Centripetal Force Examples

39
Centripetal Force Examples Physics 6A Prepared by Vince Zaccone For Campus Learning Assistance Services at

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Centripetal Force Examples. Physics 6A. Prepared by Vince Zaccone For Campus Learning Assistance Services at UCSB. Ride your bike around a curve and you will notice that if you go too fast, your tires will slip and you will fall. Why does this happen?. Prepared by Vince Zaccone - PowerPoint PPT Presentation

Transcript of Centripetal Force Examples

Page 1: Centripetal Force Examples

Centripetal Force Examples

Physics 6A

Prepared by Vince Zaccone

For Campus Learning Assistance Services at UCSB

Page 2: Centripetal Force Examples

Prepared by Vince Zaccone

For Campus Learning Assistance Services at UCSB

Ride your bike around a curve and you will notice that if you go too fast, your tires will slip and you will fall.

Why does this happen?

Page 3: Centripetal Force Examples

Prepared by Vince Zaccone

For Campus Learning Assistance Services at UCSB

Ride your bike around a curve and you will notice that if you go too fast, your tires will slip and you will fall.

Why does this happen?

Static friction is not strong enough to keep your tires from slipping on the pavement.

Page 4: Centripetal Force Examples

Prepared by Vince Zaccone

For Campus Learning Assistance Services at UCSB

v2)d

v2)c

v)b2

v)a

Ride your bike around a curve and you will notice that if you go too fast, your tires will slip and you will fall.

Why does this happen?

Static friction is not strong enough to keep your tires from slipping on the pavement.

OK, let’s say you are riding your bike around a level curve and your maximum speed is v when the radius of the curve is R. Here are a couple of multiple choice questions:

1) What is your maximum speed if the radius of the curve is 2R?

Page 5: Centripetal Force Examples

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We will need to find a formula relating v and R. A diagram may help.

Ride your bike around a curve and you will notice that if you go too fast, your tires will slip and you will fall.

Why does this happen?

Static friction is not strong enough to keep your tires from slipping on the pavement.

OK, let’s say you are riding your bike around a level curve and your maximum speed is v when the radius of the curve is R. Here are a couple of multiple choice questions:

1) What is your maximum speed if the radius of the curve is 2R?

v2)d

v2)c

v)b2

v)a

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We will need to find a formula relating v and R. A diagram may help.

friction

View from aboveNotice that the friction force points toward the center of the curve. It is the centripetal force.

Ride your bike around a curve and you will notice that if you go too fast, your tires will slip and you will fall.

Why does this happen?

Static friction is not strong enough to keep your tires from slipping on the pavement.

OK, let’s say you are riding your bike around a level curve and your maximum speed is v when the radius of the curve is R. Here are a couple of multiple choice questions:

1) What is your maximum speed if the radius of the curve is 2R?

v2)d

v2)c

v)b2

v)a

Page 7: Centripetal Force Examples

Prepared by Vince Zaccone

For Campus Learning Assistance Services at UCSB

Ride your bike around a curve and you will notice that if you go too fast, your tires will slip and you will fall.

Why does this happen?

Static friction is not strong enough to keep your tires from slipping on the pavement.

OK, let’s say you are riding your bike around a level curve and your maximum speed is v when the radius of the curve is R. Here are a couple of multiple choice questions:

1) What is your maximum speed if the radius of the curve is 2R?We will need to find a formula relating v and R. A diagram may help.

friction

View from aboveNotice that the friction force points toward the center of the curve. It is the centripetal force.

R

mvfriction

2

We know a formula for friction as well:

R

vmmg

2max

s Maximum static friction will give maximum speed.

v2)d

v2)c

v)b2

v)a

Page 8: Centripetal Force Examples

Prepared by Vince Zaccone

For Campus Learning Assistance Services at UCSB

Ride your bike around a curve and you will notice that if you go too fast, your tires will slip and you will fall.

Why does this happen?

Static friction is not strong enough to keep your tires from slipping on the pavement.

OK, let’s say you are riding your bike around a level curve and your maximum speed is v when the radius of the curve is R. Here are a couple of multiple choice questions:

1) What is your maximum speed if the radius of the curve is 2R?We will need to find a formula relating v and R. A diagram may help.

friction

View from aboveNotice that the friction force points toward the center of the curve. It is the centripetal force.

R

mvfriction

2

We know a formula for friction as well:

R

vmmg

2max

s Maximum static friction will give maximum speed.

gRv smax Solve for vmax

v2)d

v2)c

v)b2

v)a

Page 9: Centripetal Force Examples

Prepared by Vince Zaccone

For Campus Learning Assistance Services at UCSB

Ride your bike around a curve and you will notice that if you go too fast, your tires will slip and you will fall.

Why does this happen?

Static friction is not strong enough to keep your tires from slipping on the pavement.

OK, let’s say you are riding your bike around a level curve and your maximum speed is v when the radius of the curve is R. Here are a couple of multiple choice questions:

1) What is your maximum speed if the radius of the curve is 2R?We will need to find a formula relating v and R. A diagram may help.

friction

View from aboveNotice that the friction force points toward the center of the curve. It is the centripetal force.

