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7. A heavy liquid with a density 11 g/cm' is poured into a U-tube as shown in the left-hand figure below. The left-hand arm of the tube has a cross-sectional area of 8.5 cm? and the right-hand arm has a cross-sectional area of 3.92 cm?

. A quantity of 97.3 g of a

light liquid with a density 1.3 g/cm' is then poured into the right-hand arm as shown in the right-hand figure below. Determine the height L of the light liquid in the column in the right arm of the U-tube, as shown in the second figure above.

Answer in units of cm.



8. If the density of the heavy liquid is 11 g/cm® by what height h1 does the heavy liquid rise in the left arm?

Answer in units of cm.

7 A heavy liquid with a density 11 g cm is poured into a U tube as shown in the left hand figure below The

Answer :

Answer:

Assuming that the two liquids do not mix:

[tex]L \approx 19.1\; \text{cm}[/tex].

[tex]h_{1} \approx 0.712\; \text{cm}[/tex].

Explanation:

To find the height of the [tex]\rho_{\text{B}} = 1.3 \; {\rm g \cdot cm^{-3}}[/tex] "light liquid" column, divide mass by density to find volume, and divide volume by cross-section area to find height:

[tex]\displaystyle L = \frac{V}{A_{\text{R}}} = \frac{m_{\text{B}} / \rho_{\text{B}}}{A_{\text{R}}} \approx \frac{(97.3 / 1.3)}{3.92} \; \text{cm} \approx 19.0934\; \text{cm}[/tex].

To find the change in the height of the [tex]\rho_{\text{A}} = 11 \; {\rm g \cdot cm^{-3}}[/tex] "heavy liquid" column, make use of the two following facts:

  • The total volume of each liquid stays the same.
  • At equilibrium, the pressure at any horizontal cross-section should be the same for each liquid column.

From each of the two facts, construct an equation about [tex]h_{1}[/tex] and [tex]h_{2}[/tex].

Note that when the "light liquid" is added, the height of the "heavy liquid" column on the right side decreased by [tex]h_{2}[/tex]. At the same time, the height of the column on the left side increased by [tex]h_{1}[/tex]. Since the total volume of the "heavy liquid" stays unchanged, the volume that went down on the right side [tex]h_{2}\, A_\text{R}[/tex] should match the volume that went up on the left side [tex]h_{1}\, A_\text{L}[/tex]:

[tex]h_{2}\, A_\text{R} = h_{1}\, A_\text{L}[/tex].

In a liquid of density [tex]\rho[/tex], the pressure at a depth of [tex]h[/tex] would be [tex]\rho\, g\, h[/tex], where [tex]g[/tex] is the gravitational field strength. At equilibrium, the pressure at the bottom of the "heavy liquid" column of depth [tex](h_{1} + h_{2})[/tex] is supposed to match that at the bottom of the "light liquid" column of depth [tex]L[/tex]. Thus:

[tex]\rho_{\text{A}}\, g \, (h_{1} + h_{2}) = \rho_{\text{B}}\, g\, L[/tex].

Thus:

[tex]\displaystyle h_{1} + h_{2} = \frac{\rho_{\text{B}}\, L}{\rho_{\text{A}}}[/tex].

To find [tex]h_{1}[/tex], rearrange one of the two equations above to express [tex]h_{2}[/tex] in terms of [tex]h_{1}[/tex], and substitute that into the other equation. For example, from the equation [tex]h_{2}\, A_\text{R} = h_{1}\, A_\text{L}[/tex]:

[tex]\displaystyle h_{2} = \left(\frac{A_{\text{L}}}{A_{\text{R}}}\right)\, h_{1}[/tex].

Substitute this expression for [tex]h_{2}[/tex] into the other equation and solve for [tex]h_{1}[/tex]:

[tex]\displaystyle h_{1} + \left(\frac{A_{\text{L}}}{A_{\text{R}}}\right)\, h_{1} = \frac{\rho_{\text{B}}\, L}{\rho_{\text{A}}}[/tex].

[tex]\displaystyle \left(1 + \frac{A_{\text{L}}}{A_{\text{R}}}\right)\, h_{1} = \frac{\rho_{\text{B}}\, L}{\rho_{\text{A}}}[/tex].

[tex]\begin{aligned} h_{1} &= \left(\frac{\rho_{\text{B}}\, L}{\rho_{\text{A}}}\right)\, \left(\frac{A_{\text{R}}}{A_{\text{L}} + A_{\text{R}}}\right) \\ &\approx \frac{(1.3)\, (19.0934)}{(11)}\, \frac{(3.92)}{(8.5) + (3.92)} \\ &\approx 0.712\; \text{cm} \end{aligned}[/tex].

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