The logistic distribution approximates the normal distribution function used in the Black-Scholes. The drawbacks to the normal cumulative distribution function are that it cannot be computed exactly through elementary functions, it cannot be inverted algebraically (i.e., the inverse bijection cannot be solved algebraically), and it is computationally expensive. An alternative is the logistic distribution which can be computed with elementary functions, can be algebraically inverted, and is computationally inexpsenive. Also, as a result of the inversion property, optimal boundary values of American options can be easily estimated for the logistic distribution.
The general solution to Black-Scholes is given by:
$$V_t = \Phi[d_1]S_t - \Phi[d_2]K e^{-r (T-t)} $$
where $\Phi[X]$ is the CDF of the normal distribution.
It can be shown that a fast (i.e., computationally cheap) numerical approximation is as follows:
$$V_t \approx \left(\frac{1}{2} + \frac{1}{2} \operatorname{Tanh} \left( \frac{\pi \, d_1}{2 \sqrt{3}} \right) \right) S_t - \left(\frac{1}{2} + \frac{1}{2} \operatorname{Tanh} \left( \frac{\pi \, d_2}{2 \sqrt{3}} \right) \right) K e^{-r(T-t)} = \left(1- \frac{1}{1+e^{\pi d_1 / \sqrt{3}}} \right)S_t - \left(1- \frac{1}{1+e^{\pi (d_1-\sigma \sqrt{T-t}) / \sqrt{3}}} \right) K e^{-r(T-t)}$$
The Logic
A logistic distribution $F$ -- which can be expressed as a rescaled hyperbolic tangent -- can closely approximate the normal distribution function $\Phi$. Likewise, its inverse function -- the "logit" function $F^{-1}$ -- can be rescaled to approximate the inverse normal CDF -- the "probit" function $\Phi^{-1}$.
In comparison, the logistic distribution has fatter tails (which may be desirable). Whereas the normal distribution's CDF and inverse CDF ("probit") cannot be expressed using elementary functions, closed form expressions for the logistic distribution's CDF and its inverse are facilely derived and behave like elementary algebraic functions.
The logistic distribution arises from the differential equation $\frac{d}{dx}f(x) = f(x)(1-f(x))$. Intuitively, this function is typically used to model a growth process in which the rate behaves like a bell curve. In physics, it arises as the "limit distribution of a finite-velocity damped random motion described by a telegraph process in which the random times between consecutive velocity changes have independent exponential distributions with linearly increasing parameters."
In comparison, the normal distribution arises from the following differential equation: $ \frac{d \,f(x)}{dx}=f(x)\frac{(\mu-x)}{\sigma^2}$). The normal distribution is commonly used to model diffusion processes. E.g., a Wiener processes is a stochastic process which has independent normally distributed increments with mean $\mu$ and variance $\sigma^2$. In the limit, this is a Brownian Motion.
Interestingly, the logistic distribution arises in a physical process which is analogous to Brownian motion.
Note that the CDF of the logistic distribution $F$ can be expressed using hyperbolic tangent function:
$F(x;\mu ,s)={\frac {1}{1+e^{{-{\frac {x-\mu }{s}}}}}}={\frac 12}+{\frac 12}\;\operatorname {Tanh}\!\left({\frac {x-\mu }{2s}}\right)$
Given that distribution's variance is ${\tfrac {s^{2}\pi ^{2}}{3}}$, the logistic distribution can be scaled to approximate the normal distribution by multiplying its variance $\frac{3}{\pi ^2}$. The resultant approximation will have the same first and second moments as the normal distribution, but will be fatter tailed (i.e., "platykurtotic").
Also, $\Phi$ is related to the error function (and its complement) by:
$\Phi (x)={\frac {1}{2}}+{\frac {1}{2}}\operatorname {erf} \left(x/{\sqrt {2}}\right)={\frac {1}{2}}\operatorname {erfc} \left(-x/{\sqrt {2}}\right)$
Thus, for a standard normal distribution with $\mu =0$ and $\sigma =1$: $$\operatorname{erf}(\frac{x}{\sqrt{2}}) \approx \operatorname{Tanh}\left(\frac{x \, \pi}{2 \sqrt{3}} \right) \equiv \frac{e^{\frac{\pi\,x}{\sqrt{3}}}-1}{e^{\frac{\pi\,x}{\sqrt{3}}}+1} $$
$$\operatorname{erf}(x) \approx \operatorname{Tanh}\left(\frac{x \, \pi}{ \sqrt{6}} \right) \equiv \frac{e^{\pi\,x\frac{2}{\sqrt{3}}}-1}{e^{\pi\,x\frac{2}{\sqrt{3}}}+1} $$
$$\Phi \left( x \right) \approx \frac{1}{2} + \frac{1}{2} \operatorname{Tanh} \left( \frac{\pi \, x}{2 \sqrt{3}} \right) \equiv 1-\frac{1}{1+e^{\pi x \over\sqrt{3}}} $$
And easily, thus:
$$x \mapsto \Phi^{-1}\left(p\right) \approx -\frac{2\sqrt{3}\operatorname{ArcTanh}\left( 1-2p \right)}{\pi}$$
Again, the chief advantage to approximating normal with the logistic distribution is that the CDF and Inverse CDF can be easily expressed using elementary functions. I have found this property to be very useful in estimating values of American options or in the general case where the terminal/optimal boundary conditions are not known.
However, it should be noted that the distributions behave differently in "the tails" which could lead to asymptotic residuals if normal is expected.