Abstract:
A controller oscillator provides a periodic output signal having first and second output level states. The oscillator is responsive to an applied saw tooth signal that varies between first and second voltages (Vlow,Vhigh). The oscillator is comprised of a comparator (82) the non-inverting input of which receives the saw tooth signal applied thereto to produce the periodic output signal at its output (86). A first voltage reference circuit (88, 90, and 92) generates the second voltage (Vhigh) that is applied to the inverting input of the comparator while the periodic output signal is at the first output level state and the input signal charges from the first voltage (Vlow) towards the second voltage. As the input signal becomes equal to the second voltage the output of the comparator switches to the second output level state and a second voltage reference (92,94, 96) provides the first voltage at the inverting input of the comparator.
Abstract:
An oscillator circuit, whose output signal has minimum fluctuation with changes in temperature, has an amplifier. Within the amplifier, a compensation resistor is connected to compensate for changes in amplitude and frequency of the output signal with temperature. A first impedance is connected between an output and a first input of the amplifier, a second impedance is connected between the first input and a second input, and a third impedance is connected between the output and the second input. A method for designing the oscillator begins by choosing an inductor with a high quality factor and a low temperature coefficient. The interconnections are designed to minimize temperature effects of parasitic impedances. A degenerative resistor is connected between the emitter of the bipolar transistor and the emitter resistor. The degenerative resistor varies in resistance with a change in temperature opposite that of an input resistance of the bipolar junction transistor. The first and second capacitors are selected to minimize the effect of variation of the parasitic impedance. The oscillator is converted to a frequency shift keying oscillator by adding frequency shifting means to modulate the frequency of the output signal between a first frequency and a second frequency according to a state of a digital input signal. The method of designing the oscillator as a frequency shift keying oscillator requires selecting an on-resistance of the frequency shifting means to prevent the first frequency and the second frequency from fluctuating with temperature.
Abstract:
A thermal RC network is fabricated in silicon as a lateral array of forward-biased PN junctions, which may take the form of the base-emitter junctions of bipolar transistors. Application of a clock signal from a voltage controlled oscillator to the silicon produces a heat pulse which propagates across the arrayed transistors of the thermal RC network. The resulting change in temperature produces a change in the V.sub.be of the arrayed transistors. The phase shift between the original clock signal and the changed V.sub.be is determined solely by the time constant .tau. of the particular thermal RC network. This time constant is a function only of the intrinsic thermal resistance and thermal capacitance of the silicon and the spacing of the laterally-arrayed transistors. The time constant is independent of the amplitude, frequency, and duty cycle of the original clock signal. The original clock signal and the time-delayed output of the RC network can be compared, and the phase shift determined. A voltage corresponding to this phase shift is then generated and fed back into the voltage controlled oscillator, producing an output signal having a constant frequency.
Abstract:
A phase locked loop ("PLL") 28 containing apparatus for automatically causing the PLL to achieve phase lock when first energized or after having lost phase lock. In addition to a phase detector 4, loop filter 13, voltage controlled oscillator ("VCO") 14 and feedback from the VCO to the phase detector 16, the PLL has a sweep circuit 30. The sweep circuit cooperates with the loop filter when the PLL is not in phase lock to automatically generate a control voltage for the VCO which control voltage increases linearly with time until the PLL achieves phase lock or until the control voltage has reached the largest voltage in the dynamic input range of the VCO. In the event that phase lock is not achieved during the period of the increasing voltage, the control voltage decreases linearly with time to drive the PLL into phase lock.
Abstract:
A self-tuning VCO (116) receives a control voltage input (Vcont) (114) and an adjustable programmable voltage (Vadj) (122) and provides optimized locked conditions even under variations in temperature. A radio temperature is measured and stored (204) while Vadj (122) is initialized and stepped and Vcont (114) attempts to lock the VCO on frequency. Once a locked condition is achieved, the Vcont (114) is monitored to determine if it falls within a predetermined voltage range. If a non-optimized condition is detected, then the Vadj (122) is automatically adjusted until the VCO (116) becomes locked with a Vcont which falls within the predetermined voltage range. When a locked condition is achieved, the radio temperature is monitored and compared (212) to the original stored temperature (204). If a temperature threshold limit is reached (216) then the VCO is re-checks itself for a locked condition and re-optimizes itself to accommodate for the variations in temperature.
Abstract:
A stabilized oscillation circuit includes a bias circuit which controllably biases a bipolar-transistor-driven crystal oscillator circuit. The bipolar-transistor-driven crystal oscillator circuit is a modified version of a conventional transistor-driven oscillator, such as a Hartley, Pierce or Colpitts-type circuit. The bias circuit includes a first current providing a reference current through a Schottky diode and a pair of bipolar transistors. The bipolar-transistor-driven crystal oscillator circuit includes an input and an output, where the input of the bipolar-transistor-driven crystal oscillator circuit is coupled to the bias circuit. The bipolar-transistor-driven crystal oscillator circuit includes a second current through a second bipolar transistor. The second current tracks the reference current so that the output of the bipolar-transistor-driven oscillator circuit is substantially constant over variations in ambient temperature.
Abstract:
A temperature compensated complementary metal-insulator-semiconductor oscillator receives a temperature independent reference voltage from an external source. The temperature independent reference voltage is attenuated and summed with a threshold voltage in order to bias a gate electrode of MOSFET. A bipolar p-n junction diode is connected to the MOSFET at a source electrode in order to bias the MOSFET with a temperature dependent forward voltage drop to compensate for temperature variations therein. The MOSFET controls a temperature independent current. A current mirror assembly receives the current and controls a Schmitt trigger oscillator. The Schmitt trigger oscillator generates a signal having a temperature independent constant period.
Abstract:
A closed loop integrated circuit temperature stabilizer 10 has an on-chip temperature sensor 12 for supplying a voltage indication of temperature to an op amp 22 which maintains chip temperature equilibrium by controlling a load transistor 30 which draws current through on-chip heating means 16.
Abstract:
A high-speed temperature-compensated integrated circuit voltagecontrolled oscillator for use in applications such as phaselocked loops. The oscillator is a nonsaturating emitter-coupled multivibrator wherein temperature compensation is achieved by establishing virtually identical temperature dependency in the current which charges the multivibrator timing capacitor and in the voltage swing which appears across the timing capacitor.
Abstract:
Disclosed are temperature compensated one-shot multivibrator circuits particularly adapted for use in industrial tachometers. The one-shots have compensating diodes or transistor junctions in the collector circuits of the timing transistors. In some of the circuits the junctions are matched to insure equal current flow through both the compensated and compensating junctions. They produce pulses have a pulse width that is substantially constant over a wide temperature range.