A beginning RC circuit that resembles a wheatstone bridge

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Discussion Overview

The discussion centers around a modified Wheatstone bridge circuit where resistors are replaced with capacitors and a switch. Participants explore how to determine the potential difference between two points in the circuit under different conditions, including AC and DC supplies.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • One participant describes the configuration of the modified Wheatstone bridge and asks how to find the potential between R3 and R4.
  • Another participant suggests using an AC supply and vector subtraction of voltages across capacitors to find the unknown capacitance when one is variable.
  • A later reply clarifies that the capacitors and resistors are not variable or equal, and the current is DC from a battery, prompting a reevaluation of the approach to find the potential difference.
  • One participant proposes a method involving drawing a right-angled triangle to calculate voltages across capacitors and resistors, providing specific values and calculations for a hypothetical scenario.
  • Another participant introduces the idea of finding a differential equation for voltage as a function of time, suggesting the use of Laplace transforms and nodal analysis to derive the voltage function.
  • It is noted that with the switch closed and a DC supply, the capacitors behave like open circuits, resulting in no current through the resistors and zero voltage across them.

Areas of Agreement / Disagreement

Participants express differing views on how to approach the problem, particularly regarding the conditions of the circuit (AC vs. DC) and the behavior of the components. No consensus is reached on a single method to determine the potential difference.

Contextual Notes

Some assumptions regarding the circuit configuration and component values are not explicitly stated, and the discussion includes various approaches that may depend on specific conditions or definitions.

Who May Find This Useful

Readers interested in circuit analysis, particularly those exploring the behavior of capacitors in modified bridge circuits under different electrical conditions.

orthovector
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Everybody knows what a wheatstone bridge looks like. R1 and R2 are on top and R3 and R4 are on bottom and R5 is in the middle of the angled box shape.

let's replace R1 and R2 with 2 different capacitors. Let's also replace R5 with a switch.

How would you figure out the potential between R3 and R4?
 
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Assuming you have an AC supply, you work out the voltage across each capacitor by considering each C/R series circuit and then you subtract the voltages vectorially.

If one of the capacitors was variable and known (and R3 = R4 ), you could adjust it until the bridge was balanced (using an AC detector like an oscilloscope) and then the two capacitors would be equal and you would know the unknown one. You would then have a capacitance bridge.
 
vk6kro said:
Assuming you have an AC supply, you work out the voltage across each capacitor by considering each C/R series circuit and then you subtract the voltages vectorially.

If one of the capacitors was variable and known (and R3 = R4 ), you could adjust it until the bridge was balanced (using an AC detector like an oscilloscope) and then the two capacitors would be equal and you would know the unknown one. You would then have a capacitance bridge.

the capacitors are NOT variable nor are they equal. The resistors are NOT variable nor are they equal. There is no amp meter nor is there a voltmeter in the middle...there is only a switch that has been closed. Now, how would you figure out the potential between R3 and R4. Also, the current is DC from a Battery.
 
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To work out the voltage across across a capacitor in series with a resistor you draw a right angled triangle with , voltage across the resistor as the horizontal side and voltage across the capacitor along the vertical side, (usually downwards for capacitors) and total voltage across the hypotenuse.

Assume 100 volts across the series combination.
Take some random values for the capacitors and resistors.
C1 300 ohms reactance
C2 450 ohms reactance
R3 270 ohms
R4 120 ohms

First, the left series combination:
Impedance = sqrt ( 300 *300 + 270 * 270) =403.6 ohms
Current = 100 / 403.6 = 0.247 A
Voltage across resistor = 270 * 0.247 = 66.9 V
Voltage across capacitor = 300 * 0.247 = 74.1 Volts
Angle = tan-1(74.1 / 66.9) =-47.88 deg

Next, the right series combination:
Impedance = sqrt ( 450 *450 + 120 * 120) =465.7 ohms
Current = 100 / 465.7 = 0.215 A
Voltage across resistor =120 * 0.215 = 25.8 V
Voltage across capacitor = 450 * 0.215= 96.75 Volts
Angle = tan-1(96.75 / 25.8) = -75.06 degYou can't subtract these voltages because they are at different phase angles.
so:
Current in R3 is 0.247 A at +47.88 degrees relative to applied voltage.
Voltage across R3 is (270 * .247) at +47.88 degrees =66.69 V at +47.75 deg relative to applied voltage
Current in R4 is 0.215 A at 75.06 degrees relative to applied voltage
Voltage across R4 is (120 * 0.215) or 11.46 volts at 75.06 degrees relative to applied voltage. Graphing these, I get a voltage of "about 60 volts".

Solving it with trig, I get 56.66 volts

All of this was with the switch open and AC. (did it say that before?)

With the switch closed and DC, it is a lot easier.

The capacitors behave like open circuits at DC so the capacitors are not conducting so there is no current in the resistors, so the voltage across the resistors is zero.
 
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You have to find the differential equation of the voltage as a function of time. Use laplace transforms of the capacitance value to find impedance ie 1/cs ohms, then use nodal and mesh analysis to find the function. Inverse transform them back into the time domain then you have the voltage function with time. In this case it would be easier to find the differential function for current. Use product over sum to merge the capacitance value to one value. also add up the other resistances. This becomes a simple diff eq if it is a DC source or an AC source. If it is a DC source the current approaches zero as a function of time, therefore at steady state all of the current will travel through the resistors.
 
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With the switch closed and a DC supply, this just becomes two parallel resistors charging two parallel capacitors.

After the charging is finished (depending on the time constant), all the supply voltage will be across the two capacitors in parallel.
 
thank you for your help people! GREAT IDEAS!
 

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