dx \] Integrate both sides: \[ \int \frac{1}{1 + z^2} \, dz = \int dx \quad \Rightarrow \quad \tan^{-1}(z) = x + c \] Recall \(z = x + y\), so: \[ \tan^{-1}(x + y) = x + c \] ✅ Correct answer: \(\tan^{-1}(x + y) = x + c\)
Given the differential equation:
\[ \frac{dy}{dx} = (x+y)^2 \]
This equation is not directly separable or linear. We can use a substitution to simplify it. Let:
\(u = x + y\)
Differentiate both sides with respect to \(x\):
\[ \frac{du}{dx} = \frac{d}{dx}(x) + \frac{d}{dx}(y) \] \[ \frac{du}{dx} = 1 + \frac{dy}{dx} \]
Rearrange to express \(\frac{dy}{dx}\) in terms of \(\frac{du}{dx}\):
\[ \mathbf{\frac{dy}{dx} = \frac{du}{dx} - 1} \]
Now substitute \(u = x+y\) and \(\frac{dy}{dx} = \frac{du}{dx} - 1\) into the original differential equation:
\[ \frac{du}{dx} - 1 = u^2 \]
Rearrange the equation to separate variables \(u\) and \(x\):
\[ \frac{du}{dx} = u^2 + 1 \]
\[ \frac{du}{u^2 + 1} = dx \]
Integrate both sides:
\[ \int \frac{1}{u^2 + 1} \, du = \int 1 \, dx \]
The integral on the left is a standard integral form:
\[ \int \frac{1}{u^2 + 1} \, du = \tan^{-1}(u) \]
The integral on the right is:
\[ \int 1 \, dx = x + c \]
where \(c\) is the constant of integration.
Equating the results of the integration:
\[ \tan^{-1}(u) = x + c \]
Finally, substitute back \(u = x + y\):
\[ \mathbf{\tan^{-1}(x+y) = x + c} \]
Comparing this with the given options, the correct option is:
\(\tan^{-1}(x+y) = x + c\)
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 ________.
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: