Lecture: Week 15a 1. Carbon nanotube inverter 2. Simple and very useful nanotech tools: Scanning Tunneling Microscope (STM) and Atomic Force Microscope (AFM) 2. How mechanical engineers use circuit analysis 3. What about radio? EE42/100 Fall 2005 Prof. White 1 1. Single carbon nanotube inverter stage (from ???) Figure 3 (a) AFM image showing the design of an intramolecular logic gate. A single nanotube bundle is positioned over the gold electrodes to produce two p-type CNTFETs in series. The device is covered by PMMA and a window is opened by e-beam lithography to expose part of the nanotube. Potassium is then evaporated through this window to produce an n-CNTFET, while the other CNTFET remains p-type. (b) Characteristics of the resulting intramolecular voltage inverter. Open red circles are raw data for five different measurements on the same device (V = ±2 V). The blue line is the average of these five measurements. The thin straight line corresponds to an output/input gain of one. EE42/100 Fall 2005 Prof. White 2 2. The Scanning Tunneling Microscope (STM) and the Atomic Force Microscope (AFM) EE42/100 Fall 2005 Prof. White 3 2a. The Scanning Tunneling Microscope The scanning tunneling microscope (STM) is a type of electron microscope that shows three-dimensional images of a sample. In the STM, the structure of a surface is studied using a stylus that scans the surface at a fixed distance from it. Currents Control the Surface An extremely fine conducting probe is held close to the sample. Electrons tunnel between the surface and the stylus, producing an electrical signal. The stylus is extremely sharp, the tip being formed by one single atom. It slowly scans across the surface at a distance of only an atom's diameter. The stylus is raised and lowered in order to keep the signal constant and maintain the distance. This enables it to follow even the smallest details of the surface it is scanning. Recording the vertical movement of the stylus makes it possible to study the structure of the surface atom by atom. A profile of the surface is created, and from that a computer-generated contour map of the surface is produced. STM inventors Rohrer and Binnig, IBM, Zurich EE42/100 Fall 2005 Prof. White 4 http://en.wkipedia.org/wiki/Image:ScanningTunnelingMicroscope_schematic.png" EE42/100 Fall 2005 Prof. White 5 Here scientists have positioned 48 iron atoms into a circular ring in order to "corral" some surface state electrons and force them into "quantum" states of the circular structure. The ripples in the ring of atoms are the density distribution of a particular set of quantum states of the corral. [Crommie, Lutz & Eigler, IBM Almaden Research Center] EE42/100 Fall 2005 Prof. White 6 STM of a molecule a molecule assembled on copper from 8 cesium and 8 iodine atoms). EE42/100 Fall 2005 Prof. White 7 2b. Example Micromechatronic System: Atomic Force Microscope http://stm2.nrl.navy.mil/how-afm/how-afm.html EE42/100 Fall 2005 Prof. White 8 EE42/100 Fall 2005 Prof. White 9 http://stm2.nrl.navy.mil/how-afm/how-afm.html EE42/100 Fall 2005 Prof. White 10 Example Application: Atomic Force Microscopy/Data Storage: The Millipede Target density: 1 terabit/sq. in. http://www.zurich.ibm.com/st/storage/millipede.html EE42/100 Fall 2005 Prof. White 11 Example Application: Atomic Force Microscopy/Data Storage Target density: 1 terabit/sq. in. thermal actuation/readout http://www.zurich.ibm.com/st/storage/millipede.html EE42/100 Fall 2005 Prof. White 12 2. How mechanical engineers can use electrical circuit analysis (Loosely excerpted from “Engineering Mechanics, vol. 2: Dynamics”, 4th Edition by Meriam and Kraige, Wiley and Sons – a text sometimes used in ME 104 at UC Berkeley) “Oscillating electrical circuits are characterized by differential equations of the same type as those obtained for oscillating mechanical systems, such as a springmass-dashpot system. Their analysis is therefore similar to that of a mechanical system. Any result obtained for the electrical circuit will also apply to the mechanical system for which it is analogous.” R Support Spring x Mass If vertical force applied to mass Is sinusoidal, as Pmsin (ωt), displacement x is solution of mx” + cx’ +kx = Pm sin (wt) Damper (dashpot) EE42/100 Fall 2005 C L V msin(ωt) Charge q is solution of Lq” + Rq’ +(1/C)q = Vmsin(ωt) Prof. White 13 Characteristics of a mechanical system and its electrical analogue Mechanical System m mass c coefficient of viscous damping k spring constant x displacement v velocity Pm applied force EE42/100 Fall 2005 Electrical System L inductance R resistance 1/C reciprocal of capacitance q charge i current Vm applied voltage Prof. White 14 3. What about radio? a. In a communication system one often shifts the information content (e.g., a waveform from a microphone) to a different (usually higher) frequency for transmission. Example: telephone carrying audible voice or music and being transmitted via RF at hundreds of MHz or even optical beams (10141015 Hz. b. Broadcast radio involves using the audio signals to modulate a steady “carrier” signal at the transmitter; the received signal is then demodulated at the receiver EE42/100 Fall 2005 Prof. White 15 0 -10 dB -20 -30 -40 30 60 125 250 500 1k 2k 4k Frequency of sound in Hz (logarithmic scale) 8k 16k Acuity of normal human hearing. Vertical axis: inverse of the sound pressure level (SPL) corresponding to minimum detectable pure tone. EE42/100 Fall 2005 Prof. White 16 Information transmission system – Purpose is to transfer information from point A to point B accurately Communication System A Source of information EE42/100 Fall 2005 Communication channel Transmitter Receiver Prof. White B Recipient of information 17 Amplitude modulated (AM) radio communication system Information source Tuner EE42/100 Fall 2005 Pickup (microphone or camera) Amplitude modulator Amplifier Antenna Carrier frequency generator Demodulator Prof. White Amplifier Output (earphone, loudspeaker, display) 18 Amplitude Modulation Radio (AM) Voltage(V) 2 0 -2 0 1 2 Tim e (ms) 3 4 Sp ectral density Frequency in Hz (expan ded scale near carrier freLower fc a rrie r Up per quen cy) Sideband Sideband Waveform (top) and spectrum (bottom) of AM radio station broadcasting a 1000 H z tone. The spacing of the sidebands from the carrier is determined by the frequency of the tone, in this case ±1000H z. EE42/100 Fall 2005 Prof. White 19 Crystal radio receiver for AM broadcasts – no batteries! + L EE42/100 Fall 2005 C1 C2 Prof. White R 20 Frequency modulated (FM) waveform Frequency modulated carrier Audio frequency waveform to be transmitted EE42/100 Fall 2005 Prof. White 21 PUZZLERS 1. Why does a nonlinear circuit generate “new” frequencies not present in the driving signal? 2. How could you use a resonant circuit to “demodulate” an FM signal? EE42/100 Fall 2005 Prof. White 22