central limit theoremdistributionsnormal distribution
In a normal distribution ,as far as I know distribution represents frequency of sth.But then how come normal distribution y-axis becomes
If distribution y-axis doesnt represent frequency, the what is central limit theorem.The central limit theorem y-axis represents the frequency of mean samples.Shouldnt it represent the above formula to satisfy a normal distribution
The normal distribution comes up as the approximate distribution for averages and weighted averages. If you have a large sample from some distribution sampling with replacement from this large sample should only give back the original distribution. So if you did not start with a normal distribution you shouldn't be getting one back.
according to the central limit theorem - the more samples you take from a population, no matter what shape the distribution is, the more normal your sampling distribution becomes.
This is incorrect in several respects. (I expect you've been told something close to this, but it's not the case.)
"no matter what shape the distribution is" ... not so. There are distributions for which the CLT doesn't hold (other limit theorems may apply).
"the more samples you take [...] the more normal your sampling distribution becomes" ... the central limit theorem doesn't actually assert this. It does happen (under certain conditions), but it's not really the CLT that says that. An example of a result that does say something (more or less) along these lines would be the Berry-Esseen theorem, which gives a bound on how far the distribution of the standardized mean can be from the standard normal distribution, and which bound decreases as $1/\sqrt{n}$.
So why, despite the central limit theorem, is the sample distribution of r not normally distributed?
The sample correlation statistic $r$ can be construed as a kind of (scaled) mean (especially if you define it with an $n$ denominator), and the CLT should apply to it. But the CLT is a theorem about the limit as $n\to\infty$; you have finite $n$. At finite sample sizes the distribution won't be normal -- indeed this should be obvious, since $r$ is bounded. The bounds will tend to make it skew as you move toward one or the other.
Indeed, even the effect you thought was CLT -- the one where increasing the sample size tends to make the sampling distribution of means more normal -- applies to $r$ too. As you take larger samples, $r$ does tend to be more nearly normally distributed in a very wide variety of circumstances.
You can investigate this fairly easily using simulation.
However, while it becomes more nearly normal as $n$ increases for a given population $\rho$, it is still generally skew at every finite sample size (when $\rho\neq 0$). The same applies when taking sample means from skewed distributions --- the skewness decreases with larger samples, but it doesn't go away.
But we don't get skew when plotting the sampling distribution of the mean
Not so! If the distribution you draw samples from is skewed, the sample means will also be skewed (but typically substantially less so):
As the sample size gets larger, the skewness in the sample mean will tend to reduce.
If we drew samples from a suitable distribution on $[-1,1]$, say a scaled-shifted beta, then as the population mean approached those bounds for a given $n$, the sample mean would tend to be more skewed (left skew for a population mean near $1$, right skew for a population mean near $-1$). But as the sample size increased for a given mean, the distribution would be less skewed. The situation is similar for the sample correlation.
Best Answer
As you can see from the definition of the normal density, it is not dimension-less, but its measurment unit (dimension in the physical meaning) is the same as that of $1/\sigma$ which in turn is the same dimension as that of $1/x$. Integrating over $f(x)$ yields a dimensionless quantity: the probability of the region of integration.
The y-axis is thus "probabilty per measurement unit of x". This holds for every probability density, not only the normal density.