4.5 Normal Distribution ======================= Key Terms --------- **Normal distribution**, **mean**, **standard deviation**, **variance**, **standardization**, **z-score**, **percentile**, **critical value**, **continuity correction**, **normal approximation**. Learning Outcomes ----------------- After studying this section, you should be able to: - describe the role of :math:`\mu` and :math:`\sigma` in a normal distribution; - convert values on an original measurement scale to the standard-normal scale; - calculate left-tail, right-tail, and interval probabilities; - find percentiles and cutoff values from probabilities; - interpret probabilities as areas under a normal density; - use a normal distribution to approximate selected discrete distributions; - apply the :math:`0.5` continuity correction correctly. 4.5.1 From the Standard Normal to the Normal Family ---------------------------------------------------- Section 4.4 introduced the standard normal random variable .. math:: Z\sim N(0,1). The standard normal distribution is one member of a much larger family. A general normal random variable may have any real-valued center and any positive standard deviation. Normal models often appear when an observed quantity is affected by many small influences. Examples include measurement error, process dimensions, biological measurements, test scores, and aggregated random effects. The key idea for probability calculations is simple: **Every normal distribution can be converted to the same standard-normal reference scale.** Thus, the :math:`z`-skills from Section 4.4 are the computational tool for working with all normal distributions. 4.5.2 Definition and Parameters -------------------------------- A continuous random variable :math:`X` follows a normal distribution if its density has the form .. math:: f(x) = \frac{1}{\sigma\sqrt{2\pi}} \exp\left[ -\frac{(x-\mu)^2}{2\sigma^2} \right], \qquad -\infty0. In this handout, the notation is .. math:: X\sim N(\mu,\sigma^2), so the second argument is the **variance**. The parameters have distinct roles: - :math:`\mu` controls **location**; - :math:`\sigma` controls **spread**; - :math:`\sigma^2` is the variance. For a normal random variable, .. math:: E(X)=\mu, \qquad \operatorname{Var}(X)=\sigma^2. The density is symmetric around :math:`\mu`, and the mean, median, and mode coincide at the center. Changing :math:`\mu` shifts the curve. Changing :math:`\sigma` changes the width and height while the total area remains 1. .. image:: ../_static/figures/continuous_distributions/figure_4_5_1_normal_location_spread.png :width: 92% :align: center The left plot illustrates a location change. The right plot keeps the center fixed and changes the spread. A larger :math:`\sigma` produces a wider, lower curve because the total probability area must remain equal to 1. 4.5.3 Probabilities Are Areas ------------------------------ For any continuous random variable, .. math:: P(X=x)=0. Therefore, .. math:: P(Xx)=P(X\geq x). For a normal random variable, probabilities are areas under the density curve. The general normal CDF does not have a simple elementary formula. Instead, we standardize the relevant boundary and use the standard normal CDF .. math:: \Phi(z)=P(Z\leq z). 4.5.4 Standardization: Moving from X to Z ----------------------------------------- Suppose .. math:: X\sim N(\mu,\sigma^2). Then .. note:: **Standardization** .. math:: Z = \frac{X-\mu}{\sigma} \sim N(0,1). For a particular value :math:`x`, .. math:: z=\frac{x-\mu}{\sigma}. The transformation subtracts the location and divides by the scale. Probability is preserved under this one-to-one transformation. For example, suppose electrical current is modeled as .. math:: X\sim N(10,2^2). Then :math:`x=13` corresponds to .. math:: z = \frac{13-10}{2} = 1.5. Therefore, .. math:: P(X>13) = P(Z>1.5). .. image:: ../_static/figures/continuous_distributions/figure_4_5_2_standardization_area_mapping.png :width: 92% :align: center The numerical scale changes, but the shaded probability area does not. The reverse transformation is equally important: .. math:: x=\mu+z\sigma. This form is used when a probability or percentile is given and the original measurement value is unknown. 4.5.5 Three Basic Probability Patterns --------------------------------------- Let .. math:: z_x=\frac{x-\mu}{\sigma}. For a left-tail probability, .. math:: P(Xx) = 1-\Phi(z_x). For an interval :math:`a13) = P(Z>1.50) = 1-\Phi(1.50). Using .. math:: \Phi(1.50)\approx0.9332, we obtain .. math:: P(X>13) \approx 1-0.9332 = 0.0668. So a current above 13 mA is unusual, but not impossible. **(b) Probability that current is below 13.06 mA** .. math:: z = \frac{13.06-10}{2} = 1.53. Therefore, .. math:: P(X<13.06) = \Phi(1.53) \approx 0.9370. **(c) Probability that current lies between 7.50 and 10.74 mA** The two standardized boundaries are .. math:: z_1 = \frac{7.50-10}{2} = -1.25 and .. math:: z_2 = \frac{10.74-10}{2} = 0.37. Hence, .. math:: P(7.50k-0.5)` * - :math:`P(X>k)` - :math:`P(Y>k+0.5)` * - :math:`P(X=k)` - :math:`P(k-0.582)`. 2. Suppose :math:`X\sim N(50,6^2)`. Find :math:`P(4482)\approx0.1151. 2. .. math:: z_1=-1, \qquad z_2=2, so .. math:: P(4424.5) \approx0.1572. 10. .. math:: P(X\leq3)\approx0.8932. 11. A single point has probability zero for a continuous random variable. 12. The binomial distribution is likely to remain strongly skewed because the expected number of successes is very small. 13. .. math:: 11.5