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CSTLS4M19G56-B0 Datasheet(PDF) 10 Page - Murata Manufacturing Co., Ltd. |
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CSTLS4M19G56-B0 Datasheet(HTML) 10 Page - Murata Manufacturing Co., Ltd. |
10 / 32 page 8 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. (Note 1) The relationship between the size of the resonator and the resonant frequency is described as follows. For example, the frequency doubles if the thickness doubles, when thickness vibration is used. The following relationship is obtained when the length of the resonators is ℓ, the resonance frequency is Fr, the speed of sound waves travelling through piezoelectric ceramics, and the wavelength is λ. Fr. ℓ = Const. (frequency constant, Fr.t for the thickness) λ = 2 ℓ C = Fr.λ = 2Fr. ℓ As seen in the above formula, the frequency constant determines the size of the resonator. (Note 2) In Fig. 2-3, when resistance R1 is omitted for simplification, the impedance Z (ω) between two terminals is expressed by the following formula. 2 Fig. Ⅰ 2 Principles of CERALOCK® Amplitude Range of Standing Wave (Min.Amplitude) (Max.Amplitude) Fig. Ⅱ L1 C1 C0 1 jωC0 ( jωL1+ ) Z (ω) = When ω = 1 jωC1 1 jωC0 + ( jωL1+ ) 1 jωC1 j ( ωL1 – ) = = ωr, Z (ωr) =0 1 ωC1 1 + – ω2 C0L1 C0 C1 1 L1C1 1 2π L1C1 When ω = Therefore from ω =2πF, Fr = ωr/2π = 1 2π C0C1L1/(C0+C1) Fa = ωa/2π = = Fr 1+ = ωa, Z (ωa) = ∞ 1 C0C1L1/(C0+C1) C1 C0 Notes P17E.pdf 2012.10.31 |
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