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M4670 データシート(PDF) 6 Page - Unisonic Technologies |
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M4670 データシート(HTML) 6 Page - Unisonic Technologies |
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6 / 9 page ![]() M4670 Preliminary CMOS IC UNISONICTECHNOLOGIESCO.,LTD 6 of 9 www.unisonic.com.tw QW-R502-442.b APPLICATION INFORMATION GENERAL AMPLIFIER FUNCTION The M4670 output signal consists of two, BTL connected, of course, the output signal can also be a pulse signal, the minimum width of each pulse is approximately 350ns. The two outputs can pulse independently exception that they both may never pulse simultaneously as this would result in zero volts across the BTL load. But in the same row of as the output pulse occurred in this case, they are connected together, as a broader pulse, to achieve an effective 100% duty cycle occurs. For a given supply voltage and load impedance, the maximum audio output power effects. The M4670 chip can achieve much high efficiencies than the class AB amplifier, while maintaining acceptable THD performance. The short driver pulse output means, a good efficiency can be issued with the M4670 inductive load. For the typical sensor load audio amplifier is a very passive. To this end, the load can act as its own filter. POWER DISSIPATION AND EFFICIENCY In general, efficiency is considered useful in the work required to produce a different power dissipated in the integrated circuit usually it is divided by the total energy output ratio. For audio systems, the energy delivered in the audible bands is considered useful including the distortion products of the input signal. Sub-sonic (DC) and super-sonic components (>22kHz) are not useful. The difference between the power flowing from the power supply and the audio band power being transduced is dissipated in the M4670 and in the transducer load. The amount of power dissipation in the M4670 is very low. This is because the on resistance of the switches used to form the output waveforms is typically less than 0.25Ω. This leaves only the transducer load as a potential "sink" for the small excess of input power over audio band output power. The M4670 dissipates only a fraction of the excess power requiring no additional PCB area or copper plane to act as a heat sink. DIFFERENTIAL AMPLIFIER EXPLANATION The M4670 is a fully differential amplifier with differential input and output stages. A differential amplifier amplifies the difference between the two input signals. Traditional audio power amplifiers have typically offered only single-ended inputs resulting in a 6dB reduction in signal to noise ratio relative to differential inputs. The M4670 also provides the possibility of DC input coupling, eliminating the need for two external AC coupling, DC blocking capacitors. The M4670 also can be used, but as a single-ended input amplifier while still retaining it is an entirely different interests. The main advantage of a differential amplifier is to increase common-mode rejection ratio (CMRR) for a single input amplifier. SHUTDOWN FUNCTION In order to reduce power consumption while not in use, the M4670 contains shutdown circuit current consumption reduced to less than the reduced 0.01μA. For the closure of trigger point is displayed as a table of electrical characteristics and typical shutdown hysteresis voltage diagram found in some of the typical performance characteristics. The best is to switch on the ground and use the smallest current supply, while in the closed state. The M4670 may be disabled chip off the ground and supply voltage, the idle current is larger than the typical value of reduced 0.01μA. Total harmonic distortion may increase, but also can be observed when the voltage is less than the diameter of the shutdown pin in PLAY mode. There has a resistor connected between GND and Shutdown pins in the M4670 internal, and this resistor is designed to eliminate any unnecessary state changes, when the Shutdown pin is floating. To minimize the supply current when the M4670 working in the Shutdown mode, if the M4670 don’t working in the Shutdown mode, the amount of additional resistor current due to the internal shutdown resistor can be found be Equation (1) below. (VSD - GND) / 300kΩ (1) The difference is only 0.5V, the current additional 1.7μA, lots will be drawn, while in the closed state. |
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