Source Transformation of dependent sources
Since this is quite within reach I will try to go through the whole story.  

Let's take a generic network N and spot one generator (either current or voltage), for now we will not consider it as dependant.  

I will name quantities with capital letters, i.e. V, I, meaning DC values, AC phasors, Laplace's variables but also -pushing a little- time domain quantities or whatever can be useful provided it can be handled by corresponding calculation rules.

Noted  prerequisite already known from circuit analisys:


any voltage generator needs to have a series impedance to be
transformable into a current one and dually any current generator
needs a parallel impedance to be transformable into a voltage one.
"remaining" network N' does not have to linear (even if in this case computations will soon get hard).




we can assert:


the two networks N are equivalent provided
\$V_\text{k}=Z_\text{k}I_\text{k}\$
which means: all quantities in "remanining network" N' are unaffected. This
includes any voltage (like \$V_\text{rs}\$), any current (like
\$I_\text{uv}\$) throughout N' and hence voltage and current at n-m
port (\$V_\text{mn}\$ and \$I_\text{nm}\$) too.


Switching to controlled generators and stripping off fancy N' graphics we get to this two circuits



Now we can try to run through all possible control variable:

x is internal to N': no problem at all.
Any quantity inside N' up to the border's ones \$V_\text{mn}\$ and \$I_\text{nm}\$ is not affected by external generator being current or voltage. From inside we cannot tell which is connected.
So in this case controlled generator can be transformed freely. 

External control variable: we just have six possibilities -depicted in blue below-, so we can easily run through them all.



What we need to do is relate those six external quantities to internal ones, so we can recover those lost in converting from current to voltage generator.

Current generator case:
we could possibly have \$V_\text{k}\$, \$I_\text{k}\$ and \$I_\text{Zk}\$ as control variable but these can easily be found as
$$
\left\{
\begin{align}
V_\text{k} &amp;=V_\text{mn} \\
I_\text{Zk} &amp;=-\frac{V_\text{mn}}{Z_\text{k}} \\
I_\text{ik} &amp;=I_\text{nm}-I_\text{Zk}=I_\text{nm}+\frac{V_\text{mn}}{Z_\text{k}}
\end{align}
\right.
$$

So having expressed all possible control variables as function of -unchanged- internal ones we are allowed to transform from current to voltage generator.

Voltage generator case:
we just have to do the same with the three possible quantities across/thru the external parts (\$I_\text{k}\$, \$V_\text{Zk}\$ and \$V_\text{vk}\$ )

$$
\left\{
\begin{align}
I_\text{k} &amp;=I_\text{nm} \\
V_\text{Zk} &amp;=-Z_\text{k}I_\text{nm} \\
V_\text{vk} &amp;=V_\text{mn}-V_\text{Zk}=V_\text{mn}+Z_\text{k}I_\text{nm}
\end{align}
\right.
$$

so we have now proved the other way round transformation, from voltage to current generator,  is always possible too.

Conclusion
Recapping


  Voltage and current controlled sources can be transformed each other. To do so it might be necessary to do some math on control variable, but this is going to be always possible.