Suppose that, while you are sitting in a chair, charge separation between your clothing and the chair puts you at a potential of 200 V, with the capacitance between you and the chair at 150 pF. When you stand up, the increased separation between your body and the chair decreases the capacitance to 10 pF. (a) What then is the potential of your body? That potential is reduced over time, as the charge on you drains through your body and shoes (you are a capacitor discharging through a resistance). Assume that the resistance along that route is 300GΩ. If you touch an electrical component while your potential is greater than 100V, you could ruin the component. (b) How long must you wait until your potential reaches the safe level of 100V?

If you wear a conducting wrist strap that is connected to ground, your potential does not increase as much when you stand up; you also discharge more rapidly because the resistance through the grounding connection is much less than through your body and shoes. (c) Suppose that when you stand up, your potential is 1400 Vand the chair-to-you capacitance is 10pF. What resistance in that wrist-strap grounding connection will allow you to discharge to100V in 0.30 s, which is less time than you would need to reach for, say, your computer?

Short Answer

Expert verified
  • a) The potential of the body is 3000V.
  • b)We need to waitlong until the potential reaches the safe level to 100V.
  • c) The resistance in the wrist-strap grounding connection is 1.1×1010Ω..

Step by step solution

01

The given data

  • a)Potential difference created due to charge separation between the clothing and chair,V1=200V
  • b)Capacitance between the chair and the body,C1=150pF
  • c)The decreased capacitance value,C'=10pF
  • d) Resistance along the route of body to shoes, R=300GΩ
  • e) If we touch an electric component with potential difference greater than 100V, the component gets ruined.
  • f) Potential difference when the body is standing, Vd'=1400V
  • g) The time to discharge , t =0.30s
02

Understanding the concept of potential drop

A condition of potential drop happens due to a change in charge separation between the two ends of the potential bridge because of discharging of the capacitance. This implies that the potential is related to the time constant of a circuit in the same way as the charge is related to it. Thus, using this condition, we calculate the required time and resistance as per the given circumstances.

Formulae:

The charge within the plates of a capacitor,q=CV (i)

The potential difference of a RC circuit,V=V0e-t/RC (ii)

03

 Calculation of the potential of the body 

(a)

In the process described in the problem, no charge is gained or lost. Thus, charge value is constant.

Now, using equation (i), the charge between the body and the chair will give the new increased potential on the body as follows:

C1V1=C2V2V2=C1V1C2=150pF10pF200V=3000V

Hence, the value of the required potential is 3000V.

04

 Calculation of the time of reaching the given potential 100V

(b)

The time constant value of a circuit not only describes the discharging condition of the charge but also the discharging of the potential difference. Thus, the time taken by the body to reach the safe level by discharging from the new potential V0=3000Vcan be given using equation (ii) as follows:

role="math" localid="1662727335305" t=RCInV0V=300×109Ω10×10-12FIn3000V100V=10s

This is a longer time than most people are inclined to wait before going on to their next task (such as handling the sensitive electronic equipment).

Hence, the value of time taken is 10s .

05

Calculation of the resistance of the wrist-strap

(c)

For the condition of standing, the resistance of the wrist-strap grounded connection needed for the potentialV0=1400Vto drop to the required safe level can be given using equation (ii) as follows:

R=tCInV0/V=0.30S10×10-12FIn1400/100=1.1×1010Ω

Hence, the value of the resistance is1.1×1010Ω.

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Most popular questions from this chapter

Cap-monster maze.In Fig. 27-22, all the capacitors have a capacitance of60μC, and all the batteries have an emf of 10 V. What is the charge on capacitor C? (If you can find the proper loop through this maze, you can answer the question with a few seconds of mental calculation).

In Figure,ε1=3.00V,ε2=1.00V , R1=4.00Ω, R1=2.00Ω , R1=5.00Ω and both batteries are ideal. (a) What is the rate at which energy is dissipated in R1 ? (b) What is the rate at which energy is dissipated in R2? (c) What is the rate at which energy is dissipated in R3? (d) What is the power of battery 1? (e) What is the power of battery 2?

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In Fig. 27-62, a voltmeter of resistance RV=300Ωand an ammeter of resistance RA=3.00Ωare being used to measure a resistance Rin a circuit that also contains a resistance R0=100Ωand an ideal battery of emf role="math" localid="1664352839658" ε=12.0V. Resistance Ris given byR=V/i , where V is the voltmeter reading and is the current in resistance R. However, the ammeter reading is inot but rather i', which is iplus the current through the voltmeter. Thus, the ratio of the two meter readings is notR but only an apparent resistanceR'=V/i' . IfR=85.0Ω , what are (a) the ammeter reading, (b) the voltmeter reading, and (c) R'? (d) IfRV is increased, does the difference between R'and Rincrease, decrease, or remain the same?

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