physics 218: mechanics instructor: dr. tatiana erukhimova sections 818, 819, 820, 821 lecture 11
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Physics 218: Mechanics Instructor: Dr. Tatiana Erukhimova
Sections 818, 819, 820, 821
Lecture 11
Quiz (folders)
A rocket is fired from a tower of height H, at t=0, with an initial velocity of magnitude W at an angle Θ above horizontal. The rocket’s engine supplies an acceleration that increases with time according to a(t)=αt2. The acceleration is always directed at an angle β with the horizontal. The rocket’s fuel runs out after 2 sec. What will its velocity and position be when the fuel runs out? Consider α, β, Θ, H, and W as known constants and neglect gravity.
amF
Newton’s second law
The vector acceleration of an object is in the same direction as the vector force applied to the object and the magnitudes are related by a constant called the mass of the object.
Kinetic Friction
• For kinetic friction, it turns out that the larger the Normal Force the larger the friction. We can write
FFriction = KineticN
Here is a constant• Warning:
– THIS IS NOT A VECTOR EQUATION!
A Recipe for Solving Problems1. Sketch Isolate the body (only external forces but not forces
that one part of the object exert on another part)
2. Write down 2nd Newton’s law
amF
Choose a coordinate system Write 2nd Newton’s law in component form:
yyxx
yxyx
maFmaF
jmaimajFiFF
,
3. Solve for acceleration
Pulling Against FrictionA box of mass m is on a surface with coefficient
of kinetic friction . You pull with constant force FP at angle The box does not leave the surface and moves to the right.
1. What is the magnitude of the acceleration?
2. What angle maximizes the acceleration?
H
Coefficient of friction:
What is the normal force?
What is the velocity of the block when it reaches the bottom?
First exam Tuesday, September 22
102 CHEN
Sections 818 and 819 start at 7 pm
Sections 820 and 821 start at 8:05 pm
All liquids, gels and aerosols must be in three-ounce or smaller containers.
No calculators and cell phones
BRING YOUR STUDENT ID!
What is included?
Chapters 1-6
Kinematics, vectors, Newton’s 2nd Law
Kinematics
dt
Vda
dt
rdV
In components:
dt
dVa
dt
dVa y
yx
x ;
dt
dyV
dt
dxV yx ;
If is given, you can find anda
V
r
daVdtaV yyxx ;
dtVydtVx yx ;
ty
Vectors
jAiAA yx
jBiBB yx
? BAC
jCiCC yx
xxx BAC yyy BAC
Newton’s 2nd Law
amF
xx maF yy maF
Friendly advice
DO NOT…
DO NOT use Const acceleration case formulas when acceleration is a function of time. You have to integrate or differentiate! What are the Const acceleration case formulas?
)0()0(2
1)( 2 xtvtatx c
)0()( vtatv c
))()((2)()( 1212
22 txtxatvtv c
DO NOT write the vector sign over a projection!
!,
,FF
scalarsareFF
jFiIf
yx
yx
DO NOT forget that Fp has two components: Fpcos θ and Fpsin θ
Do Not Forget to
•Write down what is given and express the answer in terms of what is given
•Box the answer
•Indicate the origin and positive x and y
Have a great day!
Reading: Chapter 5,6Hw: Chapter 6 problems and exercises