A schematic is a graphical representation of a circuit and is very useful in visualizing the main features of a circuit. Schematics use standardized symbols to represent the components in a circuits and solid lines to represent the wires connecting the components.
Nice blurb for the vocabulary term "schematic." Cf., also, * From GIS professionals, What are schematics? * From scientific visualization professionals, Difference between pictorial and schematic diagrams
The Series Combination of Capacitors
Review this section for Mini-homework 4, due Friday, 8:30 AM.
total capacitance
Oh, brrrother! This one was a pain in the brain, but I got it. Have you?
There are also higher-order moments, for quadrupoles, octupoles, and so on. You will see these in future classes.
As mentioned in lecture.
quadrupole
The quadrupole's electric field lines are starting to look like bundles of muscle fibers. I am not sure that is a coincidence...
Two large charged plates
Good practice problem.
An electron and a proton, each starting from rest
A nice workout.
potential
Typo by author: should read, "Find the electric field..."
The fields of nonsymmetrical charge distributions have to be handled with multiple integrals and may need to be calculated numerically by a computer.
Yes, with lots of CPU time.
Electric Field of a Line Segment
A good example to study, fairly simple calculus.
(b)
Author's typo; should read, \(2.638\times 10^{13}\tfrac{m}{s^2}\)
4: (a)
Author's typo; should read \(-6.76\times 10^5\,C\)
We assume that the dipole is a permanent dipole;
These are found in nature. One example is a water molecule. The water molecule can be dissociated into hydrogen and oxygen, i.e., dialysis, so it is not permenently permanent, but for many applications, such as a microwave oven, it does hold together in an external \(\vec{E}\) field.
Rotation of a Dipole due to an Electric Field
Another interesting fact about forces on a dipole: they create torque! It's not a problem, though. It is a feature! Microwave ovens would be useless without polar water molecules getting spun up.
-600 C
WAY OFF. Thank you, Amanda M. for catching the textbook author's NAPPIN'!!!!!
True answer: -28.8 Coulombs
(a) What is the electric field of an oxygen nucleus
Try this one, and then check the solution.
What is the electric field of a proton
Another good study problem.
The electric field in a particular thundercloud
Good study problem.
Example
Good example to workout
xample
Another good example to workout
Suppose we have N source charges q1,q2,q3,…,qN located at positions r→1,r→2,r→3,…,r→N, applying N electrostatic forces on a test charge Q.
This is the principal abstraction of the semester: the electric field, \(\vec{E}\).
The idea of "abstracting" is visible in the mathematical process of factoring, which the author does here when he factors out a common factor, the test charge \(Q\), from the big sum of forces.
Then, later in the semester, the structure of spacetime will require that we see the electric field's "partner in crime," the magnetic field, customarily written as \(\vec{B}\). Then the drama of electromagnetic radiation, light, will play out in the coupled oscillation of \(\vec{E}\text{ and }\vec{B}\), transporting energy, momentum and angular momentum across spacetime.
we often define a Coulomb’s constant
I hardly ever use \(\epsilon_0\). Mostly, I use Coulomb's constant, \(k\). However, the textbook authors use \(\epsilon_0\) frequently...
dry table salt
But in a solution, NaCl dissociates into ions!
In Gravitation(opens in new tab), we examined the force of gravity, which acts on all objects with mass. In this chapter, we begin the study of the electric force, which acts on all objects with a property called charge. The electric force is much stronger than gravity (in most systems where both appear), but it can be a force of attraction or a force of repulsion, which leads to very different effects on objects. The electric force helps keep atoms together, so it is of fundamental importance in matter. But it also governs most everyday interactions we deal with, from chemical interactions to biological processes.
A good intro blurb, comparing the gravitational interaction,
$$\vec{F}\left(r\right)=-\frac{G m_1 m_2}{r^2}\hat{r}$$
to the Coulomb interaction,
$$\vec{F}\left(r\right)=\frac{k q_1 q_2}{r^2}\hat{r}$$
in which \(\hat{r}\) points from object #1 toward object #2.
Rectangular Toroid
Reminiscent of the "Tokamak" structure of ITER.
If we take the time derivative of the angular momentum, we arrive at an expression for the torque on the particle
Be sure to read through this section on torque.
Notice that if θ=0, then dB→=0→. The field produced by a current element Idl→ has no component parallel to
Not quite.
