From problem 10 from book
the density of minimum value among n independent random variables with an exponential density has mean μ/n,
where μ is mean of exponential density of individual variable.
Here n = 100
μ=1000,
so the expected time for the first of the bulbs to burn out is
E(M)=μ/n
1000/100 = 10 hours
\(f_Z(z) = (1/2)e^{-\lambda|z|}\) can be re-written as \(f_Z(z) = \begin{cases} (1/2)e^{-\lambda z}, & \mbox{if } z \ge 0, \\ (1/2)e^{\lambda z}, & \mbox{if }z <0. \end{cases}\)
Since \(X_1\) and \(X_2\) have exponential density, their PDF is
\[ \begin{split} f_Z(z) &= f_{X_1+(-X_2)}(z) \\ &= \int_{-\infty}^{\infty} f_{-X_2}(z-x_1) f_{X_1}(x_1) dx_1 \\ &= \int_{-\infty}^{\infty} f_{X_2}(x_1-z) f_{X_1}(x_1) dx_1 \\ &= \int_{-\infty}^{\infty} \lambda e^{-\lambda(x_1-z)} \lambda e^{-\lambda x_1} dx_1 \\ &= \int_{-\infty}^{\infty} \lambda^2 e^{-\lambda x_1 + \lambda z} e^{-\lambda x_1} dx_1 \\ &= \int_{-\infty}^{\infty} \lambda^2 e^{\lambda z - \lambda x_1 - \lambda x_1} dx_1 \\ &= \int_{-\infty}^{\infty} \lambda^2 e^{\lambda(z-2x_1)} dx_1 \end{split} \]
Consider \(z=x_1-x_2\), then \(x_2=x_1-z\).
If \(z \ge 0\), then \(x_2=(x_1-z) \ge 0\), and \(x_1 \ge z\), and, using WolframAlpha, \(f_Z(z) = \int_{z}^{\infty} \lambda^2 e^{\lambda(z-2x_1)} dx_1 = \frac{1}{2} \lambda e^{-\lambda z}\).
If \(z < 0\), then \(x_2=(x_1-z) \ge 0\), and \(x_1 \ge 0\), and \(f_Z(z) = \int_{0}^{\infty} \lambda^2 e^{\lambda(z-2x_1)} dx_1 =\frac{1}{2} \lambda e^{\lambda z}\).
Combining two sides we get \(f_Z(z) = \begin{cases} (1/2)e^{-\lambda z}, & \mbox{if } z \ge 0, \\ (1/2)e^{\lambda z}, & \mbox{if }z <0. \end{cases}\)
P(|X−10|≥2) P(|X−10|≥5) P(|X−10|≥9) P(|X−10|≥20)
here mean μ=10
variance \(σ^2=100/3\)
Standarddeviation σ = sqrt(100/3)
\(P(|X−μ|≥kσ)≤1/k^2\)
\(kσ = 2\)
\(k = \frac2{\sqrt{100/3}}\)
\(P(|X−10|⩾2)=1/k^2 = 8.3333≈1\)
\(kσ = 5\)
\(k = \frac5{\sqrt{100/3}}\)
\(P(|X−10|⩾5)=1k2=1.3333≈1\)
\(kσ=9\)
\(k = \frac9{\sqrt{100/3}}\)
\(P(|X−10|⩾9)=1k2=0.4115\)
\(kσ=20\)
\(k = \frac{20}{\sqrt{100/3}}\)
\(P(|X−10|⩾20)=1k2=0.0833\)