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PAGE 1/13
General Physics Laboratory – Experiment Report
2nd Semester, Year 2016
Exp. #2-1 : Measurement of the Electrostatic Constant and the Electric Permittivity in Vacuum
by Using a Torsion Balance and Understanding of Coulomb's Law
Student ID
Major
Name
Team #
Experiment Lecturer
Student's
Mentioned
Items
Experiment Class Date
Submission Time
Submission Place
Introductory Physics Office
Report Box #
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Lecturer's
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keep
one’s
Experiment
Reports
completed
evaluation
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Experiment Lecturers until the grade decision of General Physics
Laboratory.
▶ If a student is absent from the Experiment Class because of proper
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Last Update : 2016-08-30
PAGE 2/13
General Physics Laboratory – Experiment Report
2nd Semester, Year 2016
1. Objective
In this experiment, the electrostatic constant and the electric permittivity in vacuum will be measured by using a torsion balance. In addition, Coulomb's law
will be quantitatively understood.
2. Theory
(1) Coulomb's law
ions exist between separated charges, these objects move quickly to
decrease the electric field produced by separated charges. Therefore, it is
Charges with the same sign repel each other, and charges with the
only possible to keep relatively small amount of charges separated in the
opposite sign attract each other. The magnitude  of the electrostatic
laboratory. In this reason, despite that the electrostatic force is extremely
force or Coulomb force applied between two point charges  and 
larger than the gravitational force, the measurement of the electrostatic
separated by a distance  is given as the following.
force needs a delicate torsion balance whereas the measurement of the
gravitational force can be done by a simple spring balance. The torsion
balance will provide a direct and precise method in measuring the
electrostatic force.
If the electrostatic force is inversely proportional to the square of the
distance between two objects, it can be shown mathematically that the
electric field is zero at all points inside the homogeneously charged
conductive sphere. It is well known that this fact is correct based on the
  
   
 
  
  

measurement with a considerable precision done on the electric field inside
(Eq. 1)
a charged conductive sphere. If the electrostatic force is expressed as
Fig. 1. Electrostatic force applied between two point charges.
Here,

     ×  N⋅m  C 
 
 
  
,


   ×  
is
obtained
from
such
an
indirect
measurement method.
is
called
the
electrostatic
constant or Coulomb constant in vacuum, and     ×   Fm is
called the electric permittivity in vacuum where F  C  N⋅m is the SI
※ Answer the following questions.
unit of capacitance. The electrostatic force is inversely proportional to the
1. If protons with a mass  g and electrons with a mass  g are
square of the distance between two objects, similar to the gravitational
separated by a distance  m , show that the electrostatic force of
force.
about  ×  N is applied between two.
(2) Torsion balance
(3) Restoring torque and torsion constant
If protons with a mass of  g and electrons with a mass of  g are
separated by a distance of  m , the electrostatic force of about
If the restoring torque applied in a torsion balance is  and the twist
 ×  N is applied between two. This force corresponds to the
angle of a torsion wire from the zero point is  , there is a

gravitational force applied to an object with a mass of about  of the

proportionality relation between them when they are sufficiently small so
Moon on the surface of the Earth. Since an extremely great force is
applied between charges with small quantities, it could seem that a delicate
torsion balance will not be needed to measure the electrostatic force
applied between charged objects in the laboratory.
In general, it is difficult to keep charges separated, because the magnitude
of the electrostatic force is very large and the size of a proton and an
that the relation between them can be expressed as follows:
   (Eq. 2)
 × 
Here,  is called the torsion constant. If the torque is given by 

 is  , the magnitude of the torque is
and the angle between  and 
   . Here,  is the distance between the rotation axis and the action
point of the force, and  is the magnitude of the force. Therefore, the
easily mobile electron is very small. Negatively charged electrons repel each

relation of    and    is made so that the torsion constant

other and attract positively charged protons. In addition, if free electrons or
can be measured by using this relation.
Introductory Physics Office, Department of Physics, College of Science, Korea University
Last Update : 2016-08-30
PAGE 3/13
General Physics Laboratory – Experiment Report
2nd Semester, Year 2016
(4) Capacitance of a conductive sphere
Consider a capacitor consisting of two conductive spheres with the same
centers and radii  and  (  ).
Fig. 2. A capacitor consisting of two conductive spheres with the same
centers.
One conductive sphere is charged by   and the other is charged by
 . If the potential difference between two conductive spheres is  , the
capacitance of this capacitor is given by
 
