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CHAPTER 2 : DC METER
2.1.1 PMMC

 The  Permanent Magnet Moving Coil (PMMC)
  galvanometer used for dc measurement only.
 The motor action is produced by the flow of a
  small current throught a moving coil which is
  positioned in the field of a permanent magnet
 The basic moving coil system-D’Arsonval
  galvonometer
Figure 2.1: d’Arsonval meter
2.1.3 Deflecting Torque

 Resulting from the effects of magnetic
  electrostatic.
 This torque causes the pointer moves from
  the zero position
                  F
                          IRON CORE

       N              S


              F
DEFLECTING TORQUE

            Td = BANI (Nm)
B = flux density in Wb/m2 or Tesla (T)
N = number of coils
A = Area cross-section
    (length (l) x coil diameter (d)m2 )
I = current flowing through the coil - Ampere
2.1.4 DAMPING CURVE

 Works  to speed up the pointer stops
 Pointer may oscillate before the show
  reading and damping torque required to
  accelerate the needle stops.
Damping curve

               V
                   Under damp

                            Critical damp

  Steady
  state

                            Over damp


                                            t
           0
2.1.5 Damping Curve
   Over damp – pointer will move slowly and never
    reach the steady state. The value will be less than
    the actual value.

   Under damp - pointer will oscillate until it finally reach
    the final value. The result is difficult to read.

   Critical damp - pointer to achieve the true value of
    free oscillations in a short time.
2.1.6 Types of damping

Eddy   current damping
Air friction damping
Fluid damping
EDDY CURRENT DAMPING

   An aluminum disc D, is controlled by a reel, can be
    move between a the pole of a permanent magnet M.
   If the disk moves clockwise, the e.m.f induced in the
    disc circulate eddy currents distribution as shown
    (interrupted lines). From Lenz Law, the current will
    impose a force against the movement of their forms.
    Therefore, the resulting damping force is counter
    clockwise.

                                    M
                          D
Air friction Damping

A piece of the blade is attached to the
 moving parts in the meter. Resistance
 produced by the air around will give the
 desired damping.
Fluid damping

 The same principle is used but the blade is
 allowed to move in a container of liquid with
 suitable viscosity.
2.2 DC VOLTMETER

 The basic d’Arsonval meter can be converted
 to a dc voltmeter by connecting a multiplier
 Rs in series with it as shown in Figure 2.6.
 The purpose of the multiplier is to extend the
 range of the meter and to limit the current
 through the d’Arsonval meter to the
 maximum full-scale deflection current.
2.2.1 Basic DC Voltmeter circuit




                                                     Figure 2.6

To find the value of the multiplier resistor, we may first determine
the sensitivity, S, of the d’Arsonval. If the sensitivity is known, the
total voltmeter resistance can be calculated easily.
The sensitivity of a voltmeter is always specified by the
manufacturer, and is frequently printed on the scale of the
instrument.
Voltmeter

•   If the full-scale meter current is known, the
    sensitivity can be determined as the
    reciprocal of the full scale current.

              Sensitivity = 1 / Ifs

 Where     Ifs is the full-scale deflection current
    of d’Arsonval meter.
2.2.2 Multiplier Resistance

 Thevalue of the multiplier resistance can be
 found using this relationship:

          Rs + Rm = S x Vrange
 Thus,

          Rs = (S x Vrange) - Rm
2.2.3 Example

 Calculate the value of the multiplier
  resistance on the 50 V range of a dc
  voltmeter that used a 500μA d’Arsonval
  meter with an internal resistance of 1 kΩ.
Solution :

   S    = 1/Ifs
         = 1/500µA = 2KΩ/V

    Rs   = S x Range – Rm
         = 2 kΩ/V x 50 V – 1 kΩ
         = 99 kΩ
2.2.4 Multi range Voltmeter
   A multi range voltmeter consists of a deflection instrument,
    several multiplier resistors and a rotary switch. Two possible
    circuits are illustrated in Figure 2.7 (a) and (b).




               Figure 2.7(a): Multirange Voltmeter
 Infigure 2.7 (a) only one of the three
  multiplier resistors is connected in series with
  the meter at any time. The range of this
  meter is
             V = Im ( R + Rm )

 Where  the multiplier resistance, R can be R1
  or R2 or R3.
Figure 2.7(b): A commercial version of a multi range voltmeter
   In figure 2.7(b) the multiplier resistors are connected
    in series, and each junction is connected to one of
    the switch terminals. The range of this voltmeter can
    be also calculated from the equation

                      V = Im (Rm + R)

   Where the multiplier, R, now can be R3 or (R3 + R2)
    or (R1 + R2 + R3)
    (Note: the largest voltage range must be associated
    with the largest sum of the multiplier resistance)
2.2.5 Example

 Calculate    the value of the multiplier
  resistance for the multiple range dc voltmeter
  circuit shown in Figure 2.7(a) and Figure
  2.7(b), if Ifs = 50μA and Rm = 1kΩ
2.2.6
2.2.7
DC Voltmeter Loading Effect


