Question #45522

A stamping machine produces ‘can tops’ whose diameters are normally distributed with a standard deviation of 0.02 inch. At what nominal mean diameter should the machine be set, so that no more than 9 % of the ‘can tops’ produced have diameters exceeding 3.5 inches?
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Expert's answer

2014-09-05T12:12:37-0400

Answer on Question #45522 - Math - Statistics and Probability

Normal distribution:


f(x,μ,σ)=1σ2πe(xμ)22σ2f(x, \mu, \sigma) = \frac{1}{\sigma \sqrt{2\pi}} e^{-\frac{(x - \mu)^2}{2\sigma^2}}


Where μ\mu — mean of the distribution, σ\sigma — standard deviation, f(x,μ,σ)f(x, \mu, \sigma) — probability density function, xx — variable.

Input of the task: σ=0.02\sigma = 0.02 inch, P(3.5<x)0.09P(3.5 < x) \leq 0.09 (9% corresponds to 9100=0.09\frac{9}{100} = 0.09), μ\mu — ?

P(3.5<x)P(3.5 < x) — probability of xx to be greater than 3.5 inches; xx — diameter of the "can tops".


P(3.5<x)=3.5f(x,μ,σ)dx=3.51σ2πe(xμ)22σ2dx0.09P(3.5 < x) = \int_{3.5}^{\infty} f(x, \mu, \sigma) \, dx = \int_{3.5}^{\infty} \frac{1}{\sigma \sqrt{2\pi}} e^{-\frac{(x - \mu)^2}{2\sigma^2}} \, dx \leq 0.09

σ=0.02\sigma = 0.02 (inch); σ2=0.022=0.0004\sigma^2 = 0.02^2 = 0.0004 (inch²);


3.51σ2πe(xμ)22σ2dx=3.510.022πe(xμ)22×0.0004dx=10.022π3.5e(xμ)20.0008dx0.093.5e(xμ)20.0008dx0.09×0.022π0.004512=4.512×103\begin{aligned} & \int_{3.5}^{\infty} \frac{1}{\sigma \sqrt{2\pi}} e^{-\frac{(x - \mu)^2}{2\sigma^2}} \, dx = \int_{3.5}^{\infty} \frac{1}{0.02\sqrt{2\pi}} e^{-\frac{(x - \mu)^2}{2 \times 0.0004}} \, dx = \frac{1}{0.02\sqrt{2\pi}} \int_{3.5}^{\infty} e^{-\frac{(x - \mu)^2}{0.0008}} \, dx \leq 0.09 \\ & \int_{3.5}^{\infty} e^{-\frac{(x - \mu)^2}{0.0008}} \, dx \leq 0.09 \times 0.02\sqrt{2\pi} \approx 0.004512 = 4.512 \times 10^{-3} \end{aligned}


Consider t=xμ0.0008t = \frac{x - \mu}{\sqrt{0.0008}}, dt=dx0.0008dt = \frac{dx}{\sqrt{0.0008}}, dx=0.0008×dt0.0283dtdx = \sqrt{0.0008} \times dt \approx 0.0283 \, dt.

Upper boundary: limxxμ0.0008=\lim_{x \to \infty} \frac{x - \mu}{\sqrt{0.0008}} = \infty; lower boundary: xμ0.00083.53.5μ0.028335.36(3.5μ)\left. \frac{x - \mu}{\sqrt{0.0008}} \right|_{3.5} \approx \frac{3.5 - \mu}{0.0283} \approx 35.36(3.5 - \mu);

Thus, 3.5e(xμ)20.0008dx=0.028335.36(3.5μ)et2dt4.512×103\int_{3.5}^{\infty} e^{-\frac{(x - \mu)^2}{0.0008}} \, dx = 0.0283 \int_{35.36(3.5 - \mu)}^{\infty} e^{-t^2} \, dt \leq 4.512 \times 10^{-3};

Consider a=35.36(3.5μ)a = 35.36(3.5 - \mu).


0.0283aet2dt4.512×103aet2dt159.435×1030.1594\begin{aligned} & 0.0283 \int_{a}^{\infty} e^{-t^2} \, dt \leq 4.512 \times 10^{-3} \\ & \int_{a}^{\infty} e^{-t^2} \, dt \leq 159.435 \times 10^{-3} \approx 0.1594 \end{aligned}


There is no elementary indefinite integral for et2dt\int e^{-t^2} \, dt, hence the only way is to use methods of numerical integration. Result: a0.94836a \geq 0.94836.

Thus, a=35.36(3.5μ)0.94836a = 35.36(3.5 - \mu) \geq 0.94836; μ0.9483635.363.5-\mu \geq \frac{0.94836}{35.36} - 3.5; μ3.50.9483635.36\mu \leq 3.5 - \frac{0.94836}{35.36};

μ3.50.02682\mu \leq 3.5 - 0.02682; μ3.47318\mu \leq 3.47318;

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