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SPH4U: Lecture 7 Notes - mjburns.orgmjburns.org/SPH4U/Review Problems ppt.pdf · Page 3...

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Page 1 SPH4U: Practice Problems Today’s Agenda Run and Hide Review: Pegs & Pulleys Used to change the direction of forces An ideal massless pulley or ideal smooth peg will change the direction of an applied force without altering the magnitude: The tension is the same on both sides! F 1 = -T i ideal peg or pulley F 2 = T j | F 1 | = | F 2 | massless rope Problem: Accelerometer A weight of mass m is hung from the ceiling of a car with a massless string. The car travels on a horizontal road, and has an acceleration a in the x direction. The string makes an angle with respect to the vertical (y) axis. Solve for in terms of a and g. a i Accelerometer... Draw a free body diagram for the mass: What are all of the forces acting? m T (string tension) mg (gravitational force) i
Transcript

Page 1

SPH4U: Practice Problems

Today’s Agenda

Run and Hide

Review: Pegs & Pulleys

Used to change the direction of forces

An ideal massless pulley or ideal smooth peg will change the

direction of an applied force without altering the magnitude: The

tension is the same on both sides!

F1 = -T i

ideal peg

or pulley

F2 = T j

| F1 | = | F2 |

massless rope

Problem: Accelerometer

A weight of mass m is hung from the ceiling of a car with a massless

string. The car travels on a horizontal road, and has an acceleration

a in the x direction. The string makes an angle with respect to the

vertical (y) axis. Solve for in terms of a and g.

a

i

Accelerometer...

Draw a free body diagram for the mass:

What are all of the forces acting?

m

T (string tension)

mg (gravitational force)

i

Page 2

Accelerometer...

Using components (recommended):

i: FX = TX = T sin = ma

j: FY = TY - mg

= T cos - mg = 0

T

mg

m

ma

j

i

Accelerometer...

Using components :

i: T sin = ma

j: T cos - mg = 0

Eliminate T : mg

m

ma

T sin = ma

T cos = mgtan

a

g

j

i

T

Accelerometer...

Alternative solution using vectors (elegant but not as systematic):

Find the total vector force FNET:

T

mg

FTOT

m

T (string tension)

mg (gravitational force)

Accelerometer...

Alternative solution using vectors (elegant but not as systematic):

Find the total vector force FNET:

Recall that FNET = ma:

So

ma

tanma a

mg g

T

mg

tana

g

m

T (string tension)

mg (gravitational force)

Page 3

Accelerometer...

Let’s put in some numbers:

Say the car goes from 0 to 60 mph in 10 seconds:

60 mph = 60 x 0.45 m/s = 27 m/s.

Acceleration a = Δv/Δt = 2.7 m/s2.

So a/g = 2.7 / 9.8 = 0.28 .

= arctan (a/g) = 15.6 deg

tana

g

a

Understanding

A person standing on a horizontal floor feels two forces: the

downward pull of gravity and the upward supporting force from the

floor. These two forces

(A) Have equal magnitudes and form an action/reaction pair

(B) Have equal magnitudes but do not form an action/reaction pair

(C) Have unequal magnitudes and form an action/reaction pair

(D) Have unequal magnitudes and do not form an action/reaction pair

(E) None of the above

Because the person is not accelerating, the net force they feel is

zero. Therefore the magnitudes must be the same (opposite

directions. These are not action/reaction forces because they act of

the same object (the person). Action/Reaction pairs always act on

different objects.

Angles of an Inclined plane

ma = mg sin

mg

N

The triangles are similar, so the angles are the same!

Problem: Inclined plane

A block of mass m slides down a frictionless ramp that

makes angle with respect to the horizontal. What is its

acceleration a ?

ma

Page 4

Inclined plane...

Define convenient axes parallel and perpendicular to plane:

Acceleration a is in x direction only.

ma

i

j

Inclined plane...