 Asthe DC ammeter, the DC voltmeter also
 observe for loading effect whenever it is
 inserted to a measured circuit. Figure 2.7
 shows a circuit with the DC voltmeter is
 inserted into it. Inserting voltmeter always
 increase the resistance and decrease the
 current flowing through the circuit.
Figure 2.7: Circuit with voltmeter insertion effect
 Withoutthe insertion of the DC voltmeter, the
 voltage VRB can be found as:

             RB
     VRB = _______ X E
           RB + RA
2.2.8 LOADING EFFECT


 Inserting the voltmeter in parallel with RB
  gives us the total inserted resistance as :
            RT = RS + RM

 Thus,   yield to
              Req = RB //RT
m
 Now, the voltage VRB with the voltmeter
 insertion is found as:

              Req
     VRB = ________ x E
            Req + RA
 Therefore,
                            m
  Insertion error = VRB – VRB X 100%
                     VRB
DC Voltmeter
Example 1.
 Calculate the value of the multiplier Rs on
  the 50-V range of a DC Voltmeter that used
  200-µA meter movements with an internal
  resistance of 1.2kΩ.
DC Voltmeter
Example 2.
 Calculate the
  values of Rs for
  the multiple-
  range DC
  Voltmeter
  circuits as
  shown below:
DC Voltmeter
Example 3.
 Calculate the
  values of Rs for
  the multiple-
  range DC
  Voltmeter
  circuits as
  shown below:
Voltmeter Loading Effects
 When a voltmeter is used to measure the
  voltage across a circuit component, the
  voltmeter circuit itself is in parallel with the
  circuit component.
 Since the parallel combination of two
  resistors is less than either resistor alone,
  the resistor seen by the source is less with
  the voltmeter connector than without.
Voltmeter Loading Effects
 Therefore, the voltage across the
  component is less whenever the
  voltmeter is connected.
 The decrease in voltage maybe negligible
  or appreciable, depending on the
  Sensitivity of the voltmeter being used.
 This effect is called voltmeter loading
  and the resulting error is called
  loading error.
Voltmeter Loading Effects
Example 5:
 Two different voltmeters are used
  to measure the voltage across RB in
  the circuit below. The meters are:
   Meter A : S= 1kΩ/V;Rm=0.2kΩ; Range =10V
   Meter B : S=20kΩ/V;Rm=2.2kΩ; Range = 10V

   Calculate:
    Voltage across   RB without any meter.
    Voltage across   RB when meter A is
      used.
    Voltage across   RB when meter B is
      used.
    Loading Errors   in both voltmeter
      readings.
Voltmeter Loading Effects
Example 6:
 Find the voltage reading and the
   percentage of loading error of
   each reading obtained with a
   voltmeter on:
    Its 5-V range.
    Its 10-V range
    Its 50-V range.
   The meter has a 20-kΩ/V
      sensitivity and connected
      across RA.

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2 dc meter

  • 1. CHAPTER 2 : DC METER
  • 2. 2.1.1 PMMC  The Permanent Magnet Moving Coil (PMMC) galvanometer used for dc measurement only.  The motor action is produced by the flow of a small current throught a moving coil which is positioned in the field of a permanent magnet  The basic moving coil system-D’Arsonval galvonometer
  • 4. 2.1.3 Deflecting Torque  Resulting from the effects of magnetic electrostatic.  This torque causes the pointer moves from the zero position F IRON CORE N S F
  • 5. DEFLECTING TORQUE Td = BANI (Nm) B = flux density in Wb/m2 or Tesla (T) N = number of coils A = Area cross-section (length (l) x coil diameter (d)m2 ) I = current flowing through the coil - Ampere
  • 6. 2.1.4 DAMPING CURVE  Works to speed up the pointer stops  Pointer may oscillate before the show reading and damping torque required to accelerate the needle stops.
  • 7. Damping curve V Under damp Critical damp Steady state Over damp t 0
  • 8. 2.1.5 Damping Curve  Over damp – pointer will move slowly and never reach the steady state. The value will be less than the actual value.  Under damp - pointer will oscillate until it finally reach the final value. The result is difficult to read.  Critical damp - pointer to achieve the true value of free oscillations in a short time.
  • 9. 2.1.6 Types of damping Eddy current damping Air friction damping Fluid damping
  • 10. EDDY CURRENT DAMPING  An aluminum disc D, is controlled by a reel, can be move between a the pole of a permanent magnet M.  If the disk moves clockwise, the e.m.f induced in the disc circulate eddy currents distribution as shown (interrupted lines). From Lenz Law, the current will impose a force against the movement of their forms. Therefore, the resulting damping force is counter clockwise. M D
  • 11. Air friction Damping A piece of the blade is attached to the moving parts in the meter. Resistance produced by the air around will give the desired damping.
  • 12. Fluid damping  The same principle is used but the blade is allowed to move in a container of liquid with suitable viscosity.
  • 13. 2.2 DC VOLTMETER  The basic d’Arsonval meter can be converted to a dc voltmeter by connecting a multiplier Rs in series with it as shown in Figure 2.6. The purpose of the multiplier is to extend the range of the meter and to limit the current through the d’Arsonval meter to the maximum full-scale deflection current.
  • 14. 2.2.1 Basic DC Voltmeter circuit Figure 2.6 To find the value of the multiplier resistor, we may first determine the sensitivity, S, of the d’Arsonval. If the sensitivity is known, the total voltmeter resistance can be calculated easily. The sensitivity of a voltmeter is always specified by the manufacturer, and is frequently printed on the scale of the instrument.
  • 15. Voltmeter • If the full-scale meter current is known, the sensitivity can be determined as the reciprocal of the full scale current. Sensitivity = 1 / Ifs  Where Ifs is the full-scale deflection current of d’Arsonval meter.
  • 16. 2.2.2 Multiplier Resistance  Thevalue of the multiplier resistance can be found using this relationship: Rs + Rm = S x Vrange  Thus, Rs = (S x Vrange) - Rm
  • 17. 2.2.3 Example  Calculate the value of the multiplier resistance on the 50 V range of a dc voltmeter that used a 500μA d’Arsonval meter with an internal resistance of 1 kΩ.
  • 18. Solution :  S = 1/Ifs = 1/500µA = 2KΩ/V Rs = S x Range – Rm = 2 kΩ/V x 50 V – 1 kΩ = 99 kΩ
  • 19. 2.2.4 Multi range Voltmeter  A multi range voltmeter consists of a deflection instrument, several multiplier resistors and a rotary switch. Two possible circuits are illustrated in Figure 2.7 (a) and (b). Figure 2.7(a): Multirange Voltmeter
  • 20.  Infigure 2.7 (a) only one of the three multiplier resistors is connected in series with the meter at any time. The range of this meter is V = Im ( R + Rm )  Where the multiplier resistance, R can be R1 or R2 or R3.
  • 21. Figure 2.7(b): A commercial version of a multi range voltmeter
  • 22. In figure 2.7(b) the multiplier resistors are connected in series, and each junction is connected to one of the switch terminals. The range of this voltmeter can be also calculated from the equation V = Im (Rm + R)  Where the multiplier, R, now can be R3 or (R3 + R2) or (R1 + R2 + R3) (Note: the largest voltage range must be associated with the largest sum of the multiplier resistance)
  • 23. 2.2.5 Example  Calculate the value of the multiplier resistance for the multiple range dc voltmeter circuit shown in Figure 2.7(a) and Figure 2.7(b), if Ifs = 50μA and Rm = 1kΩ
  • 24. 2.2.6
  • 25. 2.2.7 DC Voltmeter Loading Effect  Asthe DC ammeter, the DC voltmeter also observe for loading effect whenever it is inserted to a measured circuit. Figure 2.7 shows a circuit with the DC voltmeter is inserted into it. Inserting voltmeter always increase the resistance and decrease the current flowing through the circuit.
  • 26. Figure 2.7: Circuit with voltmeter insertion effect
  • 27.  Withoutthe insertion of the DC voltmeter, the voltage VRB can be found as: RB VRB = _______ X E RB + RA
  • 28. 2.2.8 LOADING EFFECT  Inserting the voltmeter in parallel with RB gives us the total inserted resistance as : RT = RS + RM  Thus, yield to Req = RB //RT
  • 29. m  Now, the voltage VRB with the voltmeter insertion is found as: Req VRB = ________ x E Req + RA
  • 30.  Therefore, m Insertion error = VRB – VRB X 100% VRB
  • 31.
  • 32. DC Voltmeter Example 1.  Calculate the value of the multiplier Rs on the 50-V range of a DC Voltmeter that used 200-µA meter movements with an internal resistance of 1.2kΩ.
  • 33. DC Voltmeter Example 2.  Calculate the values of Rs for the multiple- range DC Voltmeter circuits as shown below:
  • 34. DC Voltmeter Example 3.  Calculate the values of Rs for the multiple- range DC Voltmeter circuits as shown below:
  • 35. Voltmeter Loading Effects  When a voltmeter is used to measure the voltage across a circuit component, the voltmeter circuit itself is in parallel with the circuit component.  Since the parallel combination of two resistors is less than either resistor alone, the resistor seen by the source is less with the voltmeter connector than without.
  • 36. Voltmeter Loading Effects  Therefore, the voltage across the component is less whenever the voltmeter is connected.  The decrease in voltage maybe negligible or appreciable, depending on the Sensitivity of the voltmeter being used.  This effect is called voltmeter loading and the resulting error is called loading error.
  • 37. Voltmeter Loading Effects Example 5:  Two different voltmeters are used to measure the voltage across RB in the circuit below. The meters are: Meter A : S= 1kΩ/V;Rm=0.2kΩ; Range =10V Meter B : S=20kΩ/V;Rm=2.2kΩ; Range = 10V Calculate:  Voltage across RB without any meter.  Voltage across RB when meter A is used.  Voltage across RB when meter B is used.  Loading Errors in both voltmeter readings.
  • 38. Voltmeter Loading Effects Example 6:  Find the voltage reading and the percentage of loading error of each reading obtained with a voltmeter on:  Its 5-V range.  Its 10-V range  Its 50-V range. The meter has a 20-kΩ/V sensitivity and connected across RA.