e2+\(\frac{4}{3}\)
loge4+\(\frac{e}{3}\)
\(\frac{4e^2}{3}\)
e2-\(^{\frac{4}{3}}\)
To find the value of \( f(e) \), we start by differentiating both sides of the given equation with respect to \( x \):
Given,
\[ 3 \int_{1}^{x} f(t) \, dt = x f(x) - \frac{x^3}{3} \]
Differentiating both sides using the Fundamental Theorem of Calculus and the Leibniz rule:
\[ \frac{d}{dx}\left[3 \int_{1}^{x} f(t) \, dt\right] = \frac{d}{dx}\left[ x f(x) - \frac{x^3}{3} \right] \]
This implies:
\[ 3 f(x) = f(x) + x \frac{d f}{dx} - x^2 \]
Rearranging terms, we get:
\[ 2 f(x) = x \frac{d f}{dx} - x^2 \]
Adding \( x^2 \) and dividing by \( x \), we simplify:
\[ \frac{d f}{dx} = \frac{2 f(x) + x^2}{x} \]
Let \( u = f(x) \), then:
\[ \frac{d u}{dx} = \frac{2 u}{x} + x \]
This is a first-order linear differential equation that we solve using the integrating factor method:
Identifying \( P(x) = \frac{2}{x} \), the integrating factor \( \mu(x) = e^{\int P(x) \, dx} = e^{2 \ln x} = x^2 \).
Multiplying the differential equation by the integrating factor:
\[ x^2 \frac{d u}{dx} = 2 u + x^3 \]
Which simplifies to:
\[ x^2 \frac{d u}{dx} = (2 u + x^3) \]
The left side simplifies to \( \frac{d}{dx}(x^2 u) \), giving:
\[ \frac{d}{dx}(x^2 u) = x^3 \]
Integrating both sides:
\[ x^2 u = \frac{x^4}{4} + C \]
Solving for \( u = f(x) \):
\[ f(x) = \frac{x^4}{4x^2} + \frac{C}{x^2} = \frac{x^2}{4} + \frac{C}{x^2} \]
Using the initial condition \( f(1) = \frac{1}{3} \):
\[ \frac{1}{3} = \frac{1}{4} + C \]
Solving for \( C \):
\[ C = \frac{1}{3} - \frac{1}{4} = \frac{4-3}{12} = \frac{1}{12} \]
Thus, the function \( f(x) \) is:
\[ f(x) = \frac{x^2}{4} + \frac{1}{12x^2} \]
Finally, we find \( f(e) \):
\[ f(e) = \frac{e^2}{4} + \frac{1}{12 e^2} \]
Evaluating this expression, we find that the closest answer is:
\[ \frac{4 e^2}{3} \]
The correct answer is \( \boxed{\frac{4 e^2}{3}} \).
The correct option is (C) : \(\frac{4e^2}{3}\)
Evaluate: \[ \int_1^5 \left( |x-2| + |x-4| \right) \, dx \]
Figure 1 shows the configuration of main scale and Vernier scale before measurement. Fig. 2 shows the configuration corresponding to the measurement of diameter $ D $ of a tube. The measured value of $ D $ is:
The center of a disk of radius $ r $ and mass $ m $ is attached to a spring of spring constant $ k $, inside a ring of radius $ R>r $ as shown in the figure. The other end of the spring is attached on the periphery of the ring. Both the ring and the disk are in the same vertical plane. The disk can only roll along the inside periphery of the ring, without slipping. The spring can only be stretched or compressed along the periphery of the ring, following Hooke’s law. In equilibrium, the disk is at the bottom of the ring. Assuming small displacement of the disc, the time period of oscillation of center of mass of the disk is written as $ T = \frac{2\pi}{\omega} $. The correct expression for $ \omega $ is ( $ g $ is the acceleration due to gravity):
Given below is the list of the different methods of integration that are useful in simplifying integration problems:
If f(x) and g(x) are two functions and their product is to be integrated, then the formula to integrate f(x).g(x) using by parts method is:
∫f(x).g(x) dx = f(x) ∫g(x) dx − ∫(f′(x) [ ∫g(x) dx)]dx + C
Here f(x) is the first function and g(x) is the second function.
The formula to integrate rational functions of the form f(x)/g(x) is:
∫[f(x)/g(x)]dx = ∫[p(x)/q(x)]dx + ∫[r(x)/s(x)]dx
where
f(x)/g(x) = p(x)/q(x) + r(x)/s(x) and
g(x) = q(x).s(x)
Hence the formula for integration using the substitution method becomes:
∫g(f(x)) dx = ∫g(u)/h(u) du
This method of integration is used when the integration is of the form ∫g'(f(x)) f'(x) dx. In this case, the integral is given by,
∫g'(f(x)) f'(x) dx = g(f(x)) + C