So in order to figure this out graphically I first needed to figure out the reactions. This can be done either by taking the sum of the forces about A then Figuring out the Forces at E. Alternatively, since this is symmetrical a quick short cut is simply sum the vertical applied loads (30 kN), and dividing by the number of reactions (2) to get the reaction A both A and E since they will be equal due to the symmetry. Rya = Rye = 15 kN.
The next thing to consider with a truss is that there are only axial forces. So this means the geometry of the truss will control the direction of the force vector in each member. In this example you will note that the same coloured members are will carry the same vector magnitude because of the symmetrical loading and geometry.

The next step is to draw you vectors to a an arbitrary scale. Whatever the scale you pick you will need to multiply the results by it to get your final force. In my example I used 1 kN as the same 1 m I used in the drawing the truss. Because I was in cad and had unlimited space this was not an issue for me. If you were doing it on paper you may need to use a smaller scale or get larger paper.

The next I did was start at the reaction A. I did this as it had the fewest members at the joint. Since the sum of the forces at a node have to sum to zero we can use the sum of vectors to solve the unknown magnitude of the vector GA and BA. I started by drawing the reaction vector RyA to scale. You can then proceed clockwise or counterclockwise around the node and draw in the direction of unknown vectors.

Note that each unknown vector is placed at either end of the known vector. Since we know that the vectors have to sum to zero, we know that they unknown vectors will need to intersect. Based on the direction of the RyA vector, the direction of the unknown vectors is determined.

This process is repeated at node B. It is important to note that the direction of the vector at one member member end will be opposite at the other. For node B, The 2 of the 4 vectors are known. Draw in the FyB vector to scale and draw the same vector FAB that were determined at the previous at the same scale. You will know FCB will be attached to Fyb, and you know that FGB will be attached to FAB. Extend FCB and FGB until they intersect. When you have done this successfully you will wind up with something that looks like the following:

Repeat this for node C and G.

Note that in the next image vectors GF and GA are both horizontal and on top of one another.

To get the magnitudes, measure the length of your vectors and multiply them by the scale you chose to use. Since this is a symmetrical system you can apply the magnitude to the corresponding members.
In my case I got the following results:
- AB=ED=27.0416 kN
- AG=EF=22.5 kN
- BC=DC=21.4946 kN
- GB=FD=8.3205 kN
- GC=FC=7.5 kN
- GH=15 kN
Vectors that point towards the node are in compression and the vectors that point away from the nodes are tension.
Alternatively normally loaded trusses like this have the top chord in compression and the bottom chord in tension. You can derive a convention from this to determine the interior member forces.
These values were also mathematically verified with a simple 2D online truss solver.