Title: Physics 114C Mechanics Lecture 14 Walker: Ch' 6'24 Strings
1Physics 114C - MechanicsLecture 14 (Walker
Ch. 6.2-4)Strings SpringsOctober 21, 2008
- John G. Cramer
- Professor of Physics
- B451 PAB
- cramer_at_phys.washington.edu
2Announcements
- Homework Assignment 4 is due at 1159 PM on
Thursday, October 23. Homework up to 24 hours
late will receive 70 credit. - There are now 140 out of 167 clicker
registrations. - My office hours are 130-220 PM on Tuesdays and
330-420 PM on Thursdays, both in the 114 area
of the Physics Study Center on the Mezzanine
floor of PAB C (this building). - Tycho now has most of the Exam 1 scores. Check
for underscore grades, which means you did not
write your name on a paper, and you need to see
Susan Hong. I plan to return the Exam 1 pages on
Thursday.
3Exam 1 Statistics
Average 64.5 Std Dev 19.9
High 100 Median 61 Low 11
4Lecture Schedule (Part 2)
5Clicker Question 1
You push two identical bricks across a
tabletop with constant speed v. Which Case, as
shown above, requires more force Fn?
a. F1gtF2 b. F1F2 c. F1ltF2
6Strings
When you pull on a string or rope, it
becomes taut. We say that there is tension in the
string.
7Strings
The tension in a real rope will vary along
its length, due to the weight of the rope.
Here, we will assume that all ropes, strings,
wires, etc. are massless unless otherwise stated.
8The Massless String Approximation
Isolate the string and consider the forces
on it (Fnet)x TA on STB on S mSa,so TA on
S TB on S mSa ¹TB on S
A horizontal force F acts on a block that is
connected to another block by a string.
Consider the constraints and the forces.
Massless String ApproximationAssume that mS0
so that TA on S TB on S
9Pulleys and Ropes
An ideal pulley is one that simply changes
the direction of the tension
10Pulleys
Massless String Approximation
Strings and ropes often pass over pulleys
that change the direction of the tension. In
principle, the friction and inertia in the pulley
could modify the transmitted tension.
Therefore, it is conventional to assume that such
pulleys are massless and frictionless.
Massless and Frictionless Pulley Approximation
11Springs
Spring Force A stretched or compressed
spring exerts one of the most common contact
forces. A spring can either push (when
compressed) or pull (when stretched). In either
case, the tail of the vector force is attached to
the contact point. There is no special symbol for
the spring force, but we can use Fsp.
12Hookes Law for Springs
Hookes law for springs states that the
force increases linearly with the amount the
spring is stretched or compressed
The constant k is called the spring
constant. In the SI system, k has units of N/m
or kg/s2.
13Spring Forces
Hookes law for springs states that the
force increases linearly with the amount the
spring is stretched or compressed. The force is
negative because it always opposes the
compression or extension of the spring.
14Translational Equilibrium
When an object is in translational
equilibrium, the net force on it is zero
This allows the calculation of unknown or
unmeasured forces.
15Translational Equilibrium
A person lifts a bucket of water from the
bottom of a well with a constant speed v.
Because the speed is constant, the acceleration
must be zero, and the net force on the bucket is
zero, so T1 W.
16Clicker Question 2
A
B
In which situation is the tension on the
rope larger?
a. A b. B c. Both tensions are the same
17Example Mountain Climbing (1)
A 90 kg mountain climber is suspended from
ropes as shown. Rope 3 can sustain a maximum
tension of 1500 N before breaking. What is
the smallest that angle q can become before the
rope breaks?
18Example Mountain Climbing (2)
19Connected Objects
When forces are exerted on connected
objects, their accelerations are the same.
If there are two objects connected by a string,
and we know the force and the masses, we can find
the acceleration and the tension
20Connected Objects
We treat each box as a separate system. We
write separate equations for each and solve them
together.
21Connected Objects
If there is a pulley, it is easiest to have
the coordinate system follow the string
22Example Connected Blocks
A block of mass m1 slides on a frictionless
tabletop. It is connected by a string and pulley
to a hanging mass m2. Find the acceleration
a and string tension T.
23Example Connected Masses
A block of mass m1 slides on a frictionless
tabletop. It is connected by a string and pulley
to a hanging mass m2. Find the acceleration
a and string tension T.
24Example Atwoods Machine
Atwoods Machine consists of two masses
connected by a string and pulley. Find the
acceleration a.
25Example Stagecraft (1)
A 200 kg set S used in a play is stored in a
loft above the stage. The rope holding the set
passes up and over a pulley, then is tied
backstage. The director tells a 100 kg stagehand
to lower the set. He unties the set, holds on to
the rope, and is hoisted into the loft. What
is his acceleration? (Assume a massless
rope and a massless frictionless pulley.)
26Example Stagecraft (2)
27Example A Bank Robbery (1)
Bank robbers have pushed a 1,000 kg safe to
a second-story floor-to-ceiling window. The plan
to break the window and lower the safe 3.0 m to
their truck. They stack up 500 kg of furniture,
tie a rope between the safe and the furniture,
place the rope over a pulley, and push the safe
out the window. What is the safes speed
when it hits the truck bed? (Assume mk0.5
between the furniture and the floor.)
28Example A Bank Robbery (2)
29End of Lecture 14
- Before Thursday, read Walker Chapter 6.5
- Homework Assignments 3 should be submitted
using the Tycho system by1159 PM on Thursday,
Oct. 16.(24 hours late Þ 70 credit) - Register your clicker, using the Clicker link
on the Physics 114C Syllabus page.