If \(\theta=0\), then the field point \(P\) is directly ahead of the wire element \(d\vec{\ell}\).
That is, \(d\vec{\ell}\parallel\hat{r}\), because \(\hat{r}\) points from \(d\vec{\ell}\) to \(P\).
There is a set of locations \({P_i}\) in spacetime where the field \(\vec{B}\) is absent. For the electric field, you could say that for MANY sets of locations, like the midpoint between two like charges, a ++ array or a -- array.
You can find the direction of B→ with a right-hand rule: Curl your fingers in the direction of the current, and your thumb points along the magnetic field in the interior of the solenoid.
Decent description of using right hand rule for the central \(\vec{B}\) field direction
angular velocity
Angular velocity \(\omega=\frac{d\theta}{dt}\) is like the rate of revolutions per minute, RPM, except in physics we generally do not work in units of whole revolutions and minutes. but in radians of arclength per second. I.e., \(\left[\omega\right]=\text{seconds}\)
An angular velocity like this will make sense for any pixel of an extended object, at any distance away from the center or rotation or spin.
Nonuniform circular motion:
An example of this is a driver making a turn onto the interstate (so a bit of centripetal acc.) and speeding up at the same time (a few \(m/s^2\) of tangential acc.), speeding up to merge with the flow of traffic.
if they are, they cancel one another
E.g., a spring laid out horizontally on a smooth tabletop, so smooth we can neglect friction for small amplitude experiments. The other forces are downward weight force,
$$\vec{W}=\left(mg\right)\hat{j},\quad g=-9.8\frac{m}{s^2}$$,
and the upward normal force \(\vec{N}\) from the rigidity of the surface, which exactly balances the weight force.
more complicated forces
An example of a "more complicates" force is the restoring force of a spring on a object free to move along some axis, like an x-axis on a frictionless tabletop.
In that case, \(\vec{F}\left(x\right)=\left(-kx\right)\hat{i}\)... an interesting work integral.
To be precise, this fast-moving signal, or shock wave, is a rapidly propagating change in the electrical field.
Good. "rapidly propagating change in the electrical field" means $$\frac{d\vec{E}\left(x,\,t\right)}{dt}\gg 0$$ which depends on density of the conduction electrons in the conductor, the temperature, the voltage gradient and a few other factors.
Interestingly, the individual charges that make up the current move much slower on average, typically drifting at speeds on the order of 10−4m/s. How do we reconcile these two speeds, and what does it tell us about standard conductors?
Drift velocity is quite slow.
Electrical signals move very rapidly.
Although, it may seem that the lights come on when you click the switch, the "signal" does not move instantaneously!
closed
Idealized view, but useful for practice.
Electric Field of a Conducting Plate
A good example to look at, because we will be studying the electrostatic field between two parallel plates, one positively charge and the other negatively charged.
This is the famous device known as a capacitor.
in static equilibrium
Equilibrium, no accelerations, is the key concept in this section.
The height and cross-sectional area of the cylinder are δ and ΔA, respectively. The cylinder’s sides are perpendicular to the surface of the conductor
Mislabeled in Fig. 6.39. The figure's cylinder has height marked as \(\sigma\) but should be \(\delta\).
Problem-Solving Strategy: Gauss’s Law
This is a nice synopsis.
Integration at its most basic is adding up a bunch of tiny areas shaped like trapezoids, flat bottom and parallel vertical sides \(\perp\) bottom, with slanted top determined by the derivative of the integrand, i.e., of \(f^{\prime}\left(x\right)\) when integrating \(\int\, f\left(x\right)dx\).
But Gauss' Law simplifies that tedious, difficult process by taking advantage of symmetry in the source array.
forces
Anytime you use the word "dynamics," you imply that forces are under consideration in some manner.
A Ladybug Walker
This is a good mini-workout, and the solution is given. Note the introduction of unit vector \(\hat{u}\).
Today, as a result of developments in nuclear physics, we regularly convert mass into energy in power plants, nuclear weapons, and high-energy physics experiments in particle accelerators.
