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CSTLS4M19G56-B0 Datasheet(PDF) 13 Page - Murata Manufacturing Co., Ltd. |
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CSTLS4M19G56-B0 Datasheet(HTML) 13 Page - Murata Manufacturing Co., Ltd. |
13 / 32 page ![]() 11 Note • Please read rating and CAUTION (for storage, operating, rating, soldering, mounting and handling) in this catalog to prevent smoking and/or burning, etc. • This catalog has only typical specifications because there is no space for detailed specifications. Therefore, please review our product specifications or consult the approval sheet for product specifications before ordering. 2 Principles of CERALOCK® 2 (Note 3) Fig.Ⅲ shows the equivalent circuit of an emitter grounding type transistor circuit. In the figure, Ri stands for input impedance, R0 stands for output impedance and ß stands for current amplification rate. When the oscillation circuit in Fig.2-6 is expressed by using the equivalent circuit in Fig.Ⅲ, it becomes like Fig.Ⅳ. Z1, Z2 and Z are as shown in the table for each Hartley type and Colpitts type circuit. The following 3 formulas are obtained based on Fig.Ⅳ. As i1 ≠ 0, i2 ≠ 0, i3 ≠ 0 are required for continuous oscillation, the following conditional formula can be performed by solving the formulas of (1), (2) and (3) on the current. βR0Z1Z2=(Z1+Ri)Z2 2–{Z1(Z2+Z)+ R0Z1Z2=(Z2+Z+Z1)Ri}(Z2+R0) ………… (4) Then, as Z1, Z2 and Z are all imaginary numbers, the following conditional formula is obtained by dividing the formula (4) into the real number part and the imaginary number part. (Imaginary number part) Z1Z2Z+(Z1+Z2+Z)RiR0=0 ………… (5) (Real number part) βR0Z1Z2+Z1(Z+Z2)R0+ Z2(Z+Z1)Ri=0 ………………… (6) Formula (5) represents the phase condition and formula (6) represents the power condition. Oscillation frequency can be obtained by applying the elements shown in the aforementioned table to Z1,Z2 and Z solving it for angular frequency ω. ………… (7) ………… (8) In either circuit, the term in brackets will be 1 as long as Ri and R0 is large enough. Therefore oscillation frequency can be obtained by the following formula. …… (9) … (10) Fig.Ⅲ R0 - + 1 R0 1 R Fig.ⅣHartley/Colpitts Type LC Oscillation Circuits Notes 1 23 1 R0 R - + R0 1 Z Z2 Z1 Hartley Type Z1 Z2 Z jωL1 jωL2 1 / jωC Colpitts Type 1 / jωCL1 1 / jωCL2 jωL (Hartley Type) 1 (L1L2) C{1+ } L1 · L2 (L1 + L2) CR R0 (Colpitts Type) · { 1+ 1 L CL1·CL2 CL1+CL2 } L (CL1+CL2) R R0 fosc. = (Hartley Type) 1 fosc. = (Colpitts Type) 1 CL1·CL2 CL1+CL2 βR0i1+(R0+Z2) i2–Z2i3=0 …………………… (1) Z1i1+Z2i2–(Z2+Z+Z1) i3=0 ……………………(2) (Z1+Ri) i1–Z1i3=0 …………………………… (3) P17E.pdf 2012.10.31 |
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