Our bodies separate and store charge as a power source to transmit signals
along nerves. An excess of positive ions on the outside
of the cell membrane results in a potential difference across the membrane.
The inside of the cell is at a negative potential of ~100 mV with respect to the
outside. The membrane acts like a capacitor.
Electrical signals play a role in transmitting information through our bodies. Sensory information is transmitted via nerves. Each nerve consists of a bundle of nerve cells or neurons. A neuron receives stimuli at the input end and produces a signal that is transmitted across the axon to the output end. The axon membrane can be modeled as a charged capacitor. When the neuron is stimulated, the voltage across the capacitor rapidly changes and the charge on the plates reverses, only to thereafter quickly return back to its original value. For this to happen, a current must flow through some effective resistance. The whole axon can be modeled as a chain of capacitors and resistors connected in series and parallel. A voltage and current pulse propagates along this chain.
The speed of propagation of the
action potential depends on the electrical resistance R within the core
of the axon and the capacitance C across the membrane. A simple
electrical circuit, consisting of a resistor in series with a capacitor,
has a time constant τ = RC. The
time constant characterizes the time it takes for the capacitor to
charge and discharge and therefore limits the maximum speed with which
signals can travel through the circuit.
In this laboratory you will investigate the behavior of simple circuits containing resistors and capacitors. While you will not model neurons directly, you will become more familiar with how circuits in general behave, and therefore also with how neuron circuits behave.
Open a Microsoft Word document to keep a live journal of your experimental procedures and your results. Include all deliverables, (data, graphs, analysis, outcome). Write a 'mini-reflection' immediately after finishing each investigation, experiment or activity, while the logic is fresh in your mind.
Fatal electric shock occurs when a sufficiently large electric current flows through the body. A fraction of such a current flows through the heart and may disrupt the cardiac cycle. Typical effects are listed in the table below.
| Shocking current: | Effect: |
| <1 mA | no observable effect |
| ~1 mA - ~10 mA | tingling sensation |
| ~10 mA - ~100 mA | muscular paralysis ("can't let go") |
| ~100 mA | ventricular fibrillation |
| ~1A - ~10 A | thermal damage to tissue |
Paradoxically, brief currents of > 1 A may be less dangerous than lower currents. Instead of putting the heart into ventricular fibrillation, these currents clamp the whole heart muscle at the same time. When the current is turned off, a normal heart beat may resume on its own accord. Indeed, currents of about 1 A are used clinically to defibrillate the heart.
Experiment 1
Before taking any measurements or looking up data, make a prediction. Do you think your body's electrical resistance will be higher when your skin is completely dry, or when it is wet with tap water? Write down your reasoning.
Do you have a digital multimeter? Then use it to measure the resistance of
your body when you hold one lead of the multimeter in one hand and the other
lead in the other hand. (Switch the meter on the 20 MΩ (or closest) scale.
Make sure the leads are plugged into the Ω and COM
connectors of the meter. Press the thumb of one of your
hands against the black and the thumb of the other hand against the red lead.)
If you do not have a multimeter, look at shared data in the forum.
Do the results match your prediction? Why do you think moisture changes
the electrical properties of skin?
Based on the actual measured resistance, calculate what current would flow
through you if you accidentally touched a 110 V wall outlet with a wet or dry
hand while the other hand touches a grounded object. Look at the Fatal
Shock Table. What physiological effect would this have on you?
The salty fluids within the human body are electrical conductors. Salt water conducts electricity because it has mobile electrons and ionic states via the salt atoms. Salt water provides a large surface area of contact for the conductive element and it connects with the sweat glands so electricity can flow past the skin and into your body, which has low electrical resistance. The internal resistance of an arm (from hand to shoulder) is less than 100 Ω. If there is a voltage across this internal resistance, a current will flow and heat will be generated. If the current is large or the connection time is long enough, this heat will cause burns and destroy tissue. Fortunately the resistance of dry skin is high. The dry protein of your skin is an insulator. Using a typical contact area, the skin acts like an approximately (10 - 100) kΩ resistor in series with the internal resistance of the body. At voltages below about 50 V the dry skin provides safe current limiting protection.
