Others have answered that when the hot and cold gases are in contact, they redistribute their energies very fast, so you won't be able to feel their temperatures separately, but only as a temperature of the mixture. But how fast? Would we feel anything, in the very short time even before the gases have redistributed their energies?
To answer that, we need to understand how fast this heating/cooling happens, compared to this redistribution of energies. Let's look at some numbers.
You need $800-1000^\circ\:C$ to cremate a human body. But you cannot go higher than $1530^\circ\:C$, since nitrogen in the air could ignite. Consider a box of volume 2 m^3 separated by an adiabatic partition. On one side of the partition, we heat the air to 1000 C, and on the other side, we cool the air to 0 C. Let the partition be removed at t=0.
First, let's get an idea of how much time it takes for the hot air to diffuse to the cold air side. Would it be slow, like smoke entering a room, or would it be instantaneous, like an explosion?
For an air parcel sitting in the hot compartment, the momentum equation is given by:
$$\rho\dfrac{du}{dt}=\dfrac{dP}{dx}$$
where $\rho $ is the density of air, $u$ is horizontal velocity, $P$ is the pressure.
Here only the pressure gradient force is written on the RHS since all other terms are negligible. For air, ideal gas law $PV=nRT$, $\rho=\:1 kg/m^3$, assuming one mole of gas and unit volume, we obtain:
\begin{align*}
\dfrac{du}{dt}&=\dfrac{1}{\rho}\dfrac{dP}{dx}\\
&=\dfrac{1}{\rho}\dfrac{P_1-P_2}{dx}\\
&=\dfrac{1}{\rho}nR\dfrac{T_1-T_2}{V\:dx}\\
&=\dfrac{1}{1\:kg\:m^{-3}}1\:(mol)\:8.314\:(J\:mol^{-1}\:K^{-1})\dfrac{1000\:K}{1\:(m^3)\:1\:(m)}\\
&=\:8314 ms^{-2}
\end{align*}
With this, the time the parcel takes to reach the other end of the 2m box starting from rest is $\bf{\sqrt{2*2\:(m)/8314\:(m/s^2)}=0.02\:seconds}$. That's more like an explosion. For reference, the blink of an eye takes 0.1 seconds.
Assuming that the order of magnitude of the mixing of energies and this spatial mixing is the same, the time scale of mixing is one-hundredth of a second.
Now, how much energy does it take for the $1000^\circ\: C$ air to warm your body by 1 degree?
\begin{align*}
Q&=mc\Delta T\\
&=70\:(kg)\:4186\:(Jkg^{-1}K^{-1}) 1\:(K)\\
&\approx 300\:kJ
\end{align*}
The equation for convective heat transfer is given by:
\begin{align*}
\dot{Q}&=hA\Delta T\\
&\approx 20\:(W/m^2K)\:2\:(m^2)\:1000\:(K)\\
&\approx 40\:kW
\end{align*}
Time it takes to heat the human by $\bf{1^\circ C=300/40\:s=7.5\:seconds}$
It takes $7.5$ seconds for the air to heat the body by just 1 degree, but just $0.02$ seconds for the air from the bottom compartment to reach the other side of the box. So forget about heating $1000^\circ\:C$, the mixing is at least 2 orders of magnitude faster.
The minimum temperature difference sensible for humans is 0.05 K. Plugging in this instead of 1 in the equation gives 0.38 seconds of exposure, but still mixing would have happened much before that.
TLDR: No, you won't get burned. You won't even feel the temperature change. You won't feel hot and cold gases separately, but only the temperature of the mixed gas.
Assumptions: Here only the thermal effects are considered. Effects like mutation happening to DNA due to molecules banging on it are neglected. The human body is at 37 degrees Celsius. m is the mass of the body, c is the specific heat capacity of the body, h is the convective heat transfer coefficient of the surrounding fluid and A is the surface area of the body. For an average human, $m=70\:kg$ and surface area is $\approx 2m^2$, $c=4186\:kJkg^{-1}K^{-1}$ since body is mostly water. $h$ for air is $5-40\:W/m^2 K$, lets assume $20\:W/m^2 K$. Since $T_{surrounding}>>\Delta T_{body}$, the heat transfer is assumed to be linear.