How to determine whether a wave is travelling or standing? How to determine whether a wave is travelling or standing?
I have been told that wave function of the form $f(k_1x \pm k_2t)$ is a travelling wave.
But then even a standing wave equation $2A \cos \omega t \sin kx$ can be written as superposition of two waves
$$A\sin\frac{kx-\omega t}{2} + A\sin\frac{kx+\omega t}{2}$$
This is of the form $f(k_1x \pm k_2t)$ but still not a travelling wave.
In particular is $y=\cos x \sin t \ + \cos 2x \sin 2t$ a travelling wave?
 A: The "rule" you have given is a little simplistic. To use it you have to be able to write the wave solely as a function of $(kx-\omega t)$ or of $(kx + \omega t)$. That is because the thing in the brackets, the phase of the wave, has to be kept constant to apply a meaning to a direction of travel.
e.g. take $f(kx-\omega t)$. If $t$ increases, then you can only keep the phase constant by increasing $x$. So this wave travel towards positive $x$ as $t$ increases. Try experimenting with this simulation.
A standing wave cannot be written solely as $f(kx-\omega t)$ or $f(kx+\omega t)$, so is not a wave travelling in a single direction. It is the superposition of two waves of equal frequency and amplitude travelling in opposite directions.
In general, waves can always be written as the superposition of multiple waves travelling in different directions.
Your final example can be decomposed into 4 travelling waves of the same speed, but different wavelengths, 2 travelling towards positive $x$ and two towards negative $x$.
$$ y = \frac{1}{2}(\sin [x-t] + \sin[x+t] +\sin[2x-2t] + \sin[2x+2t])$$
A: What you have done is decomposed a standing wave into two travelling waves of equal amplitude, speed and frequency which are travelling in opposite directions.
Your equation $y=\cos x \sin x \ + \cos 2x \sin 2x$ has no time dependence and so can only represent a wave profile at some instant of time.
It is like a photograph of a wave.  
What you need to look for are two terms multiplied together.
One term which depends on the position from the source eg $\sin kx$, and the other term which depends on time eg cos $\omega t$ where $\frac \omega k = c$ the speed of the wave.
This will result in the wave profile not moving along.
So when you photograph the wave the maximum displacement will always be at the same position as will the minimum displacement.
An example is $y(x,t) = A \sin(kx) \cos (\omega t) $
Here are your two travelling waves superposing to form a standing wave.

A: A wave is a function like $f(x,t)=A(x+vt) + B(x-vt)$. Standing waves are waves in suitable superposition. You can see if a wave is a stadading wave or not by locating points of the wave that is fixed all the time. Sometimes this points are at boundary, in Newman boundary conditions you have such a point but they are not in the boundary. Your example is a wave if you make $x\rightarrow x\pm vt$. You could think that $y$ is a wave produced by a sum of $A$ and $B$, but this is not the case. There is no $A$ and $B$ that builds this function $y$. There is a trick to see that, you verify if this function obey the wave equation:
$$
\frac{\partial^2 y}{\partial t^2}=v^2\frac{\partial^2 y}{\partial x^2}
$$
If the function don't obey the wave equation, this means that is not a wave.
Because $y$ has not $t$-dependence this means that $\partial^2_x y=0$, and this is not the case. Actually, the only standing wave that don't dependt on time is $y=a+bx$. Usually stading waves depends on time. A example:
$$
y(x,t)=\frac{\cos(k(x+vt))+\cos(k(x-vt))}{2}=\cos(kx)\cos(\omega t)
$$
Every time that you can separate the $x$ and $t$ such that at final you have $f(x)g(t)$, you have a standing wave. Note that $f(x)g(t)+h(x)s(t)$ is not a stading wave in general.
A: I like to describe a travelling wave as a scalar field, a periodic function of space and time, so that it is possible to define a moving frame in which the field is static.
For example: $f(x,t) = A\sin(k(x - vt))$
The argument of the function is constant for a frame moving to the left with a velocity $v$, because for it:$\; x' = x - vt$.
I think that it corresponds to our intuition of a travelling wave. It is possible to add several waves like that, resulting in complex fields.
Stationary waves are one of that possibilities, resulting from identical static fields (except for a phase) for frames moving to the left and to the right with the same velocity as:
$g(x,t) = A\sin(k(x - vt)) + A\cos(k(x + vt))$
The concept is limited to non relativistic cases, due to the transformation: $x' = x - vt$
