Physics 241 Lab: Solenoids
http://bohr.physics.arizona.edu/~leone/ua_spring_2009/phys241lab.html
Name:______
“When I Heard the Learn’d Astronomer”
When I heard the learn’d astronomer,
When the proofs, the figures, were ranged in columns before me,
When I was shown the charts and diagrams, to add, divide, and measure them,
When I sitting heard the astronomer where he lectured with much applause in
the lecture-room,
How soon unaccountable I became tired and sick,
Till rising and gliding out I wander’d off by myself,
In the mystical moist night-air, and from time to time,
Look’d up in perfect silence at the stars.
-Walt Whitman
Important:
· In this course, every student has an equal opportunity to learn and succeed.
· How smart you are at physics depends on how hard you work. Work problems daily.
· Form study groups and meet as often as possible..
· Join professional organizations.
· Physicists help people: science => technology => jobs.
Section 1:
1.1. A current carrying wire creates a magnetic field around the wire. This magnetic field may be found using the Biot-Savart Law . However, this law can be difficult to use. If there is a high degree of symmetry, you may choose to find the magnetic field produced by the current carrying wire using Ampere’s Law . Ampere’s Law simplifies finding a magnetic field in the same manner that Gauss’s Law simplifies finding an electric field.
Examine the ideal solenoid (also called “inductor”) where a very long coil of wire carries a current I is found to have a nearly uniform magnetic field inside the coils and a nearly zero magnetic field outside the coils. A cross sectional picture is provided:
In the laboratory, an experimenter may easily control the current through a solenoid, and so it is desirable to determine the strength of the magnetic field inside the solenoid as a function of the current. Because of the high degree of symmetry in the ideal solenoid, Ampere’s Law may be used to find the magnetic field inside the solenoid. Go over the following derivation with your lab partner since you will need to understand it for your lab report.
When the current in a wire changes, the strength of the magnetic field created by the current also changes. Therefore, if you know the time dependent behavior of the current, you can find the time dependent behavior of the magnetic field inside the solenoid. If the solenoid is carrying a sinusoidally oscillating current, then it will produce a sinusoidally varying magnetic field inside the coils.
1.2. A solenoid with 38,000 loops per meter is placed in series with a 10 W resistor and driven by a sinusoidally varying source voltage. Using an oscilloscope, the voltage across the resistor is found to be . Write a time dependent equation with numerical values to describe the time dependent strength of the magnetic field inside the solenoid. Then provide two specific times when the current and magnetic field have both simultaneously reached their respective amplitudes. Note that mo=4px10-7 [Tm/A].
Your answers:
Section 2:
2.1. Two very important concepts in the study of electricity and magnetism are Ampere’s Law and Faraday’s Law. Ampere’s Law states that a current in a wire creates a magnetic field. Faraday’s Law states that if the magnetic field changes (oscillates) the changing magnetic field will create a voltage in the wire. This voltage that is created by the changing magnetic field is call the “back EMF” or the “self-induced EMF”. Thus the logical flow of ideas is the changing current inside the solenoid wire causes a changing magnetic field between the solenoid coils that then causes a changing back EMF inside the solenoid wire. This is shown graphically for a sinusoidally oscillating circuit with a resistor and inductor in series:
2.2. Experimentally observe the 90o phase shift that shows that the oscillating voltage across an inductor leads the oscillating voltage across a resistor by p/2. Use a sinusoidal source voltage to drive an inductor in series with a resistor. Use your oscilloscope to measure the voltage across the resistor and inductor simultaneously so that you can view the 90o phase shift. Make a quick sketch of your observations below. Record your choices for resistance values, driving frequencies, etc. that enabled you to see the inductor lead the resistor.
Warning: at very low frequencies, the self-induced back EMF goes to zero because dB/dt is nearly zero so you would think that you would measure zero volts across the inductor. However, these inductors have ~1 km of wire and therefore some small resistance so at low frequencies you may register the voltage drop of the solenoid acting as a pure resistor. In this case, there is no phase shift. Check for yourself that the solenoid acts as a pure resistor at very low frequencies ~10 Hz.
Your parameter choices and quick sketch:
2.3. If a magnetic field is changing through the area of a loop of wire, then Faraday’s law says that this changing magnetic field will induce a negative voltage (called the back EMF) in the circuit:
· Faraday’s law: ,
where the magnetic flux fB is simply the magnetic field integrated over the cross sectional area of the wire loop:
· Magnetic flux: .
Since a solenoid has N loops each with a cross sectional area that is constant in time, this means that:
· Faraday’s law for fixed area and N loops: .
Due to the way we think about electronics, we need to remove the negative sign from this equation. This is similar to our use of V=IR for resistors in a circuit when technically the resistor causes a voltage drop (therefore a negative voltage change). Another way to think about this is that we can say that due to conservation of energy, adding all the voltages in a circuit together should yield zero: But we can always rearrange to have Thus you should write when measuring inductance in a circuit.
2.4. Find the time dependent back EMF created by the RL circuit given in section 1.2. if the cross sectional area of the inductor is 0.006 m2 and the inductor is 9 cm long. Your answer:
Restating the ideas of the previous section, if you take a single solenoid and apply an alternating source voltage, then it will have an alternating current. The alternating current of this single solenoid will produce an alternating magnetic field within the area of its own coils. Now, there is a changing magnetic field within the area of the coils. The changing magnetic field induces a voltage in this solenoid (the back EMF). This process is called self-inductance.