It is so much more powerful than the energy we can easily get from oil, coal or natural gas!
between times and That area is equal to the area inside the rectangle bounded by and
Author means \(t_2\)
useful angles expressed in both degrees and radians is
Unfortunately, the radians column is messed up, too tiny. $$30^{\circ}\longleftrightarrow\frac{\pi}{6}$$ $$45^{\circ}\longleftrightarrow\frac{\pi}{4}$$ $$60^{\circ}\longleftrightarrow\frac{\pi}{3}$$ $$90^{\circ}\longleftrightarrow\frac{\pi}{2}$$ $$120^{\circ}\longleftrightarrow\frac{2\pi}{3}$$ $$135^{\circ}\longleftrightarrow\frac{3\pi}{4}$$
Comets and Asteroids: Debris of the Solar System
Skim in this chapter for lecture on Friday, Feb. 20th...
A 76.0-kg person is being pulled
This is essentially a traffic light problem.
Because gravity is vertical,
I.e., there's no such thing as horizontal gravity.
the result is independent of the order in which the subtraction is made
Be careful. This is true for vectors
$$\vec{H}-\vec{P}=\left(-\vec{P}\right)+\vec{H}=\vec{H}+\left(-\vec{P}\right)$$
but not exactly the same for numbers: $$7-2.2\ne2.2-7$$
how different samples vary.
A good example is the solar system's comets. We took centuries of observation to get a rough idea of what they were. But in the 20th century and this century we have observed and seen the mathematical patterns of a few large groups of comets. Each group has orbital or compositional properties that vary significantly from other comet groups.
After a period of philosophical struggle
...headlined by Copernicus, Kepler and Galileo!
adding circle after circle to represent the movements of the planets around Earth
Those extra circles are known as epicycles. Cf., Ch. 2.4
objects that lie beyond our planet Earth
It is interesting that Galileo, our hero from the origin of modern science, figured out that Earth definitely orbits the Sun, and, through observation, many other astronomical facts. But he did make a few errors. For instance, he initially thought that comets were objects high up in our atmosphere!
It can be shown
This is the most abused phrase in all of science. It is sometimes known as "waving your hands," and it is usually a subsitute for doing a big pile of calculus, in this case, three-dimensional calculus. So for PHY2054, we will let discretion be the proverbial better part of valor and accept this important result. Why is it important? It is important because we now have an oscillator system!
Considerations of how Maxwell’s equations appear to different observers led to the modern theory of relativity,
As I have emphasized!
where is the magnetic field strength over an area , at an angle with the perpendicular to the area as shown in Figure 4.
Flux is a fancy way of counting field lines cutting through a given area.
by these rules:
Very important, especially when we get to the topic of flux.
radiation
Not electromagnetic radiation, per se, but charged particles, the protons, electrons and other ions that get lofted from the surface of the Sun, sometimes explosively so.
Explain the importance of the time constant, ,
We will tackle this calculus problem using a spreadsheet method, as we have before!
Voltage is similar to fluid pressure. The voltage source is like a pump, creating a pressure difference, causing current—the flow of charge. The resistor is like a pipe that reduces pressure and limits flow because of its resistance.
A handy analogy. Think of resistance like a load of gravel in a water pipe. Water flows, but not so plentifully as in an empty pipe.
shock wave moves through the system at nearly the speed of light.
Here is the answer to the riddle, drift speed very small, but lights go on almost instantly.
PhET Explorations: Capacitor Lab
Here is the link,
https://phet.colorado.edu/sims/html/capacitor-lab-basics/latest/capacitor-lab-basics_all.html
water molecules gather ions much more effectively because they have an electric field and a separation of charge to attract charges of both signs.
I,=.e., a good solvent
9: The naturally occurring charge on the ground on a fine day out in the open country is . (a) What is the electric field relative to ground at a height of 3.00 m? (b) Calculate the electric potential at this height. (c) Sketch electric field and equipotential lines for this scenario.
A nice workout.
calculate it
There seem to be some typos in the equations below this point. I will try to mend them.
electron–antielectron pai
Yes, we discussed the Feynman diagram for this process in lecture on 6/23/25.
Solving for the position
Similar to $$y\left(t\right)=y\left(0\right)+v_y\left(0\right)t+\tfrac{1}{2}gt^2$$
Constant Acceleration
This is basically a "sideways" gravitational system, \(U_1\left(x\right)=\kappa\,x\) as compared to regular gravitational potential energy, \(U\left(y\right)=\gamma\,y\).
$$\kappa=-E/x_0$$ and $$\gamma=-mg$$
If horizontal gravity DID exist, it would be something like \(U_1\)
an arbitrary direction by d→l,dl→,d\mathbf{\overset{\to }{l}}, so
Similar to my notation, \(d\vec{s}\).
Figure and Figure
ambiguous :(
Substitute
That is a method of pain.
It is better just to know that 1. if \(F\left(x\right)=m\ddot{x}\left(t\right)=-kx\), then \(x\left(t\right)\) is sinusoidal in time, \(x\left(t\right)=A\sin\left(\omega t\right)\) or \(A\cos\left(\omega t\right)\) 2. alternatively, if \(U\left(x\right)=\tfrac{1}{2}kx^2\text{ then }F\left(x\right)=-\frac{d}{dx}U\left(x\right)=-kx\), so \(x\left(t\right)\) is sinusoidal etc.
Then go from there.
Sinusoidal Oscillations
One of the most important examples in the entire book.
can oscillate
Even though it is not exactly a \(\tfrac{1}{2}kx^2\) potential.
Quartic and Quadratic Potential Energy Diagram
Sometimes known as a "sombrero potential" in quantum field theory.
Sometimes, this expression is more convenient to use
Especially when thinking about 1. oscillators and 2. various field like the electromagnetic field.
A 75.0-kg person walks down the central aisle of a subway car
A famous type of example. Einstein wrote his first papers on relativity with explanations of street cars moving at various speeds relative to an observer on the sidewalk. 🙂
displacement from the spring’s unstretched (equilibrium) position
Frequently, we have the freedom to assign the origin to that equilibrium position \(\vec{x}_{eq}\) so that \(\Delta\vec{x}\longrightarrow x\) and \(\vec{F}=\left(-kx\right)\,\hat{i}\).
Wgrav,AB=−mg^j⋅(→rB−→rA)=−mg(yB−yA).Wgrav,AB=−mgj^⋅(r→B−r→A)=−mg(yB−yA).
Important. If initial point A is above final point B, then (yB - yA) is negative and the product -mg(yB-yA), is positive....it uses the author's g value, 9.8 m/s^2. This means the object gains energy as it falls, kinetic energy.
foot-pound (ft⋅lb).(ft⋅lb).
You occasionally see commodities and machines rated in foot-pounds.
component acting parallel to the other component
In our case, the component of the force acting parallel to the path, \(F_{\parallel}\)
complete understanding of an object’s motion
Momentum and energy are part of the four-dimensional vector that completely encodes an object's dynamics: $$\mathbb{P}= \begin{bmatrix} E/c \ p_x \p_y \ p_z
\end{bmatrix}$$ c = speed of light. This vector is known as the four-momentum and the energy-momentum four-vector.
This impulse is equal to the object’s change of momentum.
Useful non-calculus shorthand: \(\vec{F}_{net}\Delta t =\Delta\vec{p}\)
the rate of change of the momentum that the force causes.
I.e., \(\vec{F}_{net}=\frac{d\vec{p}}{dt}\)
Figure 9.13
The grip is wrong in this diagram, by about \(90^{\circ}\). Do you verify?
Equations of Motion for Uniform Circular Motion
We will lecture on this on 2/7/25
for small angles (less than about ), ( and differ by about 1% or less at smaller angles).
The famous small angle approximation. See, for instance, "Trig function series."
The free-body diagram shows the vertical and horizontal forces acting on the traffic light.
I like this way of diagramming the set of x- and y-components. : )
The large horizontal components are in opposite directions and cancel,
A pattern
Note that the vertical tension in the wire acts as a normal force
I never use the term "normal force" in this manner, because there is no surface in this example. But the textbook author uses the term this way, so take it with a grain of force.
Solution for (a)
Slightly different strategy than what I use: * calculate rise time to apogee, using \(v_y\left(0\right)\); * calculate y-coordinate of apogee; * figure out the drop distance on the downhill side of the arc; * figure out the drop time from apogee to landing point;
This method avoids the big nasty quadratic formula, but you can surely use quadratic formula. : )
Note: in this problem, the rise time (from volcano to apogee) is shorter than the drop time, because the total arc is not symmetric.
