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Statistics for the Behavioral Sciences by Frederick J. Gravetter, Larry B. Wallnau ISBN 10: 1305504917 ISBN 13: 9781305504912

Statistics is one of the most practical and essential courses that you will take, and a primary goal of this popular text is to make the task of learning statistics as simple as possible. Straightforward instruction, built-in learning aids, and real-world examples have made STATISTICS FOR THE BEHAVIORAL SCIENCES, 10th Edition the text selected most often by instructors for their students in the behavioral and social sciences. The authors provide a conceptual context that makes it easier to learn formulas and procedures, explaining why procedures were developed and when they should be used. This text will also instill the basic principles of objectivity and logic that are essential for science and valuable in everyday life, making it a useful reference long after you complete the course.

Statistics is one of the most practical and essential courses that you will take, and a primary goal of this popular text is to make the task of learning statistics as simple as possible. Straightforward instruction, built-in learning aids, and real-world examples have made STATISTICS FOR THE BEHAVIORAL SCIENCES, 10th Edition the text selected most often by instructors for their students in the behavioral and social sciences. The authors provide a conceptual context that makes it easier to learn formulas and procedures, explaining why procedures were developed and when they should be used. This text will also instill the basic principles of objectivity and logic that are essential for science and valuable in everyday life, making it a useful reference long after you complete the course.

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SECTION 7.3 | Probability and the Distribution of Sample Means 207

Caution: Whenever

you have a probability

question about a sample

mean, you must use the

distribution of sample

means.

Although we cannot construct the distribution of sample means by repeatedly taking

samples and calculating means (as in Example 7.1), we know exactly what the distribution

looks like based on the information from the central limit theorem. Specifically, the distribution

of sample means has the following characteristics:

1. The distribution is normal because the population of SAT scores is normal.

2. The distribution has a mean of 500 because the population mean is μ = 500.

3. For n = 16, the distribution has a standard error of σ M

= 25:

s M

5 s Ïn 5 100

Ï16 5 100

4 5 25

This distribution of sample means is shown in Figure 7.5.

We are interested in sample means greater than 525 (the shaded area in Figure 7.5), so

the next step is to use a z-score to locate the exact position of M = 525 in the distribution.

The value 525 is located above the mean by 25 points, which is exactly 1 standard deviation

(in this case, exactly 1 standard error). Thus, the z-score for M = 525 is z = +1.00.

Because this distribution of sample means is normal, you can use the unit normal table

to find the probability associated with z = +1.00. The table indicates that 0.1587 of the

distribution is located in the tail of the distribution beyond z = +1.00. Our conclusion is

that it is relatively unlikely, p = 0.1587 (15.87%), to obtain a random sample of n = 16

students with an average SAT score greater than 525.

■ A z-Score for Sample Means

As demonstrated in Example 7.3, it is possible to use a z-score to describe the exact location

of any specific sample mean within the distribution of sample means. The z-score tells

exactly where the sample mean is located in relation to all the other possible sample means

that could have been obtained. As defined in Chapter 5, a z-score identifies the location

with a signed number so that

1. The sign tells whether the location is above (+) or below (–) the mean.

2. The number tells the distance between the location and the mean in terms of the

number of standard deviations.

s M 525

FIGURE 7.5

The distribution of sample

means for n = 16. Samples

were selected from a normal

population with μ = 500 and

σ = 100.

500 525

m

550

0 1 2

M

z

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