Find the Thevenin equivalent.

NOTE: Blue items were added to
solve the problem and are not part of the original diagram.
Express dependent source parameters in terms of mesh currents.
ib = i2
v2 = 50 K i3
Express current sources in terms of mesh currents.
Independent source:
i1 = 500 mA (Equation 1)
Dependent source:
i3 = - 80 ib
i3 = - 80 i2 (Equation 2)
Now, erasing the current sources leaves only one mesh (2) around which to write KVL.
1310 i2 + 4 X 10-5 v2 + 100 (i2 - i1) = 0
1310 i2 + 4 X 10-5 (50 K i3) + 100 (i2 - 500 mA) = 0
1410 i2 + 2 i3 = 50 mA (Equation 2)
Solving Equations 2 and 3 yields
i2 = 40 mA
i3 = - 3.2 mA
Finally
voc =v2 = 50 K i3 = 50 K (- 3.2 mA) = - 160 V
so
vTh = - 160 V
Now, find isc.
We could do a full-blown mesh analysis as indicated by the mesh currents in the circuit below, but a little bit of reflection will lead to a quicker solution.
(If you are uncomfortable with the short-cuts at this point, don't worry - you can always fall back on the algorithmic techniques: Nodal Analysis and Mesh Analysis.)
First, note that the 50 KW resistor
is shorted out, thus there is no current through it nor voltage
across it (thus v2 = 0).
We can thus remove the 50 KW
resistor from the circuit without altering the function.
(Another way of seeing this is that we effectively
have 50 KW in parallel with a wire
(0 W). This gives an equivalent resistance
of 0 W, thus we can replace the 50
KW and the wire with just a wire.)
Since v2 = 0, the dependent voltage source has a value of zero also. We can thus replace the dependent voltage source with a wire without affecting the circuit.
Making the modifications to the circuit yields

We can easily get ib using current division:
ib = 500 m (100 / 1410) = 35.461 mA
Next,
isc = - 80 ib = - 80 (35.461 m) = - 2.837 mA
Finally we can calculate RTh
RTh = voc / isc = - 160 / - 2.837 m
RTh = 56.4 KW
so the Thevenin equivalent circuit is:
