Mathcad Calculates Input Capac
abstract: step-down buck regulators are extremely popular in a variety of portable and non-portable equipment. these buck converters are terminated with an input capacitor, cin and an output capacitor, co, at the output. cin provides high-frequency filtering, so that vin has low ripple. this application note helps a system designer to set-up mathcad and compute cin for a particular step-down dc-dc regulator design.
step-down buck regulators are used in portable and non-portable equipment, such as pdas, cell phones, computers, telcom/networks, and consumer products. these buck converters are terminated with an input capacitor, cin, at the input, and an output capacitor, co, at the output. the function of both capacitors is to provide high-frequency filtering, so that vin and vo are close to pure dc, with little ripple noise.
a capacitor is often represented by a series combination of r, l, and c. r is the equivalent series resistance (esr) and l is the equivalent series inductance (esl). the term c is equal to the ideal capacitor value.
figure 1 shows a typical schematic of a synchronous buck power stage and the associated waveforms to be used for the derivations and calculations.
figure 1. typical synchronous buck power and waveforms. setting up variables and data for example calculation in mathcad: input voltage vi := 12 n := 10-9
output voltage vo := 3.3 u := 10-6, k := 10³
output current io := 25 m := 10-3
high-side switch drop vhs := 0.227
low-side switch drop vls := 0.113
switching current rise time trs := 25 × n
switching current fall time tfs := 25 × n
switching frequency fs := 600 × k
duty cycle d := (vo + vls) / (vi - vhs + vls) d = 0.287
switch(q1) on time ton := d / fs
switch(q1) off time toff := 1 / fs - ton
converter efficiency η := 0.9
input current iin := vo × io / η × vi iin := 7.639
output inductor pk-pk ripple current
irpl := 0.3 × io
input capacitor cin := 40 × u (4 x 10uf ceramic of esr = 10mω each and esl = 2.5nh each)
input capacitor esr esrcin := 2.5 × m
input capacitor esl eslcin := 0.625 × n
as seen in figure 1, the output ripple current through the input capacitor results in voltage across cin that reflects the values of esr, esl, and c. the esr and esl cause fast step voltage rise and fall, whereas c has a linear voltage rise and fall due to the fact that the capacitor charges and discharges. at the start of ton, cin sees a negative step current, which will produce a negative step voltage given by the following equation: during ton, the capacitor discharges an average current of (io-iin), which causes a linear δv of: the total voltage deviation from the start of ton to the end of ton is the summation of the above: similarly, but with opposite polarity, at the start of toff and during toff, the following voltage deviations are calculated: the peak-to-peak ripple is equal to the higher of the two, which is δvoff~1v. as seen from the above, most of the ripple is caused by esl and the fast di/dt. di/dt of 1a/ns is very realistic in today's mhz dc-dc converters. therefore, to reduce the ripple, more capacitors would need to be placed in parallel. lower value ceramic capacitors, such as 0.1uf in the 0805 or 1206 package, have half the esl of the 10uf, or ~1.2nh. place the 0.1uf as close as possible to the sensitive decoupling points.
another parameter that needs to be determined is the rms current through the input capacitor, so that the capacitor irms rating is not exceeded. from the icin waveform, the rms current can be approximated (since the peak-to-peak inductor ripple current is usually 20-30% of io max) to be: where d = (vo + vls) / (vin + vls + vhs), and iin = (vo × io) / η × vin to simplify further, let d = vo/vin (since v0 >> vls, and vin + vls - vhs ~ vin), and iin = vo × io/vin (since efficiency η ~ 1), so that the icinrms equation above becomes: the simplified version produces only ~1.4% error, and involves only three known parameters: vi, vo, and io. vo is fixed, and io, vi can have a specified range, depending on the application. however, icinrms always has a maximum value of io/2, which happens at vi = 2vo, and decreases the value for vi 2lo. the plot in figure 2 below illustrates this:
figure 2.
due to the high di/dt and pulsating current, a ceramic capacitor is chosen, for its low esr and esl. a higher ripple current rating is required at high-frequency to contain the switching spikes. make sure the rms current rating of the capacitor is well above the maximum operating rms current. for long-term reliability, choose a capacitor that will exhibit less than a 10°c temperature rise. most capacitor manufacturers provide plots that show rms current vs. temperature rise.
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step-down buck regulators are used in portable and non-portable equipment, such as pdas, cell phones, computers, telcom/networks, and consumer products. these buck converters are terminated with an input capacitor, cin, at the input, and an output capacitor, co, at the output. the function of both capacitors is to provide high-frequency filtering, so that vin and vo are close to pure dc, with little ripple noise.
a capacitor is often represented by a series combination of r, l, and c. r is the equivalent series resistance (esr) and l is the equivalent series inductance (esl). the term c is equal to the ideal capacitor value.
figure 1 shows a typical schematic of a synchronous buck power stage and the associated waveforms to be used for the derivations and calculations.
figure 1. typical synchronous buck power and waveforms. setting up variables and data for example calculation in mathcad: input voltage vi := 12 n := 10-9
output voltage vo := 3.3 u := 10-6, k := 10³
output current io := 25 m := 10-3
high-side switch drop vhs := 0.227
low-side switch drop vls := 0.113
switching current rise time trs := 25 × n
switching current fall time tfs := 25 × n
switching frequency fs := 600 × k
duty cycle d := (vo + vls) / (vi - vhs + vls) d = 0.287
switch(q1) on time ton := d / fs
switch(q1) off time toff := 1 / fs - ton
converter efficiency η := 0.9
input current iin := vo × io / η × vi iin := 7.639
output inductor pk-pk ripple current
irpl := 0.3 × io
input capacitor cin := 40 × u (4 x 10uf ceramic of esr = 10mω each and esl = 2.5nh each)
input capacitor esr esrcin := 2.5 × m
input capacitor esl eslcin := 0.625 × n
as seen in figure 1, the output ripple current through the input capacitor results in voltage across cin that reflects the values of esr, esl, and c. the esr and esl cause fast step voltage rise and fall, whereas c has a linear voltage rise and fall due to the fact that the capacitor charges and discharges. at the start of ton, cin sees a negative step current, which will produce a negative step voltage given by the following equation: during ton, the capacitor discharges an average current of (io-iin), which causes a linear δv of: the total voltage deviation from the start of ton to the end of ton is the summation of the above: similarly, but with opposite polarity, at the start of toff and during toff, the following voltage deviations are calculated: the peak-to-peak ripple is equal to the higher of the two, which is δvoff~1v. as seen from the above, most of the ripple is caused by esl and the fast di/dt. di/dt of 1a/ns is very realistic in today's mhz dc-dc converters. therefore, to reduce the ripple, more capacitors would need to be placed in parallel. lower value ceramic capacitors, such as 0.1uf in the 0805 or 1206 package, have half the esl of the 10uf, or ~1.2nh. place the 0.1uf as close as possible to the sensitive decoupling points.
another parameter that needs to be determined is the rms current through the input capacitor, so that the capacitor irms rating is not exceeded. from the icin waveform, the rms current can be approximated (since the peak-to-peak inductor ripple current is usually 20-30% of io max) to be: where d = (vo + vls) / (vin + vls + vhs), and iin = (vo × io) / η × vin to simplify further, let d = vo/vin (since v0 >> vls, and vin + vls - vhs ~ vin), and iin = vo × io/vin (since efficiency η ~ 1), so that the icinrms equation above becomes: the simplified version produces only ~1.4% error, and involves only three known parameters: vi, vo, and io. vo is fixed, and io, vi can have a specified range, depending on the application. however, icinrms always has a maximum value of io/2, which happens at vi = 2vo, and decreases the value for vi 2lo. the plot in figure 2 below illustrates this:
figure 2.
due to the high di/dt and pulsating current, a ceramic capacitor is chosen, for its low esr and esl. a higher ripple current rating is required at high-frequency to contain the switching spikes. make sure the rms current rating of the capacitor is well above the maximum operating rms current. for long-term reliability, choose a capacitor that will exhibit less than a 10°c temperature rise. most capacitor manufacturers provide plots that show rms current vs. temperature rise.
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