Coordination
between 303K lectures and 103M lab
1.
103M lab schedule
Week of lab Lab Subject Lecture
Topic
|
Sep. 3
|
-
|
no lab
|
Vectors, Motion in 1-Dimension
|
|
Sep. 10
|
|
Introduction
|
1-D & 2-D Motion
|
|
Sep. 17
|
1
|
Random Motion
|
Laws of Motion
|
|
Sep. 24
|
2
|
Uniformly Accelerated Motion
|
Circ. Motion & Newton Laws
|
|
Oct. 1
|
3
|
Force and Potential Energy
|
Work & Energy
|
|
Oct. 8
Oct. 15
|
4
|
Collisions in One Dimensional
Motion
|
Linear Momentum & Collisions
Rotation, Ang. Mom,
Torque
|
|
Oct. 22
|
5
|
Motion Under a Central Force
|
Rolling, more on Ang. Mom.
|
|
Oct. 29
Nov. 5
|
6
|
A Mechanical Oscillator
|
Oscillatory Motion: SHM …
Fluid Mechanis
|
|
Nov. 12
|
7
|
Bernoulli's Principle
|
Wave-motion + Sound-waves
|
|
Nov. 19
|
-
|
no lab--Thanksgiving
|
Sound + Superposition Waves
|
|
Nov. 26
|
8
|
Sound
|
Standing Waves + Gravity
|
|
Dec. 3
|
*
|
Make-Up Week
|
Gravity
|
2.
303K course-materials which are specifically related to 103M-labs
Although Physics 303K and Physics 103M lab are two independent courses, we
plan to have our 303K lectures support the 103M lab in following way. We will
give instructors and TAs of 303K a copy of the 103M lab manual, and ask them to
make reference to the on-going experiments in 103M. Different instructors could do it differently. Below is one
scenario which we have worked out to illustrate how this cross reference
may be done. (The labels of equations and chapters given below are based on the
current textbook, i.e. the 5th edition of Serway.)
- Experiment 2: Uniform
acceleration. During the class-period when we begin chapter 5 (which
will be one week before the experiment-week), we plan to mention
the incline plane problem of example 5.6 of Sec. 5.7. We will show that
the relationship: a=gsinq, which
is the basic expression used in this experiment.
- Experiment 3: Force
and potential energy. The
basic equation here is F=-dU/dx, where U is the potential energy function.
We plan to group chapter 7 and chapter 8 together under the heading of:
"applications of the work-energy theorem" Ei->f=Kf-Ki +Uf-Ui + Di->f.
See eq. 8.15 in Sec. 8.5. To provide a timely support to this experiment,
we plan to consider the special of case of “motion along an inclined
plane” right away, which is about one week before the experiment,
that DE=FDx= -DU, with x being along the direction
parallel to the incline plane.
This leads to the basic equation mentioned above, that F=-dU/dx,
- Experiment 4: Collisions
in one dimension. This experiment verifies the law of
conservation of linear momentum in one dimensional collisions. The theory
of conservation of linear momentum in a collision processes is discussed
in Sec. 9.1 through 9.4. Notice that this is the only case where the
lecture will be slightly lagging behind the lab. We plan to mention this
experiment in the very first lecture of chapter 9.
- Experiment 5: Motion
under a central force. In this experiment an air puck is moving under
the influence of a "central force". Through careful
measurements, one verifies to what extent the angular momentum of this
motion is conserved. During the lecture, after we have arrived at eq. 10.21
of section 10.7, (about one week before the experiment) we plan to
make a digression in the following way.
- Analogous to the
linear motion case, where the ”force equations” are given by
F=ma=d(mv)/dt=dp/dt, for the rotation case there is the corresponding
“the torque equations” are given by: i.e. t=Ia=d(Iw)/dt=dL/dt.
- The lesson here is
that when there is no "external" torque applied to a rotating
system, the angular momentum of the system is conserved, i.e. L=
constant.
- We plan to further digress
to consider the motion of a point-mass under the influence of a central
force F. The torque exerted on this mass is given by t=r x F, see eq.
11.7. For a central force, this cross product vanishes. So the torque
vanishes, or the corresponding angular momentum is constant. This is the
underlining theory of the experiment.
- Experiment 6: A
mechanical oscillation. In this lab an air puck is connected to a
spring system. One verifies whether the motion follows a SHM. A reference
to this experiment can be made in the first class of chapter 13.
- Experiment 7: Bernoulli's
principle. The goal in
chapter 15 is mainly to cover Bernoulli's principle and those concepts in
fluid mechanics necessary for leading up to this principle. We plan to
discuss this chapter and make reference to this experiment during the
week before the experiment.
- Experiment 8: Sound.
The chapter on sound will be covered one week before the experiment.