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The page computes ideal conducting parallel plate Casimir pressure from negative pi squared h bar c, divided by two hundred forty times gap to the fourth power. This source formula uses SI units. Start with a twenty nanometer gap. We plot attraction magnitude, so the graph is positive even though the signed pressure is negative. The initial magnitude is about eight thousand one hundred twenty five point seven nine pascals. Increase the gap from twenty to forty nanometers while keeping all other parameters fixed. The marker follows the source inverse fourth power curve on a fixed linear scale. Doubling the gap multiplies the denominator by sixteen, so the attraction magnitude becomes one sixteenth as large. The plot is quantitative formula geometry, not the decorative cavity animation or an experimentally calibrated material model. At forty nanometers the attraction magnitude is about five hundred seven point eight six pascals. The signed pressure remains negative. Real materials, temperature corrections and surface imperfections are outside this page’s force expression. Its temperature and oscillation controls do not change this computed pressure. Now hold the gap at twenty nanometers. Pressure magnitude is fixed at about eight thousand one hundred twenty five point seven nine pascals. Force equals pressure times area. One square millimeter is one millionth of a square meter. With area one square millimeter, the force magnitude is about zero point zero zero eight one two six newtons. Increase plate area from one to four square millimeters without changing the gap. The force marker rises on a straight line. Quadrupling area quadruples force magnitude, because the pressure expression is independent of area. The separate gray reference line holds the original force magnitude. These are fixed numeric axes and an ideal uniform pressure assumption, not a simulation of plate bending or fringe fields. At four square millimeters the force magnitude is about zero point zero three two five zero three newtons. Its signed value is negative, indicating attraction in the source convention. Pressure magnitude has not changed. This separates the material-independent source ideal pressure calculation from total force over the chosen plate area. The page also reports an illustrative energy-density fixture. Its code multiplies zero point zero zero four one four by ten divided by gap in nanometers, squared. This is a source display rule, not a derived cutoff integral or a measurement of extractable quantum energy. At ten nanometers the displayed value is zero point zero zero four one four joules per cubic meter. Increase the gap from ten to twenty nanometers. Follow this separate inverse square curve. Doubling the gap reduces the fixture to one quarter. This exponent is two, unlike the pressure exponent four taught earlier. The graph explicitly represents the page’s illustrative fixture, so it must not be interpreted as a general quantum field theory prediction. At twenty nanometers the fixture is zero point zero zero one zero three five joules per cubic meter. The page sets net extractable work to zero. Its cartoon particles, oscillation preset and random cycle display do not measure vacuum-energy generation. This video explains the actual authored calculations and their limitations, preserving the original tool.