  
     . (Eq. 3)
 
 


 

If there is one conductive sphere with a radius , the radius of the other
is treated as →∞ . Therefore, the capacitance of an isolated conductive
sphere with a radius  is given by
    . (Eq. 4)
Since the relation between the charge  and the potential difference  in
a capacitor is    , the charge of a conductive sphere can be
measured by using this relation.
(5) Corrected twist angle
Since the electrostatic force is applied between two conductive spheres
located relatively close in this experiment, a conductive sphere cannot be
treated the same way as a point charge. In this reason, the twist angle

 can be substituted with the corrected twist angle     . Here,

the correction factor  is given by


    
, (Eq. 4)

where  is the radius of a conductive sphere and  is the distance
between the centers of two conductive spheres.
Introductory Physics Office, Department of Physics, College of Science, Korea University
Last Update : 2016-08-30
PAGE 4/13
General Physics Laboratory – Experiment Report
2nd Semester, Year 2016
3. Experimental Instruments
Items
Quantity
Torsion balance
1 set
Support tube
1 ea.
Mass
3 ea.
Usage
It is used to measure the electrostatic force.
Clean up method
It should be placed at the center of
the experiment table.
It is used to support the conductive sphere of the torsion
It should be mounted on the torsion
balance when measuring the torsion constant.
balance.
Two  mg masses and one  mg mass are placed on the
conductive sphere of the torsion balance when measuring the
torsion constant.
Slide assembly
1 set
It is used to fix one of the conductive spheres.
Conductive sphere
2 ea.
Electrostatic force is applied between two conductive spheres.
They should be placed inside the
tool box of the torsion balance.
It should be placed at the center of
the experiment table.
They should be attached to the
torsion
balance
and
the
slide
assembly, respectively.
High voltage supply
1 ea.
High voltage supply
-to-wall power
1 ea.
connection cable
Charging probe
1 ea.
It is used to produce high voltage.
It should be placed at the center of
the experiment table.
It is used to connect the high voltage supply to the wall
It should be placed inside the basket
power.
of the experiment table.
It is used to charge two conductive spheres.
Introductory Physics Office, Department of Physics, College of Science, Korea University
It should be placed inside the basket
of the experiment table.
Last Update : 2016-08-30
PAGE 5/13
General Physics Laboratory – Experiment Report
2nd Semester, Year 2016
4. Experimental Procedures
(1) Measurement of the torsion constant
1) After pushing the support bar of the torsion balance outside the torsion
balance, turn the torsion balance to its side. When turning the torsion
balance, prevent the conductive sphere of the torsion balance from hitting
on the floor violently. Set the torsion balance to the zero point by rotating
the dial of the torsion balance until the index lines of the torsion balance
are aligned, and write down the angle   of the torsion balance at the
zero point. Compared to the torsion wire used in the measurement of the
gravitation constant, the torsion wire used in the measurement of the
electrostatic constant is very endurable. However, note that the torsion wire
of the torsion balance may be damaged if the dial of the torsion balance
is rotated extremely quickly or continues to rotate in only one direction. If
the torsion wire of the torsion balance is too loose or damaged, inquire of
Experiment Lecturer.
3) Change the value of a mass  to      mg, and repeat
the experimental procedures. The increase of  causes the increase of  ,
but the decrease of  can be observed when passing through    . If
the dial of the torsion balance undergoes one complete rotation, add
  to the angle  . In the same manner, if the dial of the torsion
balance undergoes two complete rotations, add    to the angle  .
4) By using a proper program, draw the torque    due to the weight
2) Take out a mass from the tool box of the torsion balance and write
of a mass vs. the twist angle       graph. If the distance 
down the value  of a mass which will be placed on the conductive
between the rotation axis of the torsion wire and the center of the
sphere of the torsion balance. Note that it is very easy to lose a mass
conductive sphere of the torsion balance is known, the torsion constant 
because of the small size. When placing a mass on the conductive sphere
of the torsion wire can be calculated from the slope of the graph.
of the torsion balance, the torque due to the weight    of a mass
makes the conductive sphere of the torsion balance go down so that the
increase of the restoring torque of the torsion wire is needed for restoring
the torsion balance to the zero point. First, place a support tube under the
conductive sphere of the torsion balance, and place a mass on the
conductive sphere of the torsion balance which will be stopped by the
support tube. And then, rotate the dial of the torsion balance slowly to lift
the conductive sphere of the torsion balance slightly above the zero point
(2) Measurement of the electrostatic force vs. the distance
1) After pushing the support bar of the torsion balance back inside the
torsion balance, place the torsion balance upright and connect the slide
assembly to the torsion balance. In order to use the scale of the slide
assembly, force the conductive sphere of the torsion balance to stop at the
zero point, and slide the conductive sphere of the slide assembly so that it
contacts with the conductive sphere of the torsion balance. Since the radii
and remove a support tube. Finally, rotate the dial of the torsion balance
 of two conductive spheres are   cm respectively, control the position
back again to set the torsion balance to the zero point and write down
of the conductive sphere of the slide assembly to make the distance 
the angle  of the torsion balance.
between the centers of two conductive spheres be   cm .
Introductory Physics Office, Department of Physics, College of Science, Korea University
Last Update : 2016-08-30
PAGE 6/13
General Physics Laboratory – Experiment Report
2nd Semester, Year 2016
2) After completing the procedures for using the scale of the slide
in the high voltage supply. For example, if the voltage displayed in high
assembly, move two conductive spheres far away. Set the torsion balance
voltage supply is   kV , it is the voltage between   terminal and
to the zero point by rotating the dial of the torsion balance until the index
  terminal of the high voltage supply so that the actual voltage
lines of torsion balance are aligned, and write down the angle   of the
charging two conductive spheres is   kV which is the voltage between
torsion balance at the zero point.
the ground terminal and   or   terminal of the high voltage supply.
3) After confirming that the high voltage supply is off, use a high voltage
supply-to-wall power connection cable to connect the high voltage supply
to the wall power and keep the high voltage supply off. Connect a
charging probe to the right or left terminal of the high voltage supply. Do
not connect the charging probe to the middle terminal of the high voltage
supply which is the ground terminal. After confirming that the voltage
adjust knob of the high voltage supply is set to the minimum, turn on the
high voltage supply.
4) Rotate the voltage adjust knob of the high voltage supply to  kV .
6) Slide the conductive sphere of the slide assembly so that two
The high voltage supply used in this experiment is a high voltage & low
conductive spheres are close, and measure the distance  between the
current instrument which makes it not dangerous, but correct manipulation
centers of two conductive spheres by using the scale of the slide assembly.
should be done to avoid any electricity accident.
When two conductive spheres are close, the torque due to the electrostatic
repulsion applied between two conductive spheres makes the conductive
5) By briefly contacting the charging probe with the conductive sphere of
the torsion balance, the conductive sphere of the torsion balance will have
a charge of  . In the same manner, by briefly contacting the charging
probe with the conductive sphere of the slide assembly, the conductive
sphere of the slide assembly will have a charge of  . In principle, the
amount of charges placed on two conductive spheres is independent of
sphere of the torsion balance shift so that it is needed to increase the
restoring torque of the torsion wire for restoring the torsion balance to the
zero point. Rotate the dial of the torsion balance slowly to restore the
torsion balance to the zero point, and write down the angle  of the
torsion balance. If the torsion constant  of the torsion wire, the corrected
the time they contact with the charging probe, if this time is sufficiently

