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A U-shaped tube, open to the air on both ends. contains mercury. Water is poured into the left arm until the water column is 10.6 cm deep. How far upward from its initial position does the mercury in the right arm rise?

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A U-shaped tube, open to the air on both ends. contains mercury. Water is poured into the left arm until the water column is 10.6 cm deep. How far upward from its initial position does the mercury in the right arm rise?

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Asked by: Rajveer Prajapat
Created at: 2025-10-10 14:49:01

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# Problem Analysis Given: - A U-shaped tube open to air at both ends. - Mercury is initially at the same level in both arms. - Water is poured the left arm, forming a column **10.6 cm** high. We are to find **how much the mercury in the right arm rises** (let's call this rise \( h \)). # Step-by-Step Solution ## 1. Initial Setup - The air pressure at the top of both arms is atmospheric and equal. - The water column pushes down on the mercury in the left arm, causing mercury to rise in the right arm. ## 2. Pressure Relationships **At the same horizontal level at the bottom of the U-tube:** - The pressure must be equal in both arms. Let: - \( \rho_{Hg} \) = density of mercury (\( 13,600 \, \text{kg/m}^3 \)) - \( \rho_{w} \) = density of water (\( 1,000 \, \text{kg/m}^3 \)) - \( g \) = acceleration due to gravity (\( 9.8 \, \text{m/s}^2 \)) - \( h_w = 10.6 \, \text{cm} = .106 \, \text{m} \) (water column height) - \( h \) = the rise of mercury in the right arm (\( \text{m} \)) After pouring water: - The mercury surface in the left arm drops by \( h \). - The mercury surface in the right arm rises by \( h \). - The difference in mercury levels between the two arms is \( 2h \). ## 3. Applying Hydrostatic Pressure **Left arm (from top to bottom):** - Atmospheric pressure (\( P_{atm} \)) - Water column: \( \rho_w g h_w \) - Mercury column: \( \rho_{Hg} g (H - h) \) (if \( H \) is initial height, but cancels out) **Right arm (from top to bottom):** - Atmospheric pressure (\( P_{atm} \)) - Mercury column: \( \rho_{Hg} g (H + h) \) Set the pressures at the bottom equal (at the same horizontal level): \[ P_{atm} + \rho_w g h_w + \rho_{Hg} g (H - h) = P_{atm} + \rho_{Hg} g (H + h) \] ## 4. Simplify Equation Cancel \( P_{atm} \) and \( \rho_{Hg} g H \): \[ \rho_w g h_w - \rho_{Hg} g h = \rho_{Hg} g h \] \[ \rho_w g h_w = 2\rho_{Hg} g h \] \[ h = \frac{\rho_w h_w}{2\rho_{Hg}} \] ## 5. Plug in Values \[ h = \frac{(1,000 \, \text{kg/m}^3)(.106 \, \text{m})}{2 \times 13,600 \, \text{kg/m}^3} \] \[ h = \frac{106}{27,200} \] \[ h \approx .003897 \, \text{m} \] \[ h \approx .39 \, \text{cm} \] # Final Answer **The mercury in the right arm rises about \( \boxed{.39 \ \text{cm}} \) from its initial position.** --- ## Summary Table | Quantity | Value | |----------------|------------------| | Water column | \( 10.6 \) cm | | Mercury rise | \( .39 \) cm | --- **Diagram (text only):** ``` Left: water (10.6 cm) + mercury (lowered) Right: mercury (raised) Difference in mercury levels: 2h h ≈ .39 cm ```

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