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Current-voltage characteristics capacitor

Figure 2.2 (a) Capacitance voltage characteristics of an n-type SiC-based capacitor at 400°C with a gate of sputtered Pt. (b) Current voltage characteristics of a Schottky diode at 400°C with a porous Pt gate electrode. [Pg.32]

If the capacitor module (the capacitor and heater) is thermally isolated from the rest of the active device, the sensitivity can be increased. If the module is built on a cantilever, the thermal isolation can be enhanced. The thermal isolation of the heater element from the rest of the active device can be tested by measuring the MOS transistor current-voltage characteristics and the threshold voltage, with and without power to the heater element. The smaller the difference, the better the thermal isolation. [Pg.3260]

Analytical approximations are helpful in order to estimate achievable device properties and to analyze measured current-voltage characteristics. Although MIS (metal insulator semiconductor) capacitors are also of interest, here only the basic analytical dependencies for OFETs, more specifically for TFTs, are compiled. [Pg.157]

The first thought experiment corresponds to dielectric measurements. It involves applying a voltage to a capacitor containing a dielectric medium at t = 0, and then holding the voltage constant at t > 0. The dependent variable is the time-dependent current which decays as dielectric relaxation of the medium occurs. From the current, the characteristic relaxation time of the time-dependent displacement ( >(r))) field can be calculated. The time is td. This is essentially a time domain analog of e(cu) dielectric measurements. [Pg.13]

Measurements of current-voltage (I/U) characteristics have been made with an account of the concept of tunable electronic material with pores in oxide of semiconductors (TEMPOS) [3-6]. TEMPOS structures, depending on the preparation details, may resemble the features of resistors, capacitors, diodes, transistors, photocells or sensors. It is worth noting that similar I/U characteristics under the influence of humidity were observed earlier [4] on the TEMPOS samples consisting of a SiOi layers with ion tracks covered with continuous fullerite layers on Si substrates. This structure has got the name of MOSBIT (moistutre sensor with buckminsterflillerene in the tracks). [Pg.629]

Fig. 11.1. Two basic types of current ampliflers. (a) Feedback picoammeter. It consists of two components, an operational amplifier (op-amp) A, and a feedback resistor 1 fb- a typical value of the feedback resistor used in STM is 10 fl. The stray capacitance Cfb is an inevitable parasitic element in the circuit. In a careful design, Cfb 0.5 pF. The input capacitance Cm is also an inevitable parasitic element in the circuit. Those parasitic capacitors, the thermal noise of the feedback resistor, and the characteristics of the op-amp are the limiting factors to the performance of the picoammeter. (b) An electrometer used as a current amplifier (the shunt current amplifier). The voltage at the input resistance is amplified by the circuit, which consists of an op-amp and a pair of resistors R, and R2. The parasitic input capacitance Cm limits the frequency response, and the Johnson noise on Rm is the major source of noise. Also, the input resistance for this arrangement is large. Fig. 11.1. Two basic types of current ampliflers. (a) Feedback picoammeter. It consists of two components, an operational amplifier (op-amp) A, and a feedback resistor 1 fb- a typical value of the feedback resistor used in STM is 10 fl. The stray capacitance Cfb is an inevitable parasitic element in the circuit. In a careful design, Cfb 0.5 pF. The input capacitance Cm is also an inevitable parasitic element in the circuit. Those parasitic capacitors, the thermal noise of the feedback resistor, and the characteristics of the op-amp are the limiting factors to the performance of the picoammeter. (b) An electrometer used as a current amplifier (the shunt current amplifier). The voltage at the input resistance is amplified by the circuit, which consists of an op-amp and a pair of resistors R, and R2. The parasitic input capacitance Cm limits the frequency response, and the Johnson noise on Rm is the major source of noise. Also, the input resistance for this arrangement is large.
Transient — Subcycle disturbance in the AC waveform evidenced by a sharp, brief discontinuity of the waveform. This may be of either polarity and may be additive or subtractive from the nominal waveform. Transients occur when there is a sudden change in the voltage or the current in a power system. Transients are short-duration events, the characteristics of which are predominantly determined by the resistance, inductance, and capacitance of the power system network at the point of interest. The primary characteristics that define a transient are the peak amplitude, the rise time, the fall time, and the frequency of oscillation. Figure 1.12 shows a transient voltage waveform at the output of a power transformer as the result of switching-in of a motor containing power factor correction capacitors. [Pg.19]

Earlier, it was stated that the current supply was limited, at any given voltage, by the internal impedance of the fire set. Typical capacitor discharge fire sets have the following impedance characteristics ... [Pg.361]

Other configurations of fuel cell vehicles can be realized combining the advantages of different types of storage systems. As an example, the Fig. 5.24 shows the combination of rechargeable batteries with a super capacitor system. In this case, a three-way converter is required to connect the two storage systems with the fuel cell stack and interface the different voltage versus current characteristics of the devices interconnected [46]. [Pg.164]

The vibrating capacitor method is a zero-determining method, where measuring the contact potential difference Vdpc amoimts to measuring the opposite voltage U that leads to a zero current. Compared to other methods, this one has some interesting characteristics which we will develop throughout this study. [Pg.178]

The time constant x of Eq. 9.15 is not found with constant amplitude current excitation as shown in Figure 9.2 the capacitor will be charged ad infinitum during the current step. The characteristic time constant of the parallel circuit alone can only be found with a constant amplitude voltage (Ri = 0) excitation. [Pg.338]

Experimental study of the acoustic emission and partial discharge current pulses have been carried out on the insulating foils for applied constant and ramp voltage. An insnlating foil with metal electrodes on the sides creates a parallel plate capacitor. This metal-insulator-metal (MIM) system has electrical characteristics represented by a constant value of conductivity and permittivity in the low electric field. [Pg.1830]


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See also in sourсe #XX -- [ Pg.193 , Pg.194 ]




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