twist angle    
    
long. If the capacitance      of a conductive sphere obtained from
      , and the distance  between the rotation axis of the torsion
the radius  of a conductive sphere and the voltage  charging two
wire and the center of the conductive sphere of the torsion balance are
conductive spheres are known, then the charges  and  placed on two
obtained from the twist angle
conductive spheres can be calculated. Note that the actual voltage 
 
known, the magnitude    of the electrostatic force can be

charging two conductive spheres is the half of the voltage   displayed
calculated.
Introductory Physics Office, Department of Physics, College of Science, Korea University
Last Update : 2016-08-30
PAGE 7/13
General Physics Laboratory – Experiment Report
2nd Semester, Year 2016
7) While rotating the dial of the torsion balance, two conductive spheres
are frequently discharged and the force between two conductive spheres

constant    and the electric permittivity   in vacuum from the
 
becomes attractive or zero. If the conductive sphere of the slide assembly
slope of the graph and compare them to the reference values.
is discharged, it can be simply solved by keeping contact between the
charging probe and the conductive sphere of the slide assembly. On the
contrary, if the conductive sphere of the torsion balance is discharged, it is
※ Answer the following questions.
impossible to keep contact between the charging probe and the conductive
sphere of the torsion balance. Therefore, it is necessary to contact the
2. Explain why the attractive force is applied between charged and
charging probe with the conductive sphere of the torsion balance each
uncharged conductive spheres.
time the conductive sphere of the torsion balance seems to be discharged.
Since the discharging time depends on the humidity of the laboratory, the
operation of the air conditioner in the laboratory gives better experimental
results. However, the torsion balance is sensitive to the air flow so that the
direction of the air flow coming from the air conditioner should be
controlled.
8) While keeping the voltage  displayed in the high voltage supply
constant as  kV , change the distance  between the centers of two
conductive spheres to         cm and
repeat the experimental procedures.
9) By using a proper program, draw the magnitude  of the electrostatic

graph and confirm the proportionality relation between two
force vs. 

quantities.
(3) Measurement of the electrostatic force vs. the charge
1) While keeping the distance  between the centers of two conductive
spheres constant as  cm and  cm respectively, change the voltage
 displayed in the high voltage supply to     kV and
repeat the experimental procedures.
2) By using a proper program, draw the magnitude  of the electrostatic
force vs.   graph and confirm the proportionality relation between two
quantities.
3) If all the measurements are finished, confirm that the voltage adjust
knob of the high voltage supply is set to the minimum and turn off the
high voltage supply. Finally, clean up the experimental instruments
according to the suggested method.
(4) Calculation of the electrostatic constant and the electric permittivity in
vacuum
From the former experimental results, complete the table of the magnitude
 
. By using a proper program, draw
 of the electrostatic force vs. 


 
graph and confirm
the magnitude  of the electrostatic force vs. 

the proportionality relation between two quantities. Find the electrostatic
Introductory Physics Office, Department of Physics, College of Science, Korea University
Last Update : 2016-08-30
PAGE 8/13
General Physics Laboratory – Experiment Report
2nd Semester, Year 2016
5. Experimental Values
(1) Measurement of the torsion constant
Gravitational acceleration  (ms )

Distance  between the rotation axis of the torsion wire and the center of the conductive sphere of the torsion balance
(cm )

Angle   of the torsion balance at the zero point (deg)
Value 
Weight   
of a mass
of a mass
(mg    kg)
(N )
Torque   
due to the
weight of a mass
(N⋅m )
Angle  of the
Twist angle
torsion balance
     
(deg)
(deg)





Slope
Introductory Physics Office, Department of Physics, College of Science, Korea University

N⋅mdeg
-intercept
deg
-intercept
N⋅m
Last Update : 2016-08-30
PAGE 9/13
General Physics Laboratory – Experiment Report
2nd Semester, Year 2016
(2) Measurement of the electrostatic force vs. the distance
Radius  of the conductive sphere (cm )

