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IR3721 Datasheet(PDF) 6 Page - International Rectifier |
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IR3721 Datasheet(HTML) 6 Page - International Rectifier |
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6 / 16 page ![]() IR3721 DATA SHEET Page 6 of 16 www.irf.com 09/15/08 THERMAL COMPENSATION FOR INDUCTOR DCR CURRENT SENSING The positive temperature coefficient of the inductor DCR can be compensated if RT varies inversely proportional to the DCR. DCR of a copper coil, as a function of temperature, is approximated by ) ⋅ ) ( + ( ⋅ ) ( = ) ( Cu R R TCR T T T DCR T DCR - 1 Equation 2 TR is some reference temperature, usually 25 °C, and TCRCu is the resistive temperature coefficient of copper, usually assumed to be 0.39 %/°C near room temperature. Note that equation 2 is linearly increasing with temperature and has an offset of DCR(TR) at the reference temperature. If RT incorporates a negative temperature coefficient thermistor then temperature effects of DCR can be minimized. Consider a circuit of two resistors and a thermistor as shown below. Rs Rth Rp Figure 2 RT Network If Rth is an NTC thermistor then the value of the network will decrease as temperature increases. Unfortunately, most thermistors exhibit far more variation with temperature than copper wire. One equation used to model thermistors is ⎟ ⎟ ⎠ ⎞ ⎜ ⎜ ⎝ ⎛ ⎟⎟ ⎠ ⎞ ⎜⎜ ⎝ ⎛ ⋅ ) ( = ) ( 0 1 1 0 T T th th e T R T R - β Equation 3 where Rth(T) is the thermistor resistance at some temperature T, Rth(T0) is the thermistor resistance at the reference temperature T0, and β is the material constant provided by the thermistor manufacturer. Kelvin degrees are used in the exponential term of equation 3. If RS is large and RP is small, the curvature of the equivalent network resistance can be reduced from the curvature of the thermistor alone. Although the exponential equation 3 can never compensate linear equation 2 at all temperatures, a spreadsheet can be constructed to minimize error over the temperature interval of interest. The equivalent resistance RT of the network shown as a function of temperature is ) ( + + = ) ( T R R R T R th p s T 1 1 1 Equation 4 using Rth(T) from equation 3. Equation 2 may be rewritten as a new function of temperature using equations 2 and 4 as follows: () ) ( + ⋅ ) ( = ) ( Τ T DCR R R T R V T I 2 CS 1 CS T R FS Equation 5 With Rs and Rp as additional free variables, use a spreadsheet to solve equation 5 for the desired full scale current while minimizing the IFS(T) variation over temperature. |
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