R

mvfriction

2

We know a formula for friction as well:

R

vmmg

2max

s Maximum static friction will give maximum speed.

gRv smax Solve for vmax

If R is doubled, vmax increases by √2

v2)d

v2)c

v)b2

v)a

Page 10: Centripetal Force Examples

Prepared by Vince Zaccone

For Campus Learning Assistance Services at UCSB

Ride your bike around a curve and you will notice that if you go too fast, your tires will slip and you will fall.

Why does this happen?

Static friction is not strong enough to keep your tires from slipping on the pavement.

OK, let’s say you are riding your bike around a curve and your maximum speed is v when the radius of the curve is R. Here are a couple of multiple choice questions:

1) What is your maximum speed if the radius of the curve is 2R?

2) What is your maximum speed if the radius is R, but the road is wet, so that your coefficient of static friction is only 1/3 of the value when the road is dry?

v3)d

v3)c

3

v)b

3

v)a

v2)d

v2)c

v)b2

v)a

Page 11: Centripetal Force Examples

Prepared by Vince Zaccone

For Campus Learning Assistance Services at UCSB

Ride your bike around a curve and you will notice that if you go too fast, your tires will slip and you will fall.

Why does this happen?

Static friction is not strong enough to keep your tires from slipping on the pavement.

OK, let’s say you are riding your bike around a curve and your maximum speed is v when the radius of the curve is R. Here are a couple of multiple choice questions:

1) What is your maximum speed if the radius of the curve is 2R?

2) What is your maximum speed if the radius is R, but the road is wet, so that your coefficient of static friction is only 1/3 of the value when the road is dry?

v3)d

v3)c

3

v)b

3

v)a

v2)d

v2)c

v)b2

v)a

We can use our formula from part 1) gRv smax

Page 12: Centripetal Force Examples

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For Campus Learning Assistance Services at UCSB

Ride your bike around a curve and you will notice that if you go too fast, your tires will slip and you will fall.

Why does this happen?

Static friction is not strong enough to keep your tires from slipping on the pavement.

OK, let’s say you are riding your bike around a curve and your maximum speed is v when the radius of the curve is R. Here are a couple of multiple choice questions:

1) What is your maximum speed if the radius of the curve is 2R?

2) What is your maximum speed if the radius is R, but the road is wet, so that your coefficient of static friction is only 1/3 of the value when the road is dry?

v3)d

v3)c

3

v)b

3

v)a

v2)d

v2)c

v)b2

v)a

We can use our formula from part 1) gRv smax

If µs decreases to µs/3 then vmax will decrease by √3.

Page 13: Centripetal Force Examples

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Wheel of Doom!

This carnival ride is a giant metal cylinder which will spin around and pin the occupants to the wall. The fun part is when the floor drops out from below and the patrons see a spike-filled pit of angry crocodiles awaiting them should they fall. As safety inspector, your problem will be to determine when it will be unsafe to ride. The given information is this: Radius of cylinder = 20m. Speed of rotation = 10 rpm.

a) Will leather-clad Biker Bob (mass = 100kg ;coeff. of static friction = 0.6) be safe?

b) How about Disco Stu, a 75kg man wearing a silk shirt and polyester pants (µs=0.15)?

Page 14: Centripetal Force Examples

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We can start by drawing a free-body diagram of the forces on the person.

Wheel of Doom!

This carnival ride is a giant metal cylinder which will spin around and pin the occupants to the wall. The fun part is when the floor drops out from below and the patrons see a spike-filled pit of angry crocodiles awaiting them should they fall. As safety inspector, your problem will be to determine when it will be unsafe to ride. The given information is this: Radius of cylinder = 20m. Speed of rotation = 10 rpm.

a) Will leather-clad Biker Bob (mass = 100kg ;coeff. of static friction = 0.6) be safe?

b) How about Disco Stu, a 75kg man wearing a silk shirt and polyester pants (µs=0.15)?

Page 15: Centripetal Force Examples

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We can start by drawing a free-body diagram of the forces on the person.

mg

Normal

friction

The normal force is the force of the wall pushing inward. This is a centripetal force (it points toward the center of the circle).

Wheel of Doom!

This carnival ride is a giant metal cylinder which will spin around and pin the occupants to the wall. The fun part is when the floor drops out from below and the patrons see a spike-filled pit of angry crocodiles awaiting them should they fall. As safety inspector, your problem will be to determine when it will be unsafe to ride. The given information is this: Radius of cylinder = 20m. Speed of rotation = 10 rpm.

a) Will leather-clad Biker Bob (mass = 100kg ;coeff. of static friction = 0.6) be safe?

b) How about Disco Stu, a 75kg man wearing a silk shirt and polyester pants (µs=0.15)?

Page 16: Centripetal Force Examples

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For Campus Learning Assistance Services at UCSB

We can start by drawing a free-body diagram of the forces on the person.

mg

Normal

friction

The normal force is the force of the wall pushing inward. This is a centripetal force (it points toward the center of the circle).

We can write down our formula for centripetal force:

R

mvN

R

mvF

2

2

cent

Wheel of Doom!

This carnival ride is a giant metal cylinder which will spin around and pin the occupants to the wall. The fun part is when the floor drops out from below and the patrons see a spike-filled pit of angry crocodiles awaiting them should they fall. As safety inspector, your problem will be to determine when it will be unsafe to ride. The given information is this: Radius of cylinder = 20m. Speed of rotation = 10 rpm.

a) