The embodiments pertain to reduction of conducted noise in direct current brushless fans used in network communication applications, and can also be used to reduce conducted noise emanating from other DC loads. The embodiments can be incorporated in the fan(s), or incorporated in the controlling electronics circuitry.
Direct Current (DC) fans are predominantly used to cool electronic equipment. The fans are typically brushless in design, to reduce cost and improve reliability. The commutation of the fan generates a current pulse on the power source. This current pulse varies in amplitude and frequency, proportional to the fan speed. Typically, the current pulse ranges from 0 Hz to 500 Hz, and may also exhibit harmonics well into the 10 kHz to 20 kHz range.
Regulatory agencies are now requiring the conducted noise in the voice band to be below low levels, for example 9+10 logIc (dBrnC), where Ic is the maximum measured input current on the power port of the telecommunications equipment. Equipment that is designed to measure analog signals with C-Message weighting is specified to measure the noise. Typically, this is performed using a Transmission Impairment Measurement Set (TIMS) that is used for measurements on Plain Old Telephone Systems (POTS). The term dBrnC is a decibel relative measurement with C-Message weighting, and is specified as dBrnC=dBm+90. Thus, as an example, an input current of 2A results in a limit of 12 dBrnC. Applying the conversion formula results in an absolute value of 12 dBrnC−90=−78 dBm in the voice band range.
Attenuating noise down to this low of a level can be achieved using a passive low-pass filter consisting of inductors, capacitors, and resistors on the power supply to the fan(s) or on the power supply port of the equipment cooled by the fan(s). The size of the filter components can increase significantly, depending on the current level required on the power port. Passive low-pass filters are widely used technology having moderate cost. However, using low pass filters causes significant pressure on the volume available to house all the components, depending on the level of attenuation and current rating.
Another method used to reduce the noise level is to use Pulse Width Modulation (PWM) on the fan power input. In the case where multiple fans are used in a system, the fans' PWM drives are driven out of phase with each other to minimize the additive current pulses. U.S. published patent application 2009/0278484 A1 dated Nov. 12, 2009 shows one example of incorporating this method.
The present embodiments counteract the effects of the undesired current pulses Ifan using an active filter to cancel out the current pulses Ifan, so that a steady current Is is seen at the fan power source 11. This method advantageously allows the use of small integrated circuits that can be incorporated in the housing(s) for the fan(s) 17, or else incorporated at the power source 11 driving the fan(s) 17. This can be achieved with small component volume and moderate cost.
The present embodiments measure the undesired current pulse Ifan and translates this pulse to voltage. Then a mathematical function Vaverage−Vpulse=VP is performed using integrated circuits such as operational amplifiers. The correction voltage Vp is then presented to a voltage controlled current source or current sink 12, connected in parallel to the fan power source 11, that adds a counteracting current pulse Ip back to the source 11 to achieve a steady current Is. This operation is represented by the formula Is=Ifan+Ip. Thus, noise reduction at the system power input 11 is achieved.
The present embodiments perform the noise canceling independent of fan 17 speed. Thus, filtering down to low frequencies approaching 0 Hz can be achieved.
These and other more detailed and specific objects and features of the present invention are more fully disclosed in the following specification, reference being had to the accompanying drawings, in which:
The embodiments will now be described more fully hereinafter with reference to the accompanying drawings. The embodiments may, however, be embodied in different forms, and should therefore not be construed as limited to the embodiments set forth herein. In the Figures, the dimensions of elements may be exaggerated for clarity of illustration. Like reference characters refer to like elements throughout.
The
In one embodiment, a current sense 13 is placed in series between the voltage source 11 and fan motor(s) 17 to provide a current measurement of Ifan. The current Ifan is then converted to voltage, to allow the above-mentioned mathematical function to be performed.
An average current to voltage converter 14, placed at the output of current sense 13, performs an average current to average voltage (Vavg) conversion. A pulse current to voltage converter 15 is also placed at the output of current sense 13, and performs a conversion of pulse current to pulse voltage (Vpulse). A Vavg−Vpulse subtraction module 16, located at the output of converters 14 and 15, then performs the mathematical function to generate the correction voltage Vp.
Vp is then introduced to the control input of variable current source (or sink) 12, which converts the pulse correction voltage Vp to pulse correction current Ip. The pulse correction current Ip is the antidote to the unwanted current pulse Ifan, and is automatically added back to the source current Is by the topology of the circuit by the relationship Is=Ifan+Ip. This results in a substantially steady current Ip, and therefore minimizes noise generated by current ripple at voltage source 11.
The
Generally, the values for the various components shown on
Diode D1 is used to set the direction of current flow. It is typically a MBRS130L.
In
The low voltage value representing Ifan is then amplified using current sense amplifiers U2 and U3 (embodying modules 14 and 15, respectively). In this example, U2 and U3 are Linear Technology, Inc. LTC6101 High Voltage, High-Side Current Sense Amplifiers.
Vavg is generated by U2, and Vpulse is generated by U3.
The output voltage of U2 is determined by the equation Vavg=VR4×R6/R5. Vavg is still a pulse at the output of U2. Thus, a capacitor C2 is used to smooth the pulse to represent the average voltage to the input of module 16.
The output voltage of U3 is determined by the equation Vpulse=VR4×R3/R2.
The mathematical function VP=Vavg−VPulse (module 16) is implemented using a typical differential amplifier, US, with accompanying components R7, R8, R9, R10, C6, and C7. U5 is typically a Linear Technology 1784. The differential amplifier U5 can be embodied by many other known implementations.
Vp is then converted to current Ip (at module 12) using a current feedback amplifier, U4, with accompanying components R11, R13, and C5. These components implement variable current source 12. U4 is typically a Linear Technology 1206. The current source 12 (which can also be a current sink) can also be embodied by many other known implementations.
The above description is included to illustrate the operation of some embodiments, and is not meant to limit the scope. From the above discussion, many variations will be apparent to one skilled in the art that would yet be encompassed by the spirit and scope of the embodiments. For example, the invention can be used to reduce unwanted conducted noise generated by any DC load, not just fans.
Number | Name | Date | Kind |
---|---|---|---|
5268623 | Muller | Dec 1993 | A |
6717380 | Sutter et al. | Apr 2004 | B1 |
6768282 | Lutter et al. | Jul 2004 | B2 |
8138712 | Yamada | Mar 2012 | B2 |
20030122515 | Lutter et al. | Jul 2003 | A1 |
20040178759 | Nakamura et al. | Sep 2004 | A1 |
20060145639 | Song et al. | Jul 2006 | A1 |
20070274015 | Isham | Nov 2007 | A1 |
20080079380 | Knittel et al. | Apr 2008 | A1 |
20090254300 | Schneider et al. | Oct 2009 | A1 |
20090278484 | Nair et al. | Nov 2009 | A1 |
20100164416 | Yamada | Jul 2010 | A1 |
20100171456 | Chakrabarti et al. | Jul 2010 | A1 |
20100171457 | Letor et al. | Jul 2010 | A1 |
Number | Date | Country | |
---|---|---|---|
20140091735 A1 | Apr 2014 | US |