How to calculate the electric field outside an infinitely long conducting cylinder with surface charge density σ I'm currently studying electromagnetism, specifically Gauss's Law, and have been presented with the following question:

Consider an infinitely long cylinder of radius R made out of a conducting
  material. The charge density of the surface of the cylinder is . Use Gauss law to
  calculate the electric field outside the cylinder.
  (Note that the element of surface in cylindrical coordinates is given by
   = ).

I am still quite stuck despite having searched the internet for a walkthrough of this problem. The answers I can find do not seem to contain the surface charge σ term which leads me to believe my answer is wrong. My current working out is as followed:
Gauss's Law is:
$$
\oint E da = \frac{Q_{enc}}{\epsilon_0} 
\label{eq1}
$$ 
Using a cylindrical Gaussian surface with radius r coaxial with the infinitely long conducting cylinder of radius R and length l, I calculated the LHS of the above equation to be:
$$
\oint E da = |E|2\pi r l \label{eq2}
$$
Then working out the RHS as I understand it gives me:
$$
\frac{Q_{enc}}{\epsilon_0} = \frac{σa}{\epsilon_0} = \frac{σ2\pi R l}{\epsilon_0}
$$
Equating the LHS to the RHS and rearranging for $E$:
$$
|E|2\pi r l = \frac{σ2\pi R l}{\epsilon_0}
$$
$$
E = \frac{R\sigma}{r\epsilon_0}
$$
Which just does not sit right with me. Where have I gone wrong? I feel like I am being a bit thick at the moment. The website Hypherphysics (http://hyperphysics.phy-astr.gsu.edu/hbase/electric/elecyl.html) states that the electric field outside the conducting infinite cylinder should be:
$$
E = \frac{\lambda}{2\pi r\epsilon_0}
$$
However it doesn't explain how they arrived at that answer, whilst also not containing $\sigma$.
Any help would be greatly appreciated! Hopefully I have made this clear enough a question.
 A: Your solution is actually correct.  The difference between your solution and the one you quote is that $\lambda/(2\pi \epsilon r)$ is the field of a wire, not that of a cylinder of finite radius $R$.  For a wire one usually gives a linear charge density $\lambda$ but for a conducting cylinder this charge is on its surface, so the charge is given through a surface charge density $\sigma$.  The total charge enclosed by your Gaussian cylinder (of radius $r$ and length $\ell$) is the charge on the surface of your conducting cylinder (of length $\ell$ and radius $R<r$):
$$
Q=\sigma \times 2\pi R\times \ell\, .
$$
Note that, for the wire version of this problem, $Q=\lambda\times \ell$ and you would recover the expression given in your link.
A: perhaps your answer is wrong ,please check correctly
the electric field outside any conductor surface (in your question charges are at surface)
is
 $\cfrac{\sigma}{\epsilon o}$
in non uniform charge distribution $\sigma$ may be different at different points
but question states uniform surface charge distribution
link describes cylinder of volume charge density not surface one like in your question
this is true for every case in electrostatics, the electric field outside surface of conductor is as above
as electric field inside conductor is $0$ , your question states a cylinder made of conducting material
in a conductor charges always accumulate at surface to make flux $0$ inside
 since $E$$=$ $0$ (inside conductor) so flux should be $0$ as well.
so the link you have mentioned doesn't mention conducting word for cylinder of surface charge density as in your question
question states surface charge density $\sigma$ not volume charge density like in link
A: I have struggled with the same issue.. And I also arrived to the result at the website Hypherphysics :)
For any region outside the charged non-conducting cylindrical shell, you will obtain the same electric field if you replace the cylindrical shell by a wire, assigning an amount charge to each point of that wire –that's the definition of Lambda!– the amount of charge contained in the ring of the shell that surrounds that point of the wire. And how much charge is present in that ring with radio R and charge density sigma? 2·pi·R·sigma.. :)
Hope it helps!
