Implementing Analog Dimming on the DS39xx CCFL Controllers
|© Dec 14, 2007, Maxim Integrated Products, Inc.
Abstract: The DS3881, DS3882, DS3988, DS3991, DS3992 and DS3994 are controllers for cold-cathode fluorescent lamps (CCFLs) that backlight liquid crystal displays (LCDs). To achieve satisfactory visual results or conserve lamp life, dimming is required in most applications. This application note first introduces the two dimming approaches commonly used for CCFLs. It then describes how to implement analog dimming on the DS39xx CCFL controllers.
CCFL Dimming Methods
There are two common methods to dim CCFLs: burst dimming, which is also called PWM dimming or digital dimming, and analog dimming. This article discusses the advantages and disadvantages of each method.
Burst dimming turns the CCFLs on and off at a certain frequency, which is called the PWM dimming frequency. If the PWM dimming frequency is greater than 60Hz, the human eye cannot detect that the CCFLs are switching on and off. During the high period of the PWM cycle, the CCFLs are turned on and work at the lamp frequency. During the low period of the PWM cycle, the CCFLs are turned off and no current flows through them. By adjusting the duty cycle of the PWM pulses, one can thus increase or decrease the brightness of the CCFLs. The principal advantage of burst dimming is that it can achieve a very large dimming ratio. In some applications, however, the PWM dimming frequency may interfere with the vertical synchronous frequency of the display signals, thereby causing visible effects on the screen. Burst dimming can also cause audible transformer noise.
Instead of turning on the CCFLs in bursts, analog dimming keeps the CCFLs on continuously. Lamp brightness is adjusted by varying the lamp current amplitude. Obviously, a greater current amplitude results in a brighter CCFL, and a lower amplitude renders a dimmer CCFL. Analog dimming has a very narrow dimming range, which is insufficient in some applications. But analog dimming does not cause any audible transformer noise, since the PWM frequency is not present. Analog dimming, moreover, does not interfere with the vertical synchronous frequency.
Table 1 compares analog dimming and burst dimming. More information can be found in the Application Note 3997: How to Achieve a 300:1 Dimming Ratio with the DS3881/DS3882 CCFL Controllers.
Table 1. Analog Dimming and Burst Dimming Compared
|1. Narrow dimming range, no more than 3:1
2. No audible transformer noise
3. No interference with the vertical synchronous frequency
|1. Large dimming ratio up to 100:1
2. Audible transformer noise can be present.
3. The PWM dimming frequency can interfere with the vertical synchronous frequency.
Implementing CCFL Analog Dimming
The DS3881 and DS3882 CCFL controllers have built-in analog dimming control functionality. The user can adjust the lamp current by using the I²C interface to set the BLC register.
The DS3988, DS3991, DS3992, and DS3994 CCFL controllers feature burst dimming. However, with the simple external circuitry illustrated in Figure 1, these DS39xx controllers can support analog dimming effectively.
Figure 1. External circuitry required to implement analog dimming on the DS39xx CCFL controllers.
In Figure 1, R4 is the lamp-current feedback resistor. The peak voltage level across R4 is VR4. After the signal passes the diode, the peak voltage level becomes VA. The peak voltage level at the LCM input, VLCM, is the linear combination of VA and the analog dimming control voltage, VDIM. Therefore:
VLCM (peak value) is 2.35V nominal. So VDIM determines VA, which is directly related to the lamp current. Note that if R1 is left open and VDIM is not available, the circuitry is virtually part of the typical multilamp current monitor circuitry presented in the DS3992/DS3994 data sheets.
Calculating Resistor Values
To calculate the resistor values, use the system requirements and Equation 1 to obtain a and b. Then use Equations 2 and 3 to calculate the appropriate values for R1, R2, and R3.
For example, if an application requires that the lamp current be 7mARMS when VDIM is 0V and 3mARMS when VDIM is 3.3V, then VA equals 19.1Vpk (√2 × 7mARMS × 2kΩ - 0.7V) when VDIM = 0V, and VA equals 7.8Vpk (√2 × 3mARMS × 2kΩ - 0.7V) when VDIM = 3.3V. Using these conditions and Equation 1, one can determine that a = 0.422 and b = 0.123.
With a and b known, now set R3 with an arbitrary value (no more than 10kΩ). Then solve Equations 2 and 3 for R1 and R2. If R3 is chosen as 3.4kΩ, then R1 = 3.65kΩ and R2 = 12.4kΩ. Since there are harmonics in the lamp current, the crest factor of the current waveform is not always √2. Thus some adjustments for the resistor values are needed to achieve the desired results. In this case, the final values of R1 and R2 are 4.42kΩ and 11.5kΩ, respectively.
In the application described above, the lamp current decreases as the dimming control voltage increases. This function is called negative-slope dimming. Conversely, positive-slope dimming means that the lamp current increases as the dimming control voltage increases. If positive-slope dimming is desired, an inverting circuit can be added between VDIM and R1.
Figures 2 and 3 show the measured lamp-current waveforms based on the circuitry in Figure 1. Figure 2 is captured at VDIM = 0V and Figure 2 at VDIM = 3.3V. The dimming ratio in this case is 2.33:1.
Figure 2. Lamp current waveforms at VDIM = 0V.
Figure 3. Lamp current waveforms at VDIM = 3.3V.
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Unknown: Dec 14, 2007