To solve the problem, we need to determine the value of \( g(3) \) given the function \( f(x) \) and the conditions for continuity and differentiability at specific points.
Step 1: Understand the function \( f(x) \) and conditions.
Step 2: Find conditions for continuity at \( x = 0 \).
Step 3: Evaluate \(\lim_{x \to 0^+} \left( \frac{1 + x}{2 + x} \right)^{\frac{1}{x}}\).
Simplifying and applying the condition of continuity: \(g(0) = 1.\)
Step 4: Use differentiability condition at \( x = 1 \).
Complex form of derivative will yield \(f'(x) = \ldots\). Evaluating \( x = 1 \), and substition using continuity condition:
Step 5: Substituting using options for correctness:
Thus the value of \( g(3) \) is \(\boxed{\log_e \left( \frac{4}{9e^{1/3}} \right)}\).
Let \( g(x) = ax + b \).
Now function \( f(x) \) is continuous at \( x = 0 \).
\[ \therefore \lim_{x \to 0} f(x) = f(0) \] \[ \lim_{x \to 0} \left( 1 + x \over 2 + x \right)^{1 \over x} = b \] \[ \Rightarrow 0 = b \] \[ \therefore g(x) = ax \]
Now, for \( x > 0 \),
\[ f'(x) = \frac{1}{x} \left( 1 + x \over 2 + x \right)^{1 \over x} \cdot \frac{1}{(2 + x)^2} + \left( 1 + x \over 2 + x \right)^{1 \over x} \cdot \ln \left( 1 + x \over 2 + x \right) \cdot \frac{1}{x^2} \] \[ f'(1) = \frac{1}{9} - \frac{2}{3} \ln \left( \frac{2}{3} \right) \]
And \( f(-1) = g(-1) = -a \)
\[ a = 2 \ln \left( \frac{2}{3} \right) - \frac{1}{9} \] \[ g(3) = 2 \ln \left( \frac{2}{3} \right) - \frac{1}{3} \] \[ = \ln \left( \frac{4}{9 e^{-1/3}} \right) \]
Two positively charged particles \(m_1\) and \(m_2\) have been accelerated across the same potential difference of 200 keV. Given mass of \(m_1 = 1 \,\text{amu}\) and \(m_2 = 4 \,\text{amu}\). The de Broglie wavelength of \(m_1\) will be \(x\) times that of \(m_2\). The value of \(x\) is _______ (nearest integer). 