I. 0.0062,
II. 0.1562,
III. 0.8664.
Let us use the common notations. The burning time of an experimental rocket obeys a normal probability law with mean µ=4.76 seconds and standard deviation s = 0.04 seconds.
We have a random variable X normally distributed with mean µ and standard deviation s. To solve the problems, we note that Z = (X – 4.76)/0.04 is the standardized version of X. So, we have
P(X < 4.66) = FZ((4.66-4.76)/0.04),
P(X > 4.80) = 1 - P(X <= 4.80) = 1 - Fz((4.80-4.76)/0.04),
P(4.70 < X < 4.82) = FZ((4.82-4.76)/0.04) - FZ((4.70-4.76)/0.04),
where FZ(x) is the cumulative distribution function for a standard normal random variable.
Calculating the arguments and using tabulated values of the cumulative distribution function for a standard normal distribution, we obtain
P(X < 4.66) = FZ(–2.5) = 1 – FZ(2.5) = 1 – 0.9938 = 0.0062,
P(X > 4.80) = 1 – FZ(1.0) = 1 – 0.8413 = 0.1587,
P(4.70 < X < 4.82) = FZ(1.5) – FZ(–1.5) = FZ(1.5) – (1 – FZ(1.5)) = 0.8664.
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