IBIS模型可以共享有关振荡器行为的信息，但却很少透露有关振荡器行为的信息集成电路的设计。与集成电路组件和设计被识别的风险相比，降低了其他仿真模型，因为IBIS模型不保存IC的任何结构信息。

用户可以检查振荡器产品的结构模型的内部方面。宜必思模型,然而，是行为模型，这意味着它们记录了电流、电压和电流之间的关系稍后在模拟电路中重复的时间。这允许振荡器的性能整合到一个更大的系统的设计中，而不透露任何关于组成的细节振荡器本身。表1是IBIS摘录，显示了Abracon晶振的ASDDV的上升输出波形系列CMOS振荡器。

ECS晶振ECS-2520MVQ多伏振荡器系列符合AEC-Q200标准的MultiVolt? SMD石英晶体振荡器允许客户在多种设计中使用相同的器件。MVQ系列符合AEC-Q200标准的低功耗、固定频率、低抖动、MulitVolt? SMD晶体振荡器采用2.5x2.0mm封装。MultiVolt? 功能允许客户将同一设备用于具有不同电源电压的多种设计，从而降低了资格要求和库存。ECS-2520MVQ贴片晶振是一款微型SMD HCMOS振荡器，具有MultiVolt能力为1.6V至3.6V的2.5×2.0×0.8毫米陶瓷封装四脚贴片晶振，非常适合LoRa WAN、lora模块，低功耗/便携式、工业和汽车应用。

lora模块低功耗晶振供应ECS-2520MVQ-250-BN-TR

ECS晶振ECX2-LMV系列，编码ECX2-LMV-7CN-125.000-TR，是一款LVDS输出差分晶体振荡器，小体积晶振尺寸7.0x5.0mm六脚贴片晶振，有源晶振，工作电压范围为2.375V至3.63V，频率范围100.000MHz至320.000MHz，频率温定性±25PPM，工作温度-40℃至+85℃，ECX2-LMV系列有源晶振具有小体积，轻薄型，低电源电压，低抖动，低功耗，低损耗，低耗能，满足产品低消耗电流的特点。应用：SONET/SDH，光纤通道，千兆以太网，存储区域网络，宽带接入，FPGA/DSP，测试和测量等

LVDS差分晶振ECX2-LMV-7CN-125.000-TR用于存储区域网络应用

Abracon晶振ASPIAIG-S6055和ASPIAIG-S8050是一系列屏蔽SMD功率电感，设计用于要求在-40℃至125℃环境温度下工作的汽车、工业和其它高可靠性应用。这些电感具有紧凑的外形，ASPAIG-S6055的尺寸为6.0x6.0x5.5毫米，ASPAIG-S8050的尺寸为8.0x8.0x5.0mm毫米SMD晶振。这些电感旨在满足下一代DC/DC转换器和开关模式电源(SMPS)的要求，提供出色的尺寸与功率密度平衡，电感范围为1μH至470μH。该系列提供高达16A的饱和电流，25?时保证24mωDCR。屏蔽结构降低了EMI。该系列通过TS-16949和AEC-Q200认证，支持PPAP级。

Abracon晶振紧凑型屏蔽SMD电源汽车用电感器ASPIAIG-S6055

绿色无铅的SMD无源晶振ABM10AIG-16.000MHZ-4Z-T3用于航空电子，Core losses – are losses from the inductors core material. Core losses are caused by Hysteresis loss and Eddy current loss, both of which are converted to heat. 
Hysteresis losses are caused by the friction of the molecular domains inside core material.
These molecular domains become magnetized and polarized to the direction of the
current flowing through the conductor. As the current alternates at a frequency, the
magnetic domains must alternate polarity accordingly causing molecular friction and
dispersed in the form of heat.
Eddy currents are circulating currents that manifest in the core due the changing magnetic
field within the conductive core material. Eddy currents are a function of the frequency of
the magnetization, volume of the magnetic core, peak flux density and other various
parameters of the inductor.
Another way to categorize the losses previously described are as AC and DC sensitive components.
The DCR is purely a DC component and easiest loss to calculate. AC losses include the AC copper loss,hysteresis loss and eddy current loss. The total power loss (Watts) of the inductor is calculated using the following equation:
The AMXLA family consists of two series that are of different dimensions and different performance. As with any inductor, the AMXLA family is influenced by all the previous mentioned effects. However, the AMXLA extended temperature inductor family allows designers to operate these inductors at elevated temperature making it necessary to clearly understand how heat affects the inductor performance. 

This section includes performance graphs of the AMXLA-Q1040 series. In order to minimize the size of this app note, graphs will not include all inductors in the series. The 1.0µH inductor is used as an example where the whole series cannot be illustrated.

磁芯损耗-是电感器磁芯材料的损耗。磁芯损耗是由磁滞损耗和涡流损耗引起的，两者都转化为热量。
磁滞损耗是由芯材内部分子域的摩擦引起的。
这些分子结构域被磁化并极化到流过导体的电流。当电流以某一频率交替时，则磁畴必须相应地交替极性，从而引起分子摩擦和以热的形式分散，而这些电流之中必然也少不了石英晶体的支持。