To add onto Clement's answer: If you think of the events as being the possible decay of a radioactive atom, with one trial per second, then your statements 2 and 3 reflect the difference between the mean life of the element (which would be about $100$ seconds), and the half-life of the element (which would be about $69$ seconds).
The inter-event time follows a geometric distribution, with the time $\tau$ between events having the probability distribution
$$
P(\tau = n) = p(1-p)^n
$$
with $p = 1/100$. (You might write $n-1$ in the exponent, depending on what you mean by "between.") The continuous analogue of this is the exponential distribution, where the probability density function (PDF) of the inter-event time is given by
$$
f_\tau(t) = \lambda e^{-\lambda t}
$$
with $\lambda = 1/100$. Here, $\lambda$ gives (as $p$ did, above) the event "rate," which you may notice is the derivative $f'_\tau(0)$. It turns out that for this distribution, the mean lifetime of an atom is given by $1/\lambda = 100$.
However, the half-life of the element is given by the cumulative distribution function (CDF), which is the definite integral, from $0$ to $t$, of the PDF. That is,
$$
F_\tau(t) = \int_{x=0}^t f_\tau(x) \, dx = 1-e^{-\lambda t}
$$
The CDF gives the probability that an event happens before time $t$; equivalently, for this scenario, it gives the proportion of the sample that has decayed by time $t$. Thus, the half-life is governed by
$$
e^{-\lambda t} = \frac{1}{2}
$$
$$
\lambda t = \ln 2 \doteq 0.69315
$$
which is why you found the half-life and the mean life to be related in approximately a $69:100$ ratio.