LM4910 stereo headphone amplifier.
LM4910 [pertaining to|belonging to] the Boomer [series of|group of] National Semiconductors is an [built-in|integrated] stereo amplifier [mainly|primarily] [meant for|aimed at] stereo headphone [applications|usages]. The IC [could be|could very well be] [controlled|operated] from 3.3V ans its [can provide|can offer] 0.35mW output power into a 32 ohm [load|headphone]. The LM4910 [possesses|is equipped with] [very low|surprisingly low] distortion ([less than|much less than] 1%) [along with|in conjunction with] the shutdown current is [lower than|below] 1uA. This [low|minimal] [shut down|power down] current [considers|assumes] it [appropriate for|most suitable for] battery [controlled|dominated] [applications|programs]. The IC is so [created|designed] [that there are|that we have] no need of the output coupling capacitors, half supply by-pass capacitors and bootstrap capacitors. More features of the IC are switch ON/OFF clicking noise removal, on the surface programmable gain etc.
How to Build a Stereo headphone amplifier
Stereo headphone amplifier LM4910
Circuit diagram of the LM4910 stereo headphone amplifier is witnessed above. C1 and C2 are actually the input DC decoupling capacitors for the left together with right input channels. R1 along with R2 tend to be the individual input resistors. R3 is the feed back resistor for left channel whereas R4 is the feed back resistor for the right channel. C3 is the supply of power filter capacitor. The feed-back resistors additionally implements the closed-loop gain together with the involved input resistors.
The IC can be purchased basically in SMD packages and proper care need to be applied while soldering.
The circuit could very well be operated from approximately between 2.2V to 5V DC.
The headphone load could possibly be a 32 ohm headphone.
Total optimum supply voltage is 6V and approximately above may well ruin the IC.
A logic low voltage at the shutdown pins shut downs the IC and a logic high voltage at the comparable pin activates the IC.
the LM4910 has about three operational amplifiers in house. A couple of the amplifier's include
on the surface configurable gain although the other amplifier is usually internally predetermined at the bias point behaving as a unity-gain buffer.
The closed-loop gain of the two configurable amplifiers is defined by opting the ratio of Rf
As a result, the gain for every channel of the IC is
AV = -(Rf/Ri)-------Eq#1
By just operating the loads by means of outputs VO1 and VO2 with VO3 working like a buffered bias voltage the LM4910 is not going to call for output coupling capacitors.
The standard single-ended amplifier setup in which one particular aspect of the load is linked with ground demands huge, pricey output coupling capacitors while Building a Stereo headphone amplifier
The construction like the one included in the LM4910 features a significant edge over single supply, single-ended amplifiers.
Because outputs VO1, VO2, and VO3 are generally biased at VREF = 1.58V, simply no net DC voltage is available throughout each load.
That gets rid of the importance of output coupling capacitors that happen to be recommended inside a single-supply, single-ended amplifier setup.
With no output coupling capacitors inside a regular single-supply, single-ended amplifier, the bias voltage is defined along the load which results in either elevated interior IC power waste and probable loudspeaker problems.
Energy waste can be a serious worry when making an effective amplifier. An immediate outcome of the higher power transferred to the load by a bridge amplifier can be an escalation in inside energy turbulence.
The highest power waste for any presented application could be produced by the power dissipation chart or from the earlier equation