Day 29 - Calculus of Variations

Day 29 - Calculus of Variations#

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Announcements#

  • Midterm 2 is posted (Due 14 November 2025 at 11:59 pm)

  • Office Hours this week: Midterm 2 Help

Seminars this Week#

MONDAY, November 3, 2025#

Condensed Matter Seminar 4:10 pm,1400 BPS, In Person and Zoom, Host ~ Philip Crowley Speaker: Chaitanya Murthy, University of Rochester
Title: A modified interferometer to measure anyonic braiding statistics Zoom Link: https://msu.zoom.us/j/93613644939 Meeting ID: 936 1364 4939 Password: CMP

Seminars this Week#

TUESDAY, November 4, 2025#

High Energy Physics Seminar, 1:30 pm, 1400 BPS, Host~ Joshua Isaacson
Speaker: Mareen Hoppe, Technische Universität Dresden Title: Simulating polarization effects in Monte-Carlo event generators
Organized by: Joey Huston, Sophie Berkman and Brenda Wenzlick

Seminars this Week#

WEDNESDAY, November 5, 2025#

Astronomy Seminar, 1:30 pm, 1400 BPS, In Person and Zoom, Host~ Speaker: Nick Konidaris, Carnegie Observatories Title: The Sephira Project: Astronomical Imaging with Third-Order Intensity Correlations

Seminars this Week#

WEDNESDAY, November 5, 2025#

FRIB Nuclear Science Seminar, 3:30pm., FRIB 1300 Auditorium and online via Zoom Speaker: Assistant Professor Xing Wu of The Facility for Rare Isotope Beams (FRIB)
Title: Towards Quantum Control and Sensing of 227ThO Molecules and Other Radioactive Molecules for Nuclear Schiff Moment Search Please click the link below to join the webinar: Join Zoom Meeting: https://msu.zoom.us/j/91861947571?pwd=IlUS6RkYdHibaosm4aznsYsctbaMrU.1 Meeting ID: 939 4416 7137 Passcode: 026775

Seminars this Week#

THURSDAY, November 6, 2025#

Colloquium, 3:30 pm, 1415 BPS, in person and zoom. Host ~ Jay Strader/Laura Chomiuk Refreshments and social half-hour in BPS 1400 starting at 3 pm Speaker: Nick Konidaris, Carnegie Observations Title: SDSS Local Volume Mapper instrument and Early Science Results

Seminars this Week#

FRIDAY, November 7, 2025#

IReNA Online Seminar, 9:00am, In Person and Zoom, FRIB 2025 Nuclear Conference Room, Light refreshments will be served at 1:50pm. Hosted by: Sota Kimura (University of Tsukuba) Speaker Tomoshi Takeda, Hiroshima University, Japan Title: A New Approach to X-ray Astronomy: Development and Observational Results of the CubeSat Observatory NinjaSat

Seminars this Week#

FRIDAY, November 7, 2025#

Special HEP Seminar High Energy Physics Seminar, 1:00 pm, 1400 BPS, Host~ Joey Huston Speaker: Eric Bachmann, Technische Universität Dresden Title: Evidence for longitudinal polarization in same-sign WW scattering with the ATLAS detector
Organized by: Joey Huston, Sophie Berkman and Brenda Wenzlick

Seminars this Week#

FRIDAY, November 7, 2025#

QuIC Seminar, 12:30pm, -1:30pm, 1300 BPS, Virtual only today
Speaker: Philip Crowley, MSU Title: Quantum dynamics for quantum sensing Full Scheule is at: https://sites.google.com/msu.edu/quic-seminar/ For more information, reach out to Ryan LaRose

Calculus of Variations#

Variational calculus is a mathematical method to find functions that optimize a certain quantity. We will use variational calculus to derive the Euler-Lagrange equations for a set of generalized coordinates (i.e., \(q,\dot{q}\)). This is fundamental to Lagrangian mechanics.

\[L(q, \dot{q}, t) = T(\dot{q}) - U({q})\]
\[S = \int_{t_1}^{t_2} L(q, \dot{q}, t) \, dt \qquad \delta S = 0 \]
\[ \dfrac{d}{dt} \left( \dfrac{\partial L}{\partial \dot{q}} \right) - \dfrac{\partial L}{\partial q} = 0 \]

Clicker Question 30-1#

The generic segment, \(ds\), of a curve in 2D Cartesian coordinates is given by

\[ds = \sqrt{(dx)^2 + (dy)^2}\]

The integral of \(ds\) from \(s_1\) to \(s_2\) gives the length of the curve, \(l\). What is the correct expression for \(l\)?

  1. \(l = \int_{s_1}^{s_2} ds\)

  2. \(l = \int_{s_1}^{s_2} \sqrt{(dx)^2 + (dy)^2}\)

  3. \(l = \int_{s_1}^{s_2} \sqrt{1 + (dy/dx)^2} \, dx\)

  4. \(l = \int_{s_1}^{s_2} \sqrt{(dx/dy)^2 + 1} \, dy\)

  5. More than one of the above

Clicker Question 30-2#

I can explain why:

\[\int_{s_1}^{s_2} f((Y(x), Y'(x), x) \, dx > \int_{s_1}^{s_2} f((y(x), y'(x), x) \, dx\]

where \(Y(x) = y(x) + \alpha \eta(x)\), the true path plus an error term.

  1. Yes, I can explain why

  2. I think I can explain why

  3. I’m having trouble seeing why

  4. I don’t think I can explain why

Clicker Question 30-3#

For the function \(Y(x) = y(x) + \alpha \eta(x)\), where \(y(x)\) is the true path, \(\eta(x)\) is a small error term, and \(\alpha\) is a small parameter, what is the derivative of \(Y(x)\) with respect to \(\alpha\)?

\[\frac{dY}{d\alpha} = ?\]

  1. \(y(x)\)

  2. \(\eta(x)\)

  3. \(\eta'(x)\)

  4. \(\alpha \eta(x)\)

  5. \(y'(x) + \alpha \eta'(x)\)

Clicker Question 30-4#

For the function \(Y'(x) = y'(x) + \alpha \eta'(x)\), what is the derivative of \(Y'(x)\) with respect to \(\alpha\)?

\[\frac{dY'}{d\alpha} = ?\]

  1. \(y'(x)\)

  2. \(\eta'(x)\)

  3. \(\eta''(x)\)

  4. \(\alpha \eta'(x)\)

  5. \(y''(x) + \alpha \eta''(x)\)

Clicker Question 30-5#

The “surface term” that we computed for \(\int_{s_1}^{s_2} \eta'(x) \frac{df}{dy'} dx\) is:

\[\left[\eta(x)\dfrac{df}{dy'}\right]_{x_1}^{x_2}=0\]

I can explain why this surface term is equal to zero:

  1. Yes, I can explain why

  2. I think I can explain why

  3. I’m having trouble seeing why

  4. I don’t think I can explain why

  5. I don’t know what a surface term is

Clicker Question 30-6#

We completed this derivation with the following mathematical statement:

\[\int_{s_1}^{s_2} \eta(x) \left[\dfrac{\partial f}{\partial y} - \dfrac{d}{dx}\left(\dfrac{\partial f}{\partial y'}\right)\right] = 0\]

where \(\eta(x)\) is an arbitrary function. What does this imply about the term in square brackets?

  1. The term in square brackets must be a pure function of \(x\).

  2. The term in square brackets must be a pure function of \(y\).

  3. The term in square brackets must be a pure function of \(y'\).

  4. The term in square brackets must be zero.

  5. The term in square brackets must be a non-zero constant.

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