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Nana76 [90]
3 years ago
8

The liquid in the open-tube manometer in Fig. 12.8a is mercury, y1 = 3.00 cm, and y2 = 7.00 cm. Atmospheric pressure is 980 mill

ibars. (a) What is the absolute pressure at the bottom of the U-shaped tube? (b) What is the absolute pressure in the open tube at a depth of 4.00 cm below the free surface? (c) What is the absolute pressure of the gas in the container? (d) What is the gauge pressure of the gas in pascals?

Physics
1 answer:
uysha [10]3 years ago
7 0

Answer:

(a) Absolute pressure at the bottom of the U-shaped tube is: 107339 Pa, (b) The absolute pressure in the open tube at a depth of 4.00 cm below the free surface is: 103337 Pa, (c) The absolute pressure of the gas in the container is: 103337 Pa and (d) The gauge pressure of the gas in pascals is: 5337 Pa.

Explanation:

We need to apply the Pascals' law (P=p*g*h), where P is pressure, p is density, g is the gravity and h the height of the column, to determine the pressure at differents points in the open tube manometer. First we need to know the mercury density as: 13600 (Kg/m^3). Now remember that the absolute pressure is related with manometric pressure and atmospheric pressure like: P_{abs}=P_{gauge}  +P_{atm}, so we can find the absolute pressure at the bottom of the U-shaped as: P_{abs(at the bottom)} = 13600*9.81*0.07+98000=103337(Pa) (a). Using the same equation we can get the absolute pressure in the open tube at a depth of 4.00 cm as: P_{abs(4.00cm)} =13600*9.81*0.04+98000=103337(Pa)(b). Then to get the absolute pressure of the gas in the container we need to use the Pascal's law as:P_{abs(gas)}=13600*9.81*(0.07-0.03)+98000=103337(Pa) (c). Finally to find the gauge pressure of the gas in pascals we solve for Pgauge as:P_{gauge}=P_{abs}  -P_{atm} so replacing the values we get:P_{gauge}=P_{abs(gas)}-P_{atm}=103337-98000=5337(Pa) (d).

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alukav5142 [94]

Answer:

5308.34 N/C

Explanation:

Given:

Surface density of each plate (σ) = 47.0 nC/m² = 47\times 10^{-9}\ C/m^2

Separation between the plates (d) = 2.20 cm

We know, from Gauss law for a thin sheet of plate that, the electric field at a point near the sheet of surface density 'σ' is given as:

E=\dfrac{\sigma}{2\epsilon_0}

Now, as the plates are oppositely charged, so the electric field in the region between the plates will be in same direction and thus their magnitudes gets added up. Therefore,

E_{between}=E+E=2E=\frac{2\sigma}{2\epsilon_0}=\frac{\sigma}{\epsilon_0}

Now, plug in  47\times 10^{-9}\ C/m^2 for 'σ' and 8.85\times 10^{-12}\ F/m for \epsilon_0 and solve for the electric field. This gives,

E_{between}=\frac{47\times 10^{-9}\ C/m^2}{8.854\times 10^{-12}\ F/m}\\\\E_{between}= 5308.34\ N/C

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3 years ago
A basketball is thrown straight up in the air. At its peak, it is 0.02 km high and has a velocity of 0 m/s. What is its final ve
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Answer:

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Explanation:

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distance, d = 3.0 cm = 3.00 \times 10^{-2} \mathrm{m}

We need to calculate the time taken by the transducer to detect the reflected waves from the metal fragment after they were first emitted.

As we know, the velocity is the ratio of distance and the time travelled by an object. The equation form is given by,

              \text {velocity, } v=\frac{\text {distance }(d)}{\text {time}(t)}

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