The parameter L (SI units of Henry) is used to describe the solenoid’s ability to self-induce a back EMF eL. This parameter is defined as:
.
Substituting the previous results and gives:
.
2.3. Find the self-inductance parameter L for the inductor described in sections 1.2. and 2.3. Your answer:
2.4. If you allow a magnet to swing at the end of a pendulum just barely above some nonmagnetic sheet of copper, the pendulum-magnet will lose energy and come to a stop. Explain where the energy goes using the concepts of eddy currents &Lenz’s Law. Your explanation:
Section 3:
3.1. Now you will experimentally examine the magnetic field produced by a solenoid with current flowing through it. Note that a real solenoid produces a magnetic field qualitatively similar to a bar magnet of the same dimensions.
First check that your compass has not been “flipped”. The compass arrow should align itself with the local magnetic field produced by the Earth. Remember that the Earth’s north magnetic pole is at the geographic south pole. This causes the local magnetic field to point toward the north geographic pole. The compass aligns with this magnetic field and thus points toward the north geographic pole. If your compass has been flipped, fix it with a strong magnet or tell your TA so they can fix it.
Examine the direction of the windings of your solenoid. You can tell which way the current circulates by how the wire enters the solenoid. Then you can use the right-handed screw rule to determine the direction of the magnetic field inside the solenoid (which side is north and which is south).
Apply constant current using the constant voltage supply (a few volts should be good) to your solenoid. Use the right-handed screw rule to predict the positive direction (north pole) of the magnetic field produced within the solenoid and the magnetic field surrounding the solenoid in general. Test your prediction using the compass and sketch the magnetic field surrounding the solenoid below. Be sure to draw your solenoid in such a way as to show the reader how the current flows through the solenoid (see previous pictures in this manual for hints).
Your sketch of the observed magnetic field within and surrounding a real solenoid with constant current:
Section 4:
4.1. In this section you will experimentally observe the process of self-inductance. Place a solenoid in series with a 100 W resistor and drive this simple RL circuit with a sinusoidal source voltage with 10 Hz (very slow) and 10 to 20 volts source amplitude. Set your oscilloscope to measure the voltage across the resistor. The resistor voltage tells you how much power the circuit is removing from the function generator. This also tells you about how much current is flowing through the resistor and therefore the solenoid.
Qualitatively examine what happens to the current in the solenoid (via resistor voltage) as you increase the driving frequency from 100 Hz to higher frequencies. Your observations:
The impedance cL of an inductor is found to be where L is the self-inductance parameter of the solenoid and wdrive is the angular driving frequency. The total circuit impedance without a capacitor is given by . Since , explain how IR would change if wdrive was increased. (This is an alternate explanation of the previous question.) Your explanation:
Section 5:
5.1. Restating previous ideas, Faraday’s Law states that a changing magnetic field will induce a back EMF voltage: . Technically this equation shows that the back EMF produced is proportional to the rate of change of the magnetic flux, but the magnetic flux is just the magnetic field integrated over the surface area of the circuit. In simple situations this just becomes . Since the presence of a back EMF is effectively like adding a battery to a circuit, a current can be induced in a circuit without any other voltage source present!
An example of this interesting situation is when a magnet approaches a solenoid in series with a resistor:
Here the magnet’s north pole is approaching the solenoid from the left. The magnetic field strength is growing inside the inductor coils as the magnet approaches . Lenz’s Law is a very simple rule that allows you to figure out the direction of the current flow caused by the induced back EMF. Lenz’s Law states that the back EMF will cause a current that generates it’s own reactionary magnetic field that opposes that change of the magnetic field inside the solenoid. In this case the magnetic field is growing to the right. Therefore, Lenz’s Law states that there will be a reactionary magnetic field growing to the left:
Now you can simply use the right-hand screw rule to find the direction of the current traveling around the inductor coils that will produce the correct reactionary magnetic field and trace this current through the wires to find the direction of the current through the resistor.
5.2. Now solve some “simple” applications of Lenz’s Law and the right-hand screw rule for finding the current induced in a circuit with no source voltage present.
Your answer:
Your answer:
Your answer:
Your answer:
Section 6:
6.1. Now you will experimentally observe how a changing magnetic field induces a voltage in an unpowered solenoid. Check your bar magnet with your compass to see that it is labeled correctly. Remember that the compass’s needle labeled “north” should point to south magnetic poles (like the north geographic pole of the earth).
Hook up your solenoid to the oscilloscope so you can measure the electric potential difference between both ends. Don’t bother placing a resistor in series; there won’t be large enough currents to measure with the oscilloscope. Instead you will just examine the direction of the back EMF by checking the sign of the voltage across the solenoid caused by the back EMF.
6.2. Move the north pole slowly toward one side of your solenoid. Write what you see on your oscilloscope (positive or negative induced voltage). You should see some induced voltage or you are moving too slowly. Try using 500 ms/div and 50 mV/div to clearly see the response. Your observation:
6.3. Move the north pole quickly toward same side of your solenoid as in 6.2. Write what you see on your oscilloscope and compare the amplitude of the induced voltage with part 6.2. Your observation and comparison: