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Peter Apps
Daniella Garcia-Loos
Peter Apps
Daniella Garcia-Loos
If you look around, most of the objects you encounter in your daily life aren't magnetic. This shouldn't be a surprise though, because creating a magnet requires a very specific set of both micro and macroscopic features. To begin with, we've known since the 1920's that a moving charged object can create a magnetic field and become its own tiny magnet. For reasons that we won't get into here, it's primarily the electrons that determine the overall magnetic field of the atom. These electrons can cause natural magnets to occur in elements with half-filled energy levels.
Image Courtesy of Minute Physics
Collections of these elements can create magnetic domains that can align (or be forced to align) to create an overall magnetic field. In the image below we can see an external magnetic field (yellow arrows) can be used to force the individual magnetic domains into alignment which magnetizes the entire material. This is similar to how when a magnet picks up a paperclip, the paperclip becomes magnetized.
Image Courtesy of Wikipedia
Check out this video by Minute Physics for a great overview of this.
You may remember playing with magnets in elementary school, using a compass or iron filings to show the shape of the field. Magnetic field lines show the direction that the north pole of a magnet will be pushed or pulled. Just like electric charges, we can use the rule "likes repel, opposites attract". So, a north pole will repel other north poles and be attracted to south poles. Also, like electric fields, we can tell the strength of the field visually by looking at how close the lines are together.
Image Courtesy of stickmanphysics
Here are some key points about how a magnetic dipole can be created:
The Earth also produces a magnetic field that protects us from a variety of cosmic radiation. The charged particles from the solar wind spiral along the magnetic field lines and collect around the poles resulting in auroras. In order for this to occur, particles need to be charged to be affected by the Earth's magnetic field.
Image Courtesy of wikipedia
Magnetic field strength is represented by B and has units of Tesla (T) where 1T = Ns / Cm. (Aren't you happy we can just write Tesla instead of Newton second per Coulomb meter? I am! 😄)
So, why do charged particles curve in a magnetic field? They experience a force! The force from a magnetic field can be calculated using this equation:
Looking at this equation, we can see that in order to be affected by a magnetic force:
** For the AP exam, you'll be expected to be able to quantitively analyze these scenarios when the velocity is 0°, 90°, or 180° relative to the magnetic field. For all other situations, we'll deal qualitatively with the outcome.**
Ok, so we can calculate the magnitude of the force, but what about its direction? This can be easily found using the Right-Hand Rule (RHR). Point your thumb in the direction a positive charge is moving, your other fingers in the direction of the magnetic field, and your palm will face the direction of the force.
Image Courtesy of schoolbag.info
** Note that the RHR tells you information for a positive charge. If you have an electron (or other negative particles) you can still use the RHR, but the force will be facing in the opposite direction (into your palm instead of out of it).**
So we've seen that a charge moving through a magnetic field experiences a magnetic force. Let's apply the same concept to a wire and see what happens.
Image Courtesy of cnx
Any wire with current passing through it becomes an electromagnet. The magnetic field lines are circular around the wire radiating outwards. Again, we can use the right-hand rule to determine the direction of the magnetic field. This application will be referred to as the Right-Hand Curl Rule (RHCR) since we now have 2 applications of this rule.
To do the RHCR, you position your hand with your thumb pointing in the direction of the current and curl your fingers around the wire. Your fingers point in the direction of the magnetic field. In the example above, the field is coming out of the page to the left of the wire and going into the page on the right side of the wire.
The internal magnetic field created by a very long current-carrying wire can be determined using the equation:
I is the current flowing through the wire, μo is the permeability of free space constant (found on the front page of your reference tables), and r is the distance away from the wire.
For a more detailed explanation of how this phenomenon works, check out part 2 of the Minute Physics video series on magnets.
Here are some key things to remember when drawing a magnetic field:
1.
Image Courtesy of the AP Physics 2 Course & Exam Description
Answer
Choice B is correct. Use the Right Hand Rule twice. First to find the direction of the magnetic field around the wire (should be coming out of the page above the wire, and into the page below the wire) then again to find the direction of the force the wire exerts on the charge (should be towards the the bottom of the page). The question asks for the force the charge exerts on the wire which is a Newton's 3rd Law pair with the force we just found. So the wire pushes the charge towards the bottom of the page and the charge pushes the wire towards the top of the page.
What, if anything, is wrong with this diagram?
Answer
There are 2 major problems with this diagram
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