BlueText, please attach images to the posts. Do not drop them at random external servers. The forum has an attachment feature.
The circuit is symmetric with respect to the capacitor. Not only components, but also conditions present. Which means current through that capacitor must be zero. If it wasn’t, one of the sides would need to observe different conditions. That contradicts the initial assumptions. It would also raise a question of which side it would be, which by itself is not a problem, until one asks why in a perfectly symmetric situation one option would be preferred over the other.
If current through the capacitor is zero, it may be treated as open. The circuit becomes what is seen in the attachment. Let’s assume that current I
1 is present. That implies that there must be current at transistors’ bases (I
B). There are two paths available. The more obvious is loop through base-emitter junctions of both transistors. But there is nothing to drive that current. The other is two loops: one through L1, D1, base-emitter junction of Q1 and then emitter-collector of Q2, and a symmetric one for L2. However, that would induce impossible voltages. Assuming
(1) voltage across an inductor is
xv and each P-N junction drops
v: D1 cathode is
(x-1)·v, Q1 base is
(x-2)·v, the rest is dissipated on Q2. But since the situation is perfectly symmetric, equivalent reasoning for current through L2 indicates that D2 cathode must be
(x-1)·v. And that cathode is the same node as Q1 base, which leads to a contradiction. Of course voltages are relative and L2 is independent of L1, so we may neatly assume that voltage at D2 cathode is
(x-2)·v, but then base of Q2 is at
(x-3)·v, which is not the same as D1 cathode, leading to the same contradiction.
Another take is not involving currents at all. From
KVL the sum of voltages on the inner loop, formed from base-emitter junctions of Q1 and Q2, must be 0. However, if there is current through those junctions, both see some positive voltage. And a sum of two positive numbers is always positive, which contradicts KVL.
(1) The argument itself doesn’t depend on P-N junction drops being equal. I used
v for them merely for simplicity. You may conduct the same reasoning with any set of non-zero values.