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PART C Click on the third scenario shown below. In this soenario, we have two different shaped fluid volumes connectedtpgether by a horizontal tube. One can add weight to the vertical tube on the lefthand side. [line will see what happens to the pressure at different plaoes in these two intercon nected 1urolu mes. Image byrobert Hare, 20191 [Em-ed from PHEI' 5mm Step 1 Turn on the grid and turn off the Atmosphere. Place a pressure gauge at the 3meter grid location and measure the pressure. 3 Meter Pressure: 22.5D1 kPa Step 2 Add a 250 kg weight to the tube on the left-hand container. "You will notice that three things happen. First the weight displaces the uid in the tube on the lefthandside. The uid also rises in the container on the righthand side. and the pressure at our selected location {3meter location} also rises. Theoretically, the pressure at the 3-rneter point can be determined a couple of different ways using Equation 1. P=mn+pym Equation 2 p=pym Equation 3 In Equation 2, the external pressure is the pressure due to the weight of the block on the left ha nd side. One can measure this external pressure by placing another pressure gauge between the weight and the fluid. Record this measurement. The pressure p in Equations 2 and 3 should be the same since according to Pascal's principle the pressure at a given height in the uid should always be the same. 1ii'ii'ith the 250 kg weight added, record the pressure [with the weight added} at 3 meters, and the heights of the fluid {using the ruler} on the left (hi) and right hr} sides [heights are measured from the bottom]. Use the Equation 2 and 3 above to calculate the theoretical pressure at 3 meters from left and right measurements. How do your measurements compare? Repeat this for one of the other weight combinations SUD kg weight, TED _l:_g or li] kg. 3 meter 22.3o3 531 23.132 531 23.4ao 53; 23.322 Egg pressure Height of Fluid . 2.41 m 2.44 m Ri ht