E ( x ) = ∫ − ∞ + ∞ x f ( x ) d x = ∫ 0 1 x ( a + b x 2 ) d x ⇒ ∫ 0 1 ( a x + b x 3 ) d x = 3 5 ⇒ 1 2 a x 2 ∣ 0 1 + 1 4 b x 4 ∣ 0 1 = 3 5 ⇒ a 2 + b 4 = 3 5 ⇒ 2 a + b 4 = 3 5 ⇒ 2 a + b = 12 5 E(x) = \int\limits_{ - \infty }^{ + \infty } {xf(x)dx} = \int\limits_0^1 {x(a + b{x^2}} )dx \Rightarrow \int\limits_0^1 {\left( {ax + b{x^3}} \right)} dx = \frac{3}{5} \Rightarrow \frac{1}{2}a\left. {{x^2}} \right|_0^1 + \frac{1}{4}b\left. {{x^4}} \right|_0^1 = \frac{3}{5} \Rightarrow \frac{a}{2} + \frac{b}{4} = \frac{3}{5} \Rightarrow \frac{{2a + b}}{4} = \frac{3}{5} \Rightarrow 2a + b = \frac{{12}}{5} E ( x ) = − ∞ ∫ + ∞ x f ( x ) d x = 0 ∫ 1 x ( a + b x 2 ) d x ⇒ 0 ∫ 1 ( a x + b x 3 ) d x = 5 3 ⇒ 2 1 a x 2 ∣ ∣ 0 1 + 4 1 b x 4 ∣ ∣ 0 1 = 5 3 ⇒ 2 a + 4 b = 5 3 ⇒ 4 2 a + b = 5 3 ⇒ 2 a + b = 5 12
Next, we use the properties of the density function
∫ − ∞ + ∞ f ( x ) d x = 1 ⇒ ∫ 0 1 ( a + b x 2 ) d x = 1 ⇒ a x ∣ 0 1 + 1 3 b x 3 ∣ 0 1 = 1 ⇒ a + 1 3 b = 1 \int\limits_{ - \infty }^{ + \infty } {f(x)dx} = 1 \Rightarrow \int\limits_0^1 {(a + b{x^2}} )dx = 1 \Rightarrow a\left. x \right|_0^1 + \frac{1}{3}b\left. {{x^3}} \right|_0^1 = 1 \Rightarrow a + \frac{1}{3}b = 1 − ∞ ∫ + ∞ f ( x ) d x = 1 ⇒ 0 ∫ 1 ( a + b x 2 ) d x = 1 ⇒ a x ∣ 0 1 + 3 1 b x 3 ∣ ∣ 0 1 = 1 ⇒ a + 3 1 b = 1
We have the system
{ a + 1 3 b = 1 2 a + b = 12 5 ⇒ { 3 a + b = 3 10 a + 5 b = 12 ⇒ a = 3 5 , b = 6 5 \left\{ \begin{array}{l}
a + \frac{1}{3}b = 1\\
2a + b = \frac{{12}}{5}
\end{array} \right. \Rightarrow \left\{ \begin{array}{l}
3a + b = 3\\
10a + 5b = 12
\end{array} \right. \Rightarrow a = \frac{3}{5},\,\,b = \frac{6}{5} { a + 3 1 b = 1 2 a + b = 5 12 ⇒ { 3 a + b = 3 10 a + 5 b = 12 ⇒ a = 5 3 , b = 5 6
Answer: a = 3 5 , b = 6 5 a = \frac{3}{5},\,\,b = \frac{6}{5} a = 5 3 , b = 5 6