Now, since the two sides TR, RU are equal to the two sides AL, LB, and they contain equal angles,
therefore the parallelogram RW is equal and similar to the parallelogram HL.
Since again AL is equal to RT, and LM to RS, and they contain right angles,
therefore the parallelogram RX is equal and similar to the parallelogram AM.
For the same reason LE is also equal and similar to SU;
therefore three parallelograms of the solid AE are equal and similar to three parallelograms of the solid XU.
But the former three are equal and similar to the three opposite, and the latter three to the three opposite; [XI. 24]
therefore the whole parallelepipedal solid AE is equal to the whole parallelepipedal solid XU. [XI. Def. 10]
Let DR, WU be drawn through and meet one another at Y, let aTb be drawn through T parallel to DY, let PD be produced to a, and let the solids YX, RI be completed.
Then the solid XY, of which the parallelogram RX is the base and Yc its opposite, is equal to the solid XU of which the parallelogram RX is the base and UV its opposite,
for they are on the same base RX and of the same height, and the extremities of their sides which stand up, namely RY, RU, Tb, TW, Se, Sd, Xc, XV, are on the same straight lines YW, eV. [XI. 29]
But the solid XU is equal to AE:
therefore the solid XY is also equal to the solid AE.
And, since the parallelogram RUWT is equal to the parallelogram YT for they are on the same base RT and in the same parallels RT, YW, [I. 35]
while RUWT is equal to CD, since it is also equal to AB,
therefore the parallelogram YT is also equal to CD.
But DT is another parallelogram;
therefore, as the base CD is to DT, so is YT to DT. [V. 7]
And, since the parallelepipedal solid CI has been cut by the plane RF which is parallel to opposite planes,
as the base CD is to the base DT, so is the solid CF to the solid RI. [XI. 25]
For the same reason, since the parallelepipedal solid YI has been cut by the plane RX which is parallel to opposite planes,
as the base YT is to the base TD, so is the solid YX to the solid RI. [XI. 25]
But, as the base CD is to DT, so is YT to DT;
therefore also, as the solid CF is to the solid RI, so is the solid YX to RI. [V. 11]
Therefore each of the solids CF, YX has to RI the same ratio;
therefore the solid CF is equal to the solid YX. [V. 9]
But YX was proved equal to AE;
therefore AE is also equal to CF.