Can a goalkeeper
Good exercise
An arrow is shot from a height of 1.5 m toward a cliff of height
Reverse of the "baseball from the top of a cliff" example. I..e., it STARTS at the bottom of the cliff. Key time = 4.0 s.
How many meters lower will its surface be 32.0 km from the ship along a horizontal line parallel to the surface at the ship?
WHOA. Very intriguing!
The cannon on a battleship
Hmmmm. I am intrigued by this one. :D
it is caught at the same height as it left his hand.
home run problem
the bull’s-eye of the target is at same height as the release height of the arrow
home run problem
the top of the takeoff ramp is at the same height as the bus tops
This makes it a "home run" type of problem, i.e., using the symmetries of the ballistic arc that launches and lands at the same y-coordinate.
vertical
I never use the equation involving \(v_{0y}^2 \) and \(v_y^2\), because they are best to study in relation to energy and momentum concepts in later chapter. You can do all projectile problems without it, so THINK carefully.
3: Describe a situation in which one system exerts a force on another and, as a consequence, experiences a force that is equal in magnitude and opposite in direction. Which of Newton’s laws of motion apply?
We will discuss this in lecture on Monday, Aug. 19.
they are internal
This distinction -- internal vs. external -- will be important when we take a peek at atoms.
an acceleration
...an acceleration of the professor and the cart of equipment at the same rate.
Birds and airplanes also fly by exerting force on air in a direction opposite to that of whatever force they need. For example, the wings of a bird force air downward and backward in order to get lift and move forward.
This is an alternate description of the idea of dynamic lift. The usual description of dynamic lift involves a pressure differential in the surrounding fluid, air, due to the Bernoulli Effect.
loosely
In the energy-momentum method for studying the dynamics of a system, later in this textbook, we will find a perfect quantity that encodes the interaction equally, so that "action-reaction" is no longer a loose usage.
complicated mechanism
An understatement.
For example, let’s compare the motions of two baseballs. One baseball is dropped from rest.
Similar to a Ferrari going off a cliff, a problem that has been on midterms in previous semesters.
Although varies from to , depending on latitude, altitude, underlying geological formations
This kind of variation is how petroleum geologists discovered the Chicxulub impact crater in the Yucatan and Gulf of Mexico. This asteroid/comet impact is what scientists now believe triggered the extinction of most dinosaurs.
the average value
Be aware.
The textbook uses \(g=9.80\,m/s^2\) for the acceleration due to gravity at the surface of Earth. I, however, prefer to encode the direction with a - sign, $$g=-9.8\frac{m}{s^2}$$
A vector is any quantity with both magnitude and direction.
The definitive vector is the velocity vector, also defined as a tangent vector especially when working in four dimensional spacetime.
Greek letter (delta) always means “change in”
D for \(\Delta\), D for difference, i.e., subtraction.
sells bags of apples
Labeled as "5 lbs," so that is like the notional value "45000 miles" in the previous example.
they are each rather close to the actual location
If you were at a rifle range, sighting in your hunting gear, then you'd say, "Yes, I am inside the first ring, but that would not be good enough unless I am shooting the side of a barn." So maybe you adjust the magnification of your optics or buy a new sight with better optics.... or keep practicing!
rather far away from the actual location of the restaurant
So, if you were at a rifle range, you'd want to adjust your sights slightly, to get that group up and to the right, into the center.
“known masses”
The metric system is based on cubic centimeters (cc) of liquid \(H_2O\). Balance the object you are measuring with a number of cc's of liquid water, that will tell you the number of grams in your object. That is the theory. In practice, yes, you'd use various carefully machined metal cylinders etc.
observation and experiment
A famous dictum, ascribed to Galileo, is
"Measure what is measurable, and make measurable what is not so."
Perform unit conversions both in the SI and English units Explain the most common prefixes in the SI units and be able to write them in scientific notation
Good to review and double-check from time to time during the semester.
must be used for objects smaller than can be seen with a microscope.
Where Planck's constant, \(\hbar=6.58\times 10^{-16}\,eV\,s\) rules all, in which the wave properties of matter are significant.
Relativity must be used whenever an object is traveling at greater than about 1% of the speed of light or experiences a strong gravitational field such as that near the Sun.
Systematic explication of how four-dimensional spacetime behaves under various energy conditions, how four dimensional spacetime curves and affects various forms of energy, and all because of the nature of LIGHT. \(E=mc^2\) is just one equation from the most basic relativity ideas.
mystery, imagination, struggle, triumph, and disappointment
"Drama" :D
membranes.
