新型CCII电流传输器

上传人:我*** 文档编号:136398894 上传时间:2020-06-28 格式:DOC 页数:11 大小:132KB
返回 下载 相关 举报
新型CCII电流传输器_第1页
第1页 / 共11页
新型CCII电流传输器_第2页
第2页 / 共11页
新型CCII电流传输器_第3页
第3页 / 共11页
新型CCII电流传输器_第4页
第4页 / 共11页
新型CCII电流传输器_第5页
第5页 / 共11页
点击查看更多>>
资源描述

《新型CCII电流传输器》由会员分享,可在线阅读,更多相关《新型CCII电流传输器(11页珍藏版)》请在金锄头文库上搜索。

1、New CCII Current ConveyorBy: John Robinson Mar 27, 2008Abstract: Offering higher bandwidth than its voltage-feedback counterpart, the second-generation current conveyor operational amplifier (CCII) can be used in RF mixers, high-frequency precision rectifiers, and medical applications such as electr

2、ical impedance tomography. The conventional operational amplifiers cannot be used in the high-frequency applications due to their limited gain-bandwidth product. IntroductionThe current conveyor has been around since the original design, or CCI (which can be regarded as an ideal transistor), was ini

3、tially proposed by Smith and Sedra in 1968,. CCI was then replaced by a more versatile second-generation device in 1970, the CCII. Current conveyor designs have mainly been BJT due to their high transconductance values compared to their CMOS counterparts. They are used as current-feedback operationa

4、l amplifiers such as the MAX4223 low-power amplifier, which features current feedback rather than the conventional voltage feedback used by standard operational amplifiers. This means that the current feedback operational amplifier is not restricted by the conventional gain bandwidths of a standard

5、operational amplifier, and can offer a much higher bandwidth solution than its voltage-feedback counterpart.Current conveyors are used in high-frequency applications where the conventional operational amplifiers cannot be used, because the conventional designs are limited by their gain-bandwidth pro

6、duct. In theory, the current conveyor is only limited by the ft of the transistors used in its design. Some applications where current conveyors are used today include RF mixers, high-frequency precision rectifiers, and medical applications such as Electrical Impedance Tomography (EIT).A Bipolar Con

7、veyorThe diagram in Figure 1 below shows a current conveyor implemented using bipolar devices.Figure 1. A bipolar CCII.From Figure 1 it can be seen that the CCII conveyor can be modelled as an ideal transistor:Y being the base/gateX being the emitter/sourceZ being the collector/drainThis type of cir

8、cuit works well as a circuit with BJTs, as the transconductance and Early voltages of BJTs are much greater than that of CMOS devices. Therefore, current conveyors work well as source followers. Gain X/Y is close to 1; Z has a natural high-output impedance which cannot be mimicked by their CMOS coun

9、terparts.The CMOS Source FollowerAs previously explained, the major problem with a CMOS follower is the low gm and poor Early voltage (1/lambda). This equates to poor gain, because the gain for a voltage follower heavily relies on these two parameters to be large. This can be observed in the equatio

10、n below:Where gL is the load conductance, gds is the drain source conductance and gm is the transconductance of the CMOS device.A typical simulated gain with a TSMC 0.18m with a load of 1k gave a gain of 0.7. Compared to the ideal gain of 1, this represents a 30% loss in output gain.Current Conveyor

11、 Source FollowerOne can use an unbuffered amplifier (Figure 2a) to mimic a source follower with a gain of one. Then this modification can be added to the basic design in Figure 1 to make a CCII current conveyor.Figure 2a. A simple source follower.Figure 2a can be implemented as shown below in Figure

12、 2b.Figure 2b. The CCII unbuffered source follower and implementation.From Figure 2b it can be seen that output X is fed back to one of the long tail pairs of inputs (X). The other input to the long tail pair is Y, as input Y changes the current through M1. M2 differs as M3, and M4 is a current mirr

13、or. There is a current difference between M2 and M4. This imbalance is addressed by pulling current from, or to, the gate/source capacitance Cgs of device M5. Until the output X matches that of Y, the bandwidth limit is defined as the rate at which this transistor can be discharged and charged. Thus

14、, the bandwidth limit can be defined as:Current Conveyor (CCII+) Using an Unbuffered AmplifierFrom Figure 2, the first part of the current conveyor (CCII+) can be realized. To build the rest of the current conveyor (CCII+), the current from output X simply has to be mirrored. To give Zs output, see

15、the example in Figure 3.Figure 3. The current conveyor (CCII+) using an unbuffered amplifier.The current from M5/M6 is simply mirrored by M7/M8, giving the output Z(-) of the CCII+.The output impedance of Z can be improved by adding in a cascode to M7/M8 if necessary. One must be aware that to mimic

16、 the current successfully, the output impedance of X must match that of Z, i.e., the same transistor types and confirmation must be used on M5/M6 as on M7/M8.The gain of the CCII is simply:Converting from a CCII+ to a CCII-Taking the bias point Yb (Figure 3), simply add the extra connections as shown in Figure 4.Figure 4. The current conveyor configure

展开阅读全文
相关资源
相关搜索

当前位置:首页 > 办公文档 > 事务文书

电脑版 |金锄头文库版权所有
经营许可证:蜀ICP备13022795号 | 川公网安备 51140202000112号