diff --git a/CHI.R b/CHI.R
index 8994f2e..10413f6 100644
--- a/CHI.R
+++ b/CHI.R
@@ -296,6 +296,12 @@ amperometry2df <- function(datafilename, wearea = 1) {
    # Calculate current density
    currentdensity <- ff$current / wearea
    ff <- cbind(ff, currentdensity = currentdensity)
+   # Calculate charge densities and differentials
+   charge.df <- It2charge(ff$currentdensity, ff$time)
+   ff <- cbind(ff, timediff = charge.df$timediff, 
+      chargedensity = charge$charge, 
+      sumchargedensity = charge$sumcharge, 
+      dQdt = charge$dQdt)
    #
    ### Collect attributes of this experiment
    # These attributes are specific for each kind of experiment,
diff --git a/common.R b/common.R
index 1f1bf96..f63d6fa 100644
--- a/common.R
+++ b/common.R
@@ -3,6 +3,7 @@
 # Taha Ahmed, Jan 2011
 
 # CONTENTS
+# >>>> It2charge
 # >>>> ProvideSampleId
 # >>>> ConvertRefPot
 # >>>> Celsius2Kelvin
@@ -13,6 +14,31 @@
 
 
 
+##################################################
+################### It2charge ####################
+##################################################
+It2charge <- function (current, time) {
+   ## Calculates charge etc. for amperometric data
+   ## current may be a current or a current density
+   ## (up to the calling function to keep track of which it is)
+   # Calculate the difference of the time vector
+   timediff <- c(time[1], diff(time))
+   # timediff times the current gives the charge,
+   # since the time vector can be considered as
+   # the cumulative time, while we need to multiply
+   # the current with the time elapsed since the last 
+   # current measurement (the timediff).
+   charge <- current * timediff
+   differential <- cumsum(charge) / time
+   # Prepare the return dataframe
+   ff <- data.frame(time = time, timediff = timediff, 
+      current = current, charge = charge, 
+      sumcharge = cumsum(charge), dQdt = differential)
+   return(ff)
+}
+
+
+
 ##################################################
 ################ ProvideSampleId #################
 ##################################################