We are given the integral \( \int \frac{e^x}{1+x} \, dx \). We will use integration by parts.
Let:
Using the formula for integration by parts, \( \int u \, dv = uv - \int v \, du \), we get:
\[ \int \frac{e^x}{1+x} \, dx = \frac{e^x}{1+x} - \int e^x \left( -\frac{1}{(1+x)^2} \right) dx \]
Now, simplifying the expression:
\[ \int \frac{e^x}{1+x} \, dx = \frac{e^x}{1+x} + \int \frac{e^x}{(1+x)^2} \, dx \]
At this point, we notice that the integral \( \int \frac{e^x}{(1+x)^2} \, dx \) appears again. Therefore, we can isolate the original integral on one side:
\[ \int \frac{e^x}{1+x} \, dx - \int \frac{e^x}{(1+x)^2} \, dx = \frac{e^x}{1+x} \]
Now, substitute the value of the second integral back into the equation:
\[ \int \frac{e^x}{1+x} \, dx = \frac{e^x}{1+x} + C \]
Thus, the value of the integral is:
\[ \int \frac{e^x}{1+x} \, dx = \frac{e^x}{1+x} + C \]
We are given the integral:
\[ \int \frac{x e^x}{(1 + x)^2} \, dx \]
Step 1: Use substitution
Let \( u = 1 + x \), so that \( du = dx \), and \( x = u - 1 \). The integral becomes:
\[ \int \frac{(u - 1) e^{u - 1}}{u^2} \, du \]
Step 2: Simplify the expression
Since \( e^{u - 1} = \frac{e^u}{e} \), the integral becomes:
\[ \frac{1}{e} \int \left( \frac{e^u}{u} - \frac{e^u}{u^2} \right) \, du \]
Step 3: Solve the integrals
The integral of \( \frac{e^u}{u^2} \) is \( -\frac{e^u}{u} \), and after simplification, the result is:
\[ \frac{e^x}{1 + x} + c \]
The correct answer is (D): \(\frac{e^x}{1+x} + c\).
A block of certain mass is placed on a rough floor. The coefficients of static and kinetic friction between the block and the floor are 0.4 and 0.25 respectively. A constant horizontal force \( F = 20 \, \text{N} \) acts on it so that the velocity of the block varies with time according to the following graph. The mass of the block is nearly (Take \( g = 10 \, \text{m/s}^2 \)):
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