PHYSICS 231 Lecture 22: Pressure

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PHY 231 1 PHYSICS 231 Lecture 22: Pressure Remco Zegers Walk-in hour: Thursday 11:30-13:30 am Helproom

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PHYSICS 231 Lecture 22: Pressure. Remco Zegers Walk-in hour: Thursday 11:30-13:30 am Helproom. Previously. Young’s modulus. Solids:. Shear modulus. Bulk modulus Also fluids. General:. P=F/A (N/m 2 =Pa) =M/V (kg/m 3 ). Force and pressure. Air (P=1.0E+5 Pa). P=0 Vacuum. A. F. - PowerPoint PPT Presentation

Transcript of PHYSICS 231 Lecture 22: Pressure

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PHYSICS 231Lecture 22: Pressure

Remco ZegersWalk-in hour: Thursday 11:30-13:30 am

Helproom

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PreviouslySolids:

LAFL

LLAFY

0

0// Young’s modulus

xAFh

hxAFS

// Shear modulus

pressurePVVP

VVAFB

00 //

/ Bulk modulusAlso fluids

P=F/A (N/m2=Pa)

=M/V (kg/m3)

General:

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Force and pressure

A P=0Vacuum

Air (P=1.0E+5 Pa)

F

Force due to pressure difference: Fpressure=PAIf A=0.01 m2 (about 10 by 10 cm) thena force F=(1.0E+5)*0.01=1000N is needed to pullthe lit.

What is the force needed to move the lit?

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Magdeburg’s hemispheres

Otto von Guericke (Mayor of Magdeburg, 17th century)

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Pressure vs DepthHorizontal direction:P1=F1/A P2=F2/A F1=F2 (no net force)So, P1=P2

Vertical direction:Ftop=PatmAFbottom=PbottomA-Mg=PbottomA-gAh

Since the column of water is not moving:Ftop-Fbottom=0PatmA=PbottomA-gAhPbottom=Patm+ gh

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Pressure and Depth:

Pdepth=h =Pdepth=0+ gh

Where:Pdepth=h: the pressure at depth hPdepth=0: the pressure at depth 0=density of the liquidg=9.81 m/s2

h=depthPdepth=0=Patmospheric=1.013x105 Pa = 1 atm =760 TorrPascal’s principle: If P0 changes then the pressures at all depths changes with the same value.

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A submarineA submarine is built in such a way that it can stand pressuresof up to 3x106 Pa (approx 30 times the atmospheric pressure). How deep can it go?

Pdepth=h =Pdepth=0+ gh3E+06=(1.0E+05)+(1.0E+03)(9.81)hh=296 m.

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Does the shape of the container matter?

NO!!

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Your homemade pressure difference meter (PART I)

Pdepth=h =Pdepth=0+ gh

Part 2 on Friday!

h1

h2

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Pascal’s principleIn other words then before: a change in pressure applied to a fluid that is enclosed in transmitted to the wholefluid and all the walls of the container that hold the fluid.

P=F1/A1=F2/A2If A2>>A1 thenF2>>F1.

So, if we apply a smallforce F1, we can exerta very large Force F2.

Hydraulic press demo

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Hydraulic brake

6.4cm2 1.8 cm2

F=44N

R=0.34 mcoef offriction: 0.5

What is the frictionaltorque about the axle exerted by the shoe on the wheel drum when a force of 44N is applied to the pedal?

FMC/AMC=FBC/ABCFBC=44*1.8/6.4=12.4 NFshoe-drum=Fdrum-shoe=normal forceFfriction=N=0.5*12.4=6.2N=F*R=6.2*0.34=2.1 NM

n

F

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Pressure measurement.

The open-tube manometer.The pressure at A and B isthe same:P=P0+ghso h=(P-P0)/(g)

If the pressure P=1.01 atm, what is h? (the liquid is water)h=(1.01-1)*(1.0E+05)/(1.0E+03*9.81)= =0.1 m

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Pressure Measurement: the mercury barometer

P0= mercurygh

mercury=13.6E+03 kg/m3

mercury,specific=13.6

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Pressure at different altitudesThe pressure in the lecture room equals 1 atm (1.013E+05 Pa). What will the pressure on the 6th floorof the BPS building be (h=20m)? And at the top ofmount Everest (h=8500 m)?

Just like the case for a fluid, the pressure changeswith depth (height in the case of air).Plecture room=P6th floor+ airghP6th floor=Plecture room-airgh=1.013E+05-1.29*9.81*20=

=1.010+05 Pa ( 3 promille change)Pmount everest=1.013E+05-1.29*9.81*8500=-6.3E+03 Pa????The density of air changes with altitude, and so the equation does not hold; it is very easy to compress air(small bulk modulus) compared to e.g. water.(see also next chapter)