Question A
So, we have $n$ random measurements and we are interested in the distribution (and the mean) of the smallest element. Usually the lament is denoted by $X_{(1)}$.
In order to get the pdf of $X_{(1)}$ at an $a$, we have to calculate
$$f_{(1)}(a)=\lim_{\Delta a\to 0}\frac1{\Delta a} P(X_{(1)}\in[a,a+\Delta a)).$$
S0, let's proceed the following way
$$P(X_{(1)}\in[a,a+\Delta a))=P(\Phi( a)\le \Phi(X_{(1)})<\Phi(a+\Delta a))=$$
$$=P(\Phi( a)\le U_{1}<\Phi(a+\Delta a))$$
where $\Phi$ is the gaussian cdf with parameters $m$ and $s$ and $U_{(1)}$ is the smallest element of a sample of $100$ independent and uniformly distributed random variables (uniform over, of course $[0,1]$).
It is known that for the smallest element of a sample of size $100$ of i.i.d uniform random variables the probability to fall in an interval is
$$P(\Phi( a)\le U_{1}<\Phi(a+\Delta a))=n(1-\Phi(a))^{n-1}(\Phi(a+\Delta a)-\Phi(a)).$$
As a result, the pdf of the smallest element is
$$f_{(1)}(a)=\lim_{\Delta a\to 0}\frac1{\Delta a}n(1-\Phi(a))^{n-1}(\Phi(a+\Delta a)-\Phi(a))=n(1-\Phi(a))^{n-1}\phi(a).$$
Where $\phi$ is the cdf belonging to $\Phi$.
In the case of the standard normal distribution ($m=0$ and $s=1$) the cdf looks like this

The mean of this distribution is
$$n\int_{-\infty}^{\infty}a(1-\Phi(a))^{n-1}\phi(a)\ da.$$
This integral can be evaluated only by numerical methods. For $n=100$ $m=0$ and $s=1$ (which data don't really belong to height measurements) the mean is $\approx -2.5$.
As far as the largest number, the solution is symmetrical...
Question B
Let's assume that we omit the smallest number and $1$ more randomly selected samples from our set of height measurements. The probability that we omit the second smallest data is $\frac{1}{n-1}$ and the probability that don't remove that element is then $\frac{n-2}{n-1}$.
So, the pdf of the random variable we seek for is
$$f^1=\frac{n-2}{n-1}f_{(2)}+\frac1{n-1}f_{(3)}$$
where $f_{(2)}$ and $f_{(3)}$ are the densities belonging to the order statistic of the original sample of $n$ element. For both of these densities we can use the argumentation above except that we have to use the formulas given here.
If we omit $k$ further samples the the first step is to calculate the probabilities that we omit the remaining smallest element will be $X_{(2)}$ or $X_{(3)}$ or $X_{(4)}$ and so on.
Having these probabilities we can use the argumentation given in the answer answer in part A. Again, the necessary formulas can be found here.
Question C
Suppose that we have $n=\ell (k+1)+1$ numbered balls sitting on the table in the order of their numbers. Now, remove the first ball and $k$ other balls randomly. The balls are still in order but $k+1$ of them are missing. Remove the ball of the smallest number again an $k$ other balls, and so on. Do this until only one ball remains. Since we had to repeat the operation $\ell$ times the first $\ell$ balls will disappear for sure. Now, we have to calculate the probabilities that the number on the remaining ball is $\ell+1$ or $\ell+2$, ... If you know these probabilities then you will know the probabilities that $X_{(\ell+1)}$ or $X_{(\ell+2)}$ or ... will be the order statistic whose pdf will have to be calculated.
The calculation, again is based on answer A and the formulas given here.