Electrical structures. You will learn this in PHY2054.
It is not necessary to formally study all applications of physics. What is most useful is knowledge of the basic laws of physics and a skill in the analytical methods for applying them.
An enormous statement. It emphasizes what scientists do: figure out new things, by putting together a framework from first principles. That is problem-solving, which is what we want to be able to do on PHY2053/4.
from one location to another
And because GPS, of necessity, uses Einstein's general theory of relativity, even though the spacetime curvature in the neighborhood of Earth is so tiny, the civilian GPS in your vehicle can locate your vehicle to within a few feet almost anywhere on Earth. Without relativity, GPS would not be nearly as precise.
you will gain analytical abilities
I.e., learn to THINK.
broadly applicable physical laws, permitting an understanding beyond just the memorization of lists of facts.
This is why studying for a physics class is different from a class where memorization is of paramount importance, like an anatomy class.
as food calories, batteries, heat, light, and watch springs
...as well as the theory of currved four-dimensional spacetime, Einstein's general theory of relativity.
quarks
Sub-nuclear particles that bind together to form protons and neutrons plus other exotic subatomic particles like the \(\pi^+\) meson.
An RLC circuit
A nice simulator for RLC and RC and LC circuits.
Try
Worth fooling around with this one.
angular frequency of the oscillations
Derived in lecture on 11/15
we obtain
Here is the precise combination in terms of \(R\), \(L\), and \(C\).
Damped oscillations of the capacitor charge are shown in this curve of charge versus time, or q versus t. The capacitor contains a charge q0q0{q}_{0} before the switch is closed
Discharge curve, a combination of real exponential \(e^{-\alpha t}\times\) complex exponentials \(e^{\pm i\omega t}\)
Ey(x,t)=E0cos(kx−ωt).Ey(x,t)=E0cos(kx−ωt).{E}_{y}\left(x,t\right)={E}_{0}\phantom{\rule{0.2em}{0ex}}\text{cos}\phantom{\rule{0.2em}{0ex}}\left(kx-\omega t\right).
Phase \(\phi=kx-\omega t\)
Phase \(\phi=0\) corresponds to the first peak of the \(E_y\) field; \(\phi=2\pi\) corresponds to second peak, and so on. This means that the equation \(kx-\omega t=0\) is the equation of motion for the first peak of the wave, the "wave top" of the wave. Another way to view this is that
$$x=\frac{\omega}{k}t$$
That factor \(\frac{\omega}{k}\) must be the same as \(c\), the speed of the light wave.
Fourier’s theorem
Fourier transforms, another huge tool
This is the form taken by the general wave equation for our plane wave.
This concludes the derivation of the wave equation for electromagnetic waves, specifically for \(E_y\left(t,x\right)\). The constants \(\epsilon_0\text{ and }\mu_0\) are related therefore to the speed of light, \(c\).
we can set Qin=0Qin=0{Q}_{\text{in}}=0 and I=0I=0I=0 in Maxwell’s equations
a.k.a. the vacuum solutions
beyond the scope of this textbook.
Understatement. It is a lifetime's study, and that would only be scratching the surface.
do not require a medium for their propagation.
i.e., only a vacuum is needed.
through space
Even through a vacuum
interference patterns
Here is a nice blurb in YouTube about interference patterns. It is a HUGE tool for physicists and engineers. https://youtu.be/D7aftTF--5w?si=hABIsE089aUZpVT0
propagate through space.
A nice diagram
This unification of forces has been one motivation for attempts to unify all of the four basic forces in nature—the gravitational, electrical, strong, and weak nuclear forces
Einstein's great quest, but he died before he reached it, and, in fact, no one has reached it yet.
contains a charge q0q0{q}_{0} before the switch is closed
Initial condition: Charged up, i.e., \(q\left(0\right)=q_0\)
the electromagnetic energy of the oscillating circuit
Nice exercise
initial energy of the system
I.e., initial load in the capacitor
what is C
plug-in exercise
How long does it take the capacitor to become completely discharged?