Capacitance      of the conductive sphere (F ) [Use     ×   Fm .]
Angle   of the torsion balance at the zero point (deg)
Torsion constant  of the torsion wire (N⋅mdeg)
Distance  between the rotation axis of the torsion wire and the center of the conductive sphere of the torsion balance

(cm )
Voltage 
displayed in the
high voltage
supply
(kV )
Charges
Distance 
    
between the
placed on two centers of two
conductive
conductive
spheres
spheres
(C )
(cm )
Corrected



(m

)
Magnitude
 
Correction factor Angle  of the
Twist angle
twist angle
torsion balance
     
 

(deg)
(deg)

   

of the


   

(deg)
electrostatic force
(N )









※ Note that the actual voltage  charging two conductive spheres is the half of the voltage  displayed in the high voltage supply.
Slope
Introductory Physics Office, Department of Physics, College of Science, Korea University
N⋅m 
-intercept
m 
-intercept
N
Last Update : 2016-08-30
PAGE 10/13
General Physics Laboratory – Experiment Report
2nd Semester, Year 2016
(3) Measurement of the electrostatic force vs. the charge
Radius  of the conductive sphere (cm )

Capacitance      of the conductive sphere (F ) [Use     ×   Fm .]
Angle   of the torsion balance at the zero point (deg)
Torsion constant  of the torsion wire (N⋅mdeg)
Distance  between the rotation axis of the torsion wire and the center of the conductive sphere of the torsion balance

(cm )
Voltage 
displayed in the
high voltage
supply
(kV )
Charges
Distance 
    
between the
placed on two centers of two
conductive
conductive
spheres
spheres
(C )
(cm )
Magnitude
Corrected
 
(C  )
 
Correction factor Angle  of the
Twist angle
twist angle
torsion balance
     
 

(deg)
(deg)

   

of the


   

(deg)
electrostatic force
(N )










※ Note that the actual voltage  charging two conductive spheres is the half of the voltage  displayed in the high voltage supply.
※ If the former experimental setup continues, the experimental values for    kV are the same as the former experimental values.
   cm
Slope
Introductory Physics Office, Department of Physics, College of Science, Korea University
   cm
NC 
NC 
-intercept
C
C
-intercept
N
N
Last Update : 2016-08-30
PAGE 11/13
General Physics Laboratory – Experiment Report
2nd Semester, Year 2016
(4) Calculation of the electrostatic constant and the electric permittivity in vacuum
Measurement
Voltage 
Charges   
Distance  between
displayed in the
placed on
the centers of
high voltage supply
two conductive spheres
two conductive spheres
(kV )
(C )
(cm )
 


(C  m  )
Magnitude 
of the
electrostatic force
(N )


Measurement

of the
electrostatic force


vs.

the distance




Measurement

of the

electrostatic force
vs.

the charge




Slope
N⋅m  C 

-intercept
C  m 
-intercept
N
Electrostatic constant
in vacuum

 
 
Reference value
Experimental value
Error
(N⋅m C )
(N⋅m C )
(%)
Electric permittivity
in vacuum

  

Reference value
Experimental value
Error
(Fm )
(Fm )
(%)




 × 
 × 
 
Introductory Physics Office, Department of Physics, College of Science, Korea University
Last Update : 2016-08-30
PAGE 12/13
General Physics Laboratory – Experiment Report
2nd Semester, Year 2016
6. Results and Discussions (This page should be used as the first page of the corresponding section. If the contents exceed this page, additional contents
should be written by attaching papers. Contents should be written by hand, and not by a word processor. Attaching copied figures and tables to the report
is allowed.)
Introductory Physics Office, Department of Physics, College of Science, Korea University
Last Update : 2016-08-30
PAGE 13/13
General Physics Laboratory – Experiment Report
2nd Semester, Year 2016
7. Solution of Problems (This page should be used as the first page of the corresponding section. If the contents exceed this page, additional contents
should be written by attaching papers. Contents should be written by hand, and not by a word processor. Attaching copied figures and tables to the report
is allowed.)
8. Reference
Introductory Physics Office, Department of Physics, College of Science, Korea University
Last Update : 2016-08-30