Consider x and y components separately:

i: mg sin = ma. a = g sin

j: N - mg cos = 0. N = mg cos

mg

N

mg sin

mg cos

ma

i

j

Problem: Two Blocks

Two blocks of masses m1 and m2 are placed in contact on a

horizontal frictionless surface. If a force of magnitude F is applied to

the box of mass m1, what is the force on the block of mass m2?

m1 m2

F

Problem: Two Blocks Realize that F = (m1+ m2) a :

Draw FBD of block m2 and apply FNET = ma:

F2,1F2,1 = m2 a

F / (m1+ m2) = a

m22,1 ( )

+

m2m1

FF

Substitute for a :

m2

(m1 + m2)

m2F2,1 F

Page 5

Problem: Tension and Angles

A box is suspended from the ceiling by two ropes making

an angle with the horizontal. What is the tension in each

rope?

m

Problem: Tension and Angles

Draw a FBD:

T1 T2

mg

Since the box isn’t going anywhere, Fx,NET = 0 and Fy,NET = 0

T1sin T2sin

T2cos T1cos

j

i

Fx,NET = T1cos - T2cos = 0 T1 = T2

2 sin

mgT1 = T2 =Fy,NET = T1sin + T2sin - mg = 0

Problem: Motion in a Circle

A boy ties a rock of mass m to the end of a string and twirls

it in the vertical plane. The distance from his hand to the

rock is R. The speed of the rock at the top of its trajectory is

v.

What is the tension T in the string at the top of the rock’s

trajectory?

R

v

T

Motion in a Circle...

Draw a Free Body Diagram (pick y-direction to be down):

We will use FNET = ma (surprise)

First find FNET in y direction:

FNET = mg +T T

mg

y

Page 6

Motion in a Circle...

FNET = mg +T

Acceleration in y direction:

ma = mv2 / R

mg + T = mv2 / R

T = mv2 / R - mg

R

T

v

mg

y

F = ma

Motion in a Circle...

What is the minimum speed of the mass at the top of the trajectory such that the string does not go limp?

i.e. find v such that T = 0.

mv2 / R = mg + T

v2 / R = g

Notice that this doesnot depend on m.

R

mg

v

T= 0

v Rg

Understanding

Two-body dynamics

In which case does block m experience a larger acceleration?

In case (1) there is a 10 kg mass hanging from a rope. In

case (2) a hand is providing a constant downward force of

98.1 N. In both cases the ropes and pulleys are massless.

(a) Case (1) (b) Case (2) (c) same

m

10kg

a a

m

F = 98.1 N

Case (1) Case (2)

Solution

m

10kg

a

Add (a) and (b):

mWg = (m + mW)a

W

W

m ga

m m

+

(a)

(b)

T = ma (a)

mWg -T = mWa (b)

For case (1) draw FBD and write FNET = ma for each block:

mW=10kg

Page 7

Solution

The answer is (b) Case (2). In this case the block experiences a larger acceleration

98.1Na

mT = 98.1 N = ma For case (2)

m

10kg

a

Case (1)

kg10m

N198a

+

.

m

a

F = 98.1 N

Case (2)

m

N198a

.

Problem: Two strings & Two Masses on

horizontal frictionless floor:

m2 m1T2 T1

Given T1, m1 and m2, what are a and T2?

T1 - T2 = m1a (a)

T2 = m2a (b)

Add (a) + (b):

T1 = (m1 + m2)a a

a

i

1

1 2

T

m m

+

Plugging solution into (b): 22 1

1 2

mT T

m m

+

Understanding

Two-body dynamics

Three blocks of mass 3m, 2m, and m are

connected by strings and pulled with constant

acceleration a. What is the relationship between

the tension in each of the strings?

(a) T1 > T2 > T3 (b) T3 > T2 > T1 (c) T1 = T2 = T3

T3 T2 T13m2m m

a

Solution

Draw free body diagrams!!

T33mT3 = 3ma

T3 T22m

T2 - T3 = 2ma

T2 = 2ma +T3 > T3

T2 T1m

T1 - T2 = ma

T1 = ma + T2 > T2

T1 > T2 > T3

Page 8

Alternative Solution

T3 T2 T13m 2m m

a

Consider T1 to be pulling all the boxes

T3 T2 T13m 2m m

a

T2 is pulling only the boxes of mass 3m and 2m

T3 T2 T13m 2m m

a

T3 is pulling only the box of mass 3m

T1 > T2 > T3

Problem: Rotating puck & weight.

A mass m1 slides in a circular path with speed v

on a horizontal frictionless table. It is held at a

radius R by a string threaded through a

frictionless hole at the center of the table. At the

other end of the string hangs a second mass m2.

What is the tension (T) in the string?

What is the speed (v) of the sliding mass?

m1

m2

v

R

Problem: Rotating puck & weight...

Draw FBD of hanging mass:

Since R is constant, a = 0.

so T = m2g

m2

m2g

T

m1

m2

v

R

T

Problem: Rotating puck & weight...

Draw FBD of sliding mass:m1

T = m2g

2

1

mv gR

m

m1g

N

m1

m2

v

R

T

Use F = T = m1a

where a = v2 / R

m2g = m1v2 / R

T = m2g


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