Good exercise
The time variations of q and I
It is interesting to normalize the total energy equation to 1 by dividing both sides by U -- should result in a version of the Pythagorean Identity \(\sin^2\left(x\right)+\cos^2\left(x\right)=1\)
Joule heating
Joule heating, for which the energy dissipation rate is \(P=I^2 R\), and which is also known as "\(I^2 R\) heating."
Since there is no resistance in the circuit
idealization
all the energy is stored in the magnetic field of the inductor
Similar to a spring system at equilibrium, \(x=0\), where kinetic energy
$$\frac{1}{2}m\dot{x}^2$$
is maximum.
This energy is
If you think of the charge \(q\left(t\right)\) as a coordinate, e.g., like \(x\left(t\right)\), then \(U_C\) is like the potential energy of a spring oscillator,
$$U=\frac{1}{2}kx^2$$
but for which the spring constant is \(1/C\)
the total energy U in the circuit is given by
Resembles another famous system,
$$E=\frac{1}{2}kx^2+\frac{1}{2}m\dot{x}^2$$
the harmonic oscillator.
With the substitution of Equation 14.14, this becomes U=12LI2.U=12LI2.U=\frac{1}{2}L{I}^{2}. Although derived for a special case, this equation gives the energy stored in the magnetic field of any inductor.
Quadratic in current \(I\), therefore current \(I\) will oscillate.
velocity selector
We will review this application in lecture
0.5-mm segment
Note that the diagram here and Fig. 12.3, greatly exaggerate the length of the line element \(d\vec{\ell}\)
The diagram in Webcourses is much more accurate.
If not
A big "if" with a ton of trig involved.
Since the current segment is much smaller than the distance x
Since \(x\gg\ell\), the approximation as \(\Delta\ell\) is good, and so is the approximation \(r_p\approx x\)
A 10-A current flows through the wire shown.
Homework problem
You might expect that two current-carrying wires
We will tackle this section and 12.1 Biot Savart Law on Monday, Nov. 6 Biot-Savart is ROUGH.
The component of the velocity perpendicular to the magnetic field produces a magnetic force perpendicular to both this velocity and the field: vperp=vsinθ,vpara=vcosθ.vperp=vsinθ,vpara=vcosθ.{v}_{\text{perp}}=v\phantom{\rule{0.1em}{0ex}}\text{sin}\phantom{\rule{0.1em}{0ex}}\theta ,\phantom{\rule{0.5em}{0ex}}{v}_{\text{para}}=v\text{cos}\phantom{\rule{0.1em}{0ex}}\theta . where θθ\theta is the angle between v and B.
Needs a diagram!!!!!! A 3-D blackboard is needed here.
following figure
heinous diagram
circular motion of the charged particle
Because \(\vec{F}\text{ is always }\perp \vec{v}\)
A magnetic field is defined by the force that a charged particle experiences moving in this field,
Operational or experimental definition, but not a theoretical definition!
The compass needle near the wire experiences a force that aligns the needle tangent to a circle around the wire.
What the observer sees: the compass needle aligns to the field. Lecture, 10/23
What is the average
I am not sure why this problem is here.
To form a hydrogen atom
Good. Be sure to verify this answer.
If Q3Q3{Q}_{3} starts from rest
Technically, this makes the problem insoluble, since it is not specified that \(Q_1\) and \(Q_2\) are static, fixed in place, or not. IF you consider then to be fixed in place, it is an easy problem we have already studied. So proceed on that basis: I may review this problem in lecture on Wednesday, or in Discusssions.
Consider a charge Q1(+5.0μC)Q1(+5.0μC){Q}_{1}\left(+5.0\phantom{\rule{0.2em}{0ex}}\mu \text{C}\right) fixed at a site
A good workout with the nitty gritty of EPE, KE etc.
Is the electrical potential energy of two point charges positive or negative
Significant question. The potential energy curve rules the dynamical world.
* Here is a potential barrier,
* Here is a potential well.
There is a huge difference between them, and the implications extend from quantum electrodynamics to black holes.
Assembling Four Positive Charges
Finish working this one out, and try to follow the logic of the textbook authors. It is slightly different than my description, so understanding both will help you.
all of the potential energy gets converted to kinetic.
"energy at infinity" is all kinetic. The charge Q effectively has no interaction with q.
it is perpendicular to the displacement along these arcs.
As noted in lecture, 10/2
Potential Energy of a Charged Particle
A good problem to work out.
Electric Field between Oppositely Charged Parallel Plates
This diagram and description will be on part 1 of the midterm, one or two multiple choice concept questions
Note that the electric field outside a spherically symmetrical charge distribution is identical to that of a point charge at the center that has a charge equal to the total charge of the spherical charge distribution. This is remarkable since the charges are not located at the center only.
Also a very important result in Newton's Law of Universal Gravitation.
permittivity of free space
$$k=\frac{1}{4\pi\epsilon_0}$$ so $$\epsilon_0 = \frac{1}{4\pi k}$$
This can be directly attributed to the fact that the electric field of a point charge decreases as 1/r21/r21\text{/}{r}^{2} with distance, which just cancels the r2r2{r}^{2} rate of increase of the surface area.
Not a coincidence. The Coulomb interaction is formally an infinite range interaction, directly because it is inverse \(r^2\)
Therefore, we can write the electric flux ΦiΦi{\text{Φ}}_{i} through the area of the ith patch as
Preparing to integrate!
Example
Nice example, very basic
It is positive when the angle between →EiE→i{\stackrel{\to }{\textbf{E}}}_{i} and ^nn^\hat{\textbf{n}} is less than 90°90°90\text{°} and negative when the angle is greater than 90°90°90\text{°}.
$$0^{\circ}\leq\theta\leq 180^{\circ}$$ I.e., from parallel to antiparallel
This estimate of the flux gets better as we decrease the size of the patches.
Here we go. Calculus ahead
similar to the way
Also similar to how CGI makes Gollum from the "wire frame" generated by Andy Serkis' motion capture suit.<br />
On a closed surface such as that of Figure 6.6(b), ^nn^\hat{\textbf{n}} is chosen to be the outward normal at every point
Important
area (A)
Its destiny is to become an element of area, e.g.,
$$dA=dx\, dy$$
or
$$dA=r\,dr\,d\theta$$
N
Unfortunate choice of symbol, because it confounds with the unit of E field, \(\frac{N}{C}\).
(N⋅m2/CN·m2/C\text{N}·{\text{m}}^{2}\text{/C}).
I.e., units of E field, \(\frac{N}{C}\,\,\times\) units of area \(m^2\).
a hula hoop in a flowing river
Even better: a hula hoop held out the window by a friend as you drive up Alafaya to Publix for Chinese food. Even your hand out the window works a bit as an analogy. If your hand is orthogonal to the road and therefore to the velocity of the air rushing past, you feel its force of air resistance. But if you hold your palm flat, parallel to the road surface, you feel way less air resistance.
the number of electric field lines passing through an area
This statement, however, is limited, because the electric field fills ALL of space, so that is a continuous \(\infty\) of vectors, no matter what direction the element of area \(dA\) is oriented.
SO... we must agree upon a standard of field line density, somehow.
the dot product of a vector field (in this chapter, the electric field) with an area.
I.e., $$d\vec{E}\cdot\, \hat{n}\,dA$$, in which \(\hat{n}\) encodes the orientation of the infinitesimal tile of surface, \(dA\)
Electric Field due to a Ring of Charge
Hmmmmmmmmmmmm....... will there be time on Friday in lecture?
Draw the electric field for a system of three particles
Hmmmmmmmm.....
field line density
Flux!
The field line diagram of a dipole.
A ubiqitous diagram, very famous, because many molecules, even large ones, have a polar symmetry: a more positive end and a more negative end. Example: \(H_2O\).
vector field diagram of a dipole
The guts of our Quiz 1
and the vectors →ri=ri^rir→i=rir^i{\stackrel{\to }{\textbf{r}}}_{i}={r}_{i}{\hat{\textbf{r}}}_{i} are the displacements from the position of the ith charge to the position of Q.
Covered in lecture, 8/28/23, in my comments about \(\hat{r}_{21}\)
amber
Where we get the word "electric" and "electron."
it will stick to the wall
Or to your head. :D
put the comb close to a thin stream of water
You can easily do this experiment at home. Kinda cool.
n figure (a), a person holding the spinning bike wheel
We normally do this demonstration in lecture on the first day of the semester.
165 km/h
about 103 mph
without the aid of friction between the tires and the road.
This makes the example more of a pin ball machine: give the object some speed than inject it into the "frictionless" track.
