Question #204584

1. Density. A piece of copper whose density is 8.93 g/cm3 has a mass of 180 g in air and 162 g when submerged in a certain liquid. What is the mass density (in g/cm3) of the liquid?

2. Gauge Pressure. At what depth (in meters) in seawater is the gauge pressure 1.00 x 105 Pa? (density of seawater= 1025/kg/m3)

3. Pascal’s Principle. In a hydraulic press the small cylinder has a diameter of 8.00 cm, while the large piston has a diameter of 20.0 cm. If a force of 500 N is applied to the small piston, what is the force on the large piston, neglecting friction? 


1
Expert's answer
2021-06-09T08:05:51-0400

(1) The apparent weight of the piece of copper when it placed in the liquid can be written as follows:


WA=WFB.W_A=W-F_B.

Then, we can find the buoyant force acting on the piece of copper:


FB=WWA=mairgmliquidg=(mairmliquid)g,F_B=W-W_A=m_{air}g-m_{liquid}g=(m_{air}-m_{liquid})g,FB=(0.18 kg0.162 kg)9.8 ms2=0.1764 N.F_B=(0.18\ kg-0.162\ kg)\cdot9.8\ \dfrac{m}{s^2}=0.1764\ N.

Let's find the volume of the piece of copper:


V=mρ=0.18 kg8930 kgm3=2.01105 m3.V=\dfrac{m}{\rho}=\dfrac{0.18\ kg}{8930\ \dfrac{kg}{m^3}}=2.01\cdot10^{-5}\ m^3.

By the definition of the buoyant force we have:


FB=ρliquidVliquidg=ρliquidVg,F_B=\rho_{liquid}V_{liquid}g=\rho_{liquid}Vg,ρliquid=FBVg,\rho_{liquid}=\dfrac{F_B}{Vg},ρliquid=0.1764 N2.01105 m39.8 ms2=895 kgm3=0.895 gcm3.\rho_{liquid}=\dfrac{0.1764\ N}{2.01\cdot10^{-5}\ m^3\cdot9.8\ \dfrac{m}{s^2}}=895\ \dfrac{kg}{m^3}=0.895\ \dfrac{g}{cm^3}.

(2) By the definition of the gauge pressure we have:


Pgauge=PabsPatm=ρseawatergh,P_{gauge}=P_{abs}-P_{atm}=\rho_{seawater}gh,h=Pgaugeρseawaterg=1.0105 Pa1025 kgm39.8 ms2=9.9 m.h=\dfrac{P_{gauge}}{\rho_{seawater}g}=\dfrac{1.0\cdot10^5\ Pa}{1025\ \dfrac{kg}{m^3}\cdot9.8\ \dfrac{m}{s^2}}=9.9\ m.

(3)

F1A1=F2A2,\dfrac{F_1}{A_1}=\dfrac{F_2}{A_2},F2=F1A2A1=F1πr22πr12,F_2=F_1\dfrac{A_2}{A_1}=F_1\dfrac{\pi r_2^2}{\pi r_1^2},F2=500 Nπ(0.1 m)2π(0.04 m)2=3125 N.F_2=500\ N\cdot\dfrac{\pi(0.1\ m)^2}{\pi(0.04\ m)^2}=3125\ N.

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