What is the Voltage read on a Real Voltmeter?

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SUMMARY

The discussion focuses on measuring voltage across a voltage-divider network using two different voltmeters, V1 and V2, with specific internal resistances. When V0 is set to 32.4 V, R1 at 205 Ω, and R2 at 465 Ω, the readings on V1 (4.80 k Ω) and V2 (2.75 M Ω) are influenced by their respective internal resistances. The lower the internal resistance of the voltmeter, the more it affects the voltage reading due to loading effects. The calculations reveal that the equivalent resistance and current flow are critical in determining accurate voltage measurements.

PREREQUISITES
  • Understanding of voltage-divider circuits
  • Knowledge of equivalent resistance calculations
  • Familiarity with Kirchhoff's laws
  • Concept of input impedance in measuring instruments
NEXT STEPS
  • Calculate voltage readings using different internal resistances of voltmeters
  • Explore the impact of loading effects on voltage measurements
  • Learn about the concept of input impedance in amplifiers
  • Investigate advanced voltage-divider configurations and their applications
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Electrical engineering students, circuit designers, and anyone involved in voltage measurement and analysis will benefit from this discussion.

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Homework Statement


The output of the voltage-divider network shown in the diagram below is to be measured with two different voltmeters, V1 and V2. Consider the situation when V0 = 32.4 V, R1 = 205 Ω, and R2 = 465 Ω.

a) When the voltmeter V1, whose internal resistance is 4.80 k Ω is placed across R2, what would be the reading on the voltmeter V1?

b) When the voltmeter V2, whose internal resistance is 2.75 M Ω, is placed across R2, what would be the reading on the voltmeter V2?

Homework Equations



1/Req=(1/R1)+(1/R2) where Req= equivalent resistance

Req=R1+R2

V=IR


The Attempt at a Solution


I really do not know where to start with this problem. I originally found the equivalent resistance using the resistors in parallel equation and used that resistance to calculate the voltage that was running through that resistor. Using Kirchoff's Rule that the equation for the circuit was V-R1*I-Req*I=0 where Req in this case is the equivalent resistance of the voltmeter and R2. I guess am having trouble understanding what the voltmeter actually does to the circuit.
 

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tomrja said:

Homework Statement


The output of the voltage-divider network shown in the diagram below is to be measured with two different voltmeters, V1 and V2. Consider the situation when V0 = 32.4 V, R1 = 205 Ω, and R2 = 465 Ω.

a) When the voltmeter V1, whose internal resistance is 4.80 k Ω is placed across R2, what would be the reading on the voltmeter V1?

b) When the voltmeter V2, whose internal resistance is 2.75 M Ω, is placed across R2, what would be the reading on the voltmeter V2?

Homework Equations



1/Req=(1/R1)+(1/R2) where Req= equivalent resistance

Req=R1+R2

V=IR


The Attempt at a Solution


I really do not know where to start with this problem. I originally found the equivalent resistance using the resistors in parallel equation and used that resistance to calculate the voltage that was running through that resistor. Using Kirchoff's Rule that the equation for the circuit was V-R1*I-Req*I=0 where Req in this case is the equivalent resistance of the voltmeter and R2. I guess am having trouble understanding what the voltmeter actually does to the circuit.

The voltmeter presents an equivalent parallel output resistance to the circuit. So the lower the output resistance of the voltmeter (bad), the more it pulls down the voltage being measured in the middle of the voltage divider.

What voltage did you get for the two different cases of the parallel voltmeter output impedance? That's pretty much your answer.

Model the voltmeter as an infinite input impedanc amplifer (that measures the voltage), in parallel with its output resistance. The output resistance "loads" the circuit being measured. So the higher the output resistance of the meter, the more accurate the reading will be (the closer to the unloaded circuit).

Make sense?
 
berkeman said:
The voltmeter presents an equivalent parallel output resistance to the circuit. So the lower the output resistance of the voltmeter (bad), the more it pulls down the voltage being measured in the middle of the voltage divider.

What voltage did you get for the two different cases of the parallel voltmeter output impedance? That's pretty much your answer.

Model the voltmeter as an infinite input impedanc amplifer (that measures the voltage), in parallel with its output resistance. The output resistance "loads" the circuit being measured. So the higher the output resistance of the meter, the more accurate the reading will be (the closer to the unloaded circuit).

Make sense?

The part about how the higher resistance of the voltmeter makes sense because the inverse property of adding resistors in parallel.

Here are the numbers that I worked out. Maybe you can tell me where I went wrong.

I first found the equivalent resistance of the voltmeter and both resistors and found that to be 628.9316ohms. Then I calculated the current flowing through the circuit using I=V/R=(32.4V)/(628.9316ohms)=0.0515159A. Then, using that current I used V=IR once again but this time I used the resistance between the voltmeter and R2 and got V=(0.0515159A)(423.9316ohm)=21.84V. Wait... haha I got it! I guess it just took you explaining a little for me to figure it out. Thanks!
 
Nice when that happens!
 

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