Electronic – Differential pair biasing by current sources

amplifiercurrent-sourcedifferential

I'm having a problem understanding of how can a current be injected into emitter and pulled into collector via base, using only current sources at emitters and collectors of differential pair and not applying and base voltage directly (like shown in the schematic below).

schematic

simulate this circuit – Schematic created using CircuitLab

\$ I_e \$ could be a BJT constant current source and \$ I_{c1} \$ could form a current mirror with \$ I_{c2} \$. Which doesn't really matter here. What does matter is, how can \$ V_{be} \$ on both \$ Q_1 \$ and \$ Q_2 \$ be "formed" and both transistor to conduct current, if there is no directly applied voltage on either of differential pair inputs?

Here is a quote regarding biasing of differential amplifier from Wikipedia:

In contrast with classic amplifying stages that are biased from the side of the base (and so they are highly β-dependent), the differential pair is directly biased from the side of the emitters by sinking/injecting the total quiescent current. The series negative feedback (the emitter degeneration) makes the transistors act as voltage stabilizers; it forces them to adjust their VBE voltages (base currents) to pass the quiescent current through their collector-emitter junctions. So, due to the negative feedback, the quiescent current depends only slightly on the transistor's β.

So, emitter current is forced into each of transistors by \$ I_e \$ somehow, and both of them also pass it through the base into collector. But how that happens? Isn't it true that BJT acts as very high impedance load, if there is no applied \$ V_{be} \$ (basically open circuit between collector and emitter)? Also, both bases are floating, so \$ V_{be} \$ could be anything since we don't know base potential.

I hope someone could explain this matter from mathematical aspect using nodal analysis. If not that way, than any other way possible.

P.S.* I tried this circuit in LTSpice and the both transistors conduct current from their emitters/collectors, but \$ V_{be} \$ look like some random spikes, which doesn't tell me anything useful.

Best Answer

There ar two points to be considered:

  • At first, in reality there are no real current sources. However, we are using such a symbol to indicate that there is a voltage source with a comparatively very large source resistance (either a large ohmic resistor or - very often - a transistor based cicuit with a very large dynamic output resistance).

  • Secondly, the base nodes must not be open. The whole circuit can be designed using split supply with an additional negative supply voltage. In this case, the base nodes need a DC connection to ground. Or - as in your case - we need a suitable dc voltage at the base (0.7V about the common emitter potential) - created with a suitable voltage divider.

EDIT (Addendum): To Keno. Perhaps the following helps to UNDESTAND the circuit.

  • We want to build a differential amplifier.

  • No problem: The BJT can amplify the voltage difference between both input nodes: Base and Emitter: Ic=f(Vbe)

  • Problem: Both input resistances are very different (input resistance at the emitter very low).

  • Solution: We are using an additional high-impedance common collector stage (transistor T1, emitter follower) in front of the original stage with the emitter input. Now THIS stage (transistor T2, emitter input) works as a common base stage.

  • Result: Two stages in series: Common collector (T1) and common base (T2) with one single common emitter resistor.

  • Final consideration: The whole circuit is symmetrical (when we include a collector resistor into the collector path of T1 - without changing its property working as a emitter follower). Hence, we can see and describe the operation of the whole circuit from the left or from the right. In both cases, series connection of two stages (emitter follower and common base).

  • Now we can operate this two-transistor circuit from either side - or at the same time from both sides (superposition principle) -