Be extremely careful not to have electrical contact with a voltage source if you have wet or sweaty skin.
Experiment 1 Deliverables: (to be included in the your journal)
Activity 1
Link to the simulation: https://phet.colorado.edu/en/simulations/circuit-construction-kit-dc
Click the Lab icon. Explore the interface!
(a) Use one ideal battery (30V, 0 Ω internal
resistance), a light bulb (20 Ω) resistance) and ideal wires (near 0
Ω resistance) to build the circuit shown on the right. Make sure your
light bulb lights up. Use the voltmeter to measure the potential difference (ΔV)
across the battery. Record only the magnitude of the potential
difference (omit +/- signs). Make a similar potential difference
measurement across the bulb and across each length of wire. With
the non-contact ammeter, measure the current through the bulb, IBulb.
What to do if you have problems with the animation speed!
Fill in "Table A" below..
| ΔVBattery | ΔVwire A | ΔVwire B | ΔVBulb | IBulb |
|---|---|---|---|---|
(b) The Brightness Challenge
(i) You are given two 30 V ideal batteries and three 20 Ω light bulbs.
Your mission is to design a circuit that makes the bulbs glow as brightly as
possible. Experiment in the simulation. Take a screenshot your
winning circuit. Design your own data table to record the voltage and
current for each component. Explain why this specific configuration
(series, parallel, or a mix) maximizes the power delivered to the bulbs using
Ohm's Law.
(ii) Now design a circuit that makes all bulbs glow but produces the least
amount of light. Take a screenshot your winning circuit. Design your
own data table to record the voltage and current for each component.
Explain why this specific configuration (series, parallel, or a mix) minimizes
the power delivered to the bulbs using Ohm's Law.
(c) The Internal Resistance Puzzle
In the simulation, when the bulbs glow as brightly as possible, change the battery's internal resistance to 2 Ω. Don't fill out a table, just look at the bulbs. What physically changed? Why does a battery heating up internally affect the brightness of the bulbs down the line?
Activity 1 Deliverables: (to be included in the your journal)
Activity 2
In a few sentences explain how you can perform and experiment to find out if a circuit element is ohmic or nonohmic. What measurements do you make and how do you decide, based on the results of your measurements.
Activity 2 Deliverables: (to be included in the your journal)
Activity 3
Link to the simulation: https://phet.colorado.edu/en/simulations/circuit-construction-kit-ac
Click the Lab icon. Construct a circuit as shown in the diagram below.
Choose R = 50 Ω, C = 0.2 F, V = 9 V.
Use the voltmeter to measure the voltage across the capacitor.

An example is shown below.

(a) Look at the RC circuit before closing the switch.
At the exact millisecond the switch is closed (t = 0), do you think the
capacitor acts like an open switch (infinite resistance, blocking current) or a
straight wire (zero resistance, letting current flow freely)? Make a
hypothesis.
(b) Charging the capacitor:
With the simulation paused, start by clicking on the capacitor to discharge
it. The initial voltage across the capacitor should be 0 V.
Click the start button on the stopwatch. The stopwatch will start when you
play the simulation. Close switch S1.
You will monitor the voltage across the capacitor as a function of time as the capacitor in the RC circuit is charging. Start the simulation, then pause it at roughly 0.5 V intervals between 1 V and 8.9 V and record the voltage and time in a table in this spreadsheet.
We expect VC = V0(1 - e-t/τ), where V0
= 9 V is the battery voltage. We
can rewrite this as 1 - VC/V0 = e-t/τ,
or ln(1 - VC/V0) = -t/τ.
If we plot ln(1 - VC/V0) versus time the slope will be -1/τ,
where τ is the time constant of the RC circuit.
Activity 3 Deliverables: (to be included in the your journal)
Convert your journal into a lab report.
Name:
E-mail address:
Laboratory 3 Report
Save your Word document (your name_lab3.docx), go to Canvas, Assignments, Lab 3, and submit your document.