Transistors at Radio Frequency ➤ How to describe transistors at radiofrequency.
Transcription
Transistors at Radio Frequency ➤ How to describe transistors at radiofrequency.
Transistors at Radio Frequency ➤ How to describe transistors at radiofrequency. ➤ Equivalent circuits and S-parameters ➤ Y-parameters and SOLVE ➤ Stability of transistor amplifiers (brief) ➤ The Klapp RF Oscillator ➤ SOLVE Example: The Klapp Oscillator 1 ENGN4545/ENGN6545: Radiofrequency Engineering L#13 Transistors at Radio Frequency ➤ Transistors are more complex at high frequencies due to the effects of internal parasitic inductance and capacitance. ➤ Always try first to seek S-parameters from manufacturers. ➤ Or use a simulation package that has them in its database. ➤ Failing all this.. do a model. Here’s how. ➤ We try to glean enough information from datasheets and independent measurements to form a physical model to predict S-parameters. 2 ENGN4545/ENGN6545: Radiofrequency Engineering L#13 BF199 VHF Transistor 3 ENGN4545/ENGN6545: Radiofrequency Engineering L#13 Radio Frequency Transistor circuit model 4 ENGN4545/ENGN6545: Radiofrequency Engineering L#13 BF199 Datasheet 5 ENGN4545/ENGN6545: Radiofrequency Engineering L#13 Networks: Y-parameters vs S-parameters ➤ Y-parameters and S-parameters are related: (1 + S22)(1 − S11) + S12S21 yi = ∆Z0 −2S12 yr = ∆Z0 yf = −2S21 ∆Z0 (1 + S11)(1 − S22) + S12S21 yo = ∆Z0 where ∆ = (1 + S11)(1 + S22) − S21S12. 6 ENGN4545/ENGN6545: Radiofrequency Engineering L#13 Definition of Y-parameters ➤ Need these for employ solve. Ii = yiVeb + yr Vec Io = yf Veb + yoVec 7 ENGN4545/ENGN6545: Radiofrequency Engineering L#13 Using Solve For Transistors ➤ Consider the base node Ib = (yi + yr )Veb − yr Vcb ➤ Consider the collector node Ic = (yo + yf )Vec − yf Vbc ➤ Consider the emitter node Ie = (yi + yf )Vbe + (yr + yo)Vce 8 ENGN4545/ENGN6545: Radiofrequency Engineering L#13 BF199 S-parameters ➤ Use Cbe = 100pF (fT = 550M Hz), Cbc = 0.5pF , Ic = 7mA and hf e = 100. |S | 11 1 0.5 0 7 10 8 9 10 10 angle S 11 Degrees 200 100 0 −100 −200 7 10 9 8 10 frequency (Hz) ENGN4545/ENGN6545: Radiofrequency Engineering L#13 9 10 BF199 S-parameters ➤ Use Cbe = 100pF (fT = 550M Hz), Cbc = 0.5pF , Ic = 7mA and hf e = 100. |S | 21 30 20 10 0 7 10 8 9 10 10 angle S 21 Degrees 200 150 100 50 0 7 10 10 8 10 frequency (Hz) 9 10 ENGN4545/ENGN6545: Radiofrequency Engineering L#13 BF199 S-parameters ➤ Use Cbe = 100pF (fT = 550M Hz), Cbc = 0.5pF , Ic = 7mA and hf e = 100. |S | 12 0.06 0.04 0.02 0 7 10 8 9 10 10 angle S 12 Degrees 150 100 50 0 7 10 11 8 10 frequency (Hz) 9 10 ENGN4545/ENGN6545: Radiofrequency Engineering L#13 BF199 S-parameters ➤ Use Cbe = 100pF (fT = 550M Hz), Cbc = 0.5pF , Ic = 7mA and hf e = 100. |S | 22 1 0.5 0 7 10 8 9 10 10 angle S 22 Degrees 0 −5 −10 −15 −20 7 10 12 8 10 frequency (Hz) 9 10 ENGN4545/ENGN6545: Radiofrequency Engineering L#13 Example: A BF199 Common Emitter Amplifier ➤ Use the large signal equivalent (left) to set the bias point. ➤ Use the small signal equivalent (right) to set up SOLVE. 13 ENGN4545/ENGN6545: Radiofrequency Engineering L#13 Stability Criteria ➤ Is the transistor stable in isolation? Linville criterion C = |yr yf | 2gigr − real(yr yf ) ➤ Often we need to know if a transistor amplifier is stable. ➤ If a transistor with given y-parameters is loaded by source and load admittances YS = GS + jBS and YL = GL + jBL, then the transistor circuit is unconditionally stable if, 2(gi + GS )(go + GL) K = > 1 |yr yf | + real(yr yf ) ➤ The Stern Stability Criterion ➤ A number of useful related formulae.. see the web brick. 14 ENGN4545/ENGN6545: Radiofrequency Engineering L#13 Klapp RF Oscillator ➤ Model the transistor using S and Y parameters in exactly the same way as the transistor amplifier. ➤ In the project the oscillator is a VCO: the MC145170 PLL has to control the frequency of the oscillator by applying a voltage to a varactor diode or voltage variable capacitor (VVC). ➤ We need to prove that the oscillator will oscillator and at what frequency. ➤ In SOLVE we inject a current into the tank circuit of the oscillator and determine the frequency at which the ractance of the input impedance is zero and the resisitance is negative. WHY? 15 ENGN4545/ENGN6545: Radiofrequency Engineering L#13 Varactor Diode 16 ENGN4545/ENGN6545: Radiofrequency Engineering L#13 Klapp RF Oscillator 17 ENGN4545/ENGN6545: Radiofrequency Engineering L#13 Using SOLVE: Compute S-parameters and Y-parameters 18 ENGN4545/ENGN6545: Radiofrequency Engineering L#13 Using SOLVE: Set circuit values 19 ENGN4545/ENGN6545: Radiofrequency Engineering L#13 Using SOLVE: Set SOLVE admittances 20 ENGN4545/ENGN6545: Radiofrequency Engineering L#13 KLAPP oscillator input impedance BF199 local oscillator Real(Z) at node 1 1000 500 0 −500 −1000 1 2 3 4 5 6 7 8 9 10 7 x 10 2 3 4 5 6 7 8 9 10 7 x 10 Imag(Z) at node 1 1000 500 0 −500 −1000 1 21 ENGN4545/ENGN6545: Radiofrequency Engineering L#13
Similar documents
Global Radiofrequency (RF) Ablation System Market
Ablation is the process of removal of undesired organs, abnormal growths or harmful substances from the human body. Ablation is the destruction of a nerve conduction pathway by the means of high frequency alternating currents, delivered by a bipolar or unipolar catheters. Radiofrequency (RF) ablation is a non-surgical procedure which utilizes radio waves or electric currents to interfere with the nerve conduction for a period of around six to nine months. Heat is generated from medium frequency alternating current in the range of 350-500 kHz. During radiofrequency ablation, a guiding needle reaches the desired tissue with the help of image guidance device such as a CT scan.
More information