Parallel Plate Capacitance and Charge Time

In summary, the question asked for when the capacitor would be fully charged, ie, when (for what t) does the capacitor charge become 6 V.
  • #1
HelloCthulhu
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Homework Statement
A 6V battery, 0.64mm diameter/14in length single/solid copper wire alligator clips how long and an 18cm disc parallel plate air capacitor are used in a circuit. What is the capacitance? How long will it take to charge the capacitor to 100% of its capacity?
Relevant Equations
A=πr2

capacitance
$$C=K\varepsilon_0\frac{A}{d}$$
Area of 18cm disc electrode = 0.0254469m2
d of separation = 0.01m
dielectric constant = 1
ε0 = 8.85×10−12 F/m−1

voltage respect to time
V(t) = VB(1-e[SUP]-t/RC[/SUP])
V(t) = voltage in respect to time
VB = battery voltage
-e (numerical constant) = 2.71828
-t = voltage in respect to time in sec
R = resistance of the wire
C = capacitance
RC = time constant = τ

resistance for the 14in long/ 0.64mm diameter wire found here:
https://www.cirris.com/learning-center/calculators/133-wire-resistance-calculator-table
$$C=K\varepsilon_0\frac{A}{d}=C=\frac{(8.85\times10^{-12})\times1\times 0.0254469}{0.01}=0.000022531F=22.531μF$$

6V*(1-2.71828-t/0.019Ω*0.0000225307uF)

time constants
6*(1-2.71828-1) = 6*(0.632) = 3.79 sec
6*(1-2.71828-2) = 6*(0.865) = 5.18 sec
6*(1-2.71828-3) = 6*(0.950) = 5.70 sec
6*(0.982) = 5.89 sec
6*(0.993) = 5.95 sec

capacitance = 22.531μF
100% charge time = 6 sec
 
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  • #2
0.993 is not equal to one. You also did not solve for t so your equations are dimensionally inconsistent.
 
  • #3
Orodruin said:
0.993 is not equal to one. You also did not solve for t so your equations are dimensionally inconsistent.

I apologize this is my first time doing this kind of equation. I used this video to learn about time constants:



In this equation I still have the -t value over the RC value:
6V*(1-2.71828-t/0.019Ω*0.00002253)

After the RC value was solved, I should've written these equations as:
6V*(1-2.71828-4.280833e-7/4.280833e-7)
6V*(1-2.71828-1)
6V*(0.632) = 3.79 sec
 
  • #4
Again, you are being dimensionally inconsistent. 6 V multiplied by a dimensionless number still has units of volts. What you have computed is the capacitor charge after a time t=RC. This is not what the question asked for, the question asked when the capacitor would be fully charged, ie, when (for what t) does the capacitor charge become 6 V?
 
  • #5
Ok, I was definitely confused earlier. I found a more detailed tutorial on this, so I hope I have a better understanding of time constants and charging time now:

https://www.electronics-tutorials.ws/rc/rc_1.html

1t = 0.019Ω*0.00002253uF = 4.280833e-7 secs
5t = 5X4.280833e-7 = 0.00000214041 secs
 
  • #6
You might want to check your exponent calculations for the capacitance calculation. I can't imagine how an 18 cm disc capacitor separated by 10 mm of air can give such a large capacitance (the numbers of the mantissa look good, but I think the power of 10 you've ascribed to the exponent is incorrect).
 
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  • #7
gneill said:
You might want to check your exponent calculations for the capacitance calculation. I can't imagine how an 18 cm disc capacitor separated by 10 mm of air can give such a large capacitance (the numbers of the mantissa look good, but I think the power of 10 you've ascribed to the exponent is incorrect).

You're absolutely right. I submitted 22.531μF as the solution to the capacitance equation. But the capacitance is 2.25307x10-11F (0.0000225307μF).

$$C=K\varepsilon_0\frac{A}{d}=C=\frac{(8.85\times10^{-12})\times1\times0.0254469}{0.01}=2.25307\times10^{-11}F=0.0000225307μF$$

I used this online calculator to check the work. Hope I got it right this time.
https://www.omnicalculator.com/physics/capacitance
 
  • #8
Yup. So think pF rather than ##\mu F## for the capacitance value.

Your idea of suggesting that a period of 5 time constants will settle the matter is good in "engineering" terms. It is true that the engineering rule of thumb is that everything of interest in a circuit has occurred after a period of five time constants. However, be aware that theoretically, a charging (or discharging) capacitor will never reach it's final charge in a finite amount of time. In other words, this may be a trick question. You may want to review the original question as presented to you to be sure that it is asking for an "engineering" solution or a theoretical one.
 
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FAQ: Parallel Plate Capacitance and Charge Time

What is parallel plate capacitance?

Parallel plate capacitance is the ability of two parallel conductive plates separated by a dielectric material to store electrical charge when a voltage is applied. It is measured in units of farads (F).

How is parallel plate capacitance calculated?

The capacitance of a parallel plate capacitor can be calculated using the formula C = εA/d, where C is the capacitance, ε is the permittivity of the dielectric material between the plates, A is the area of the plates, and d is the distance between the plates.

What factors affect parallel plate capacitance?

The factors that affect parallel plate capacitance include the distance between the plates, the area of the plates, the permittivity of the dielectric material, and the voltage applied to the plates. Increasing the plate area or decreasing the distance between the plates will increase capacitance, while using a material with a higher permittivity will also increase capacitance. Additionally, a higher voltage will increase the amount of charge that can be stored by the plates.

What is the charge time of a parallel plate capacitor?

The charge time of a parallel plate capacitor is the amount of time it takes for the capacitor to reach its maximum charge when a voltage is applied. This can be calculated using the formula t = RC, where t is the charge time, R is the resistance in the circuit, and C is the capacitance of the capacitor.

How can parallel plate capacitance be used in practical applications?

Parallel plate capacitance has a wide range of practical applications, including in electronic circuits, power supplies, and energy storage systems. It is also used in devices such as touch screens and sensors. Parallel plate capacitors can be used to store energy and release it quickly, making them useful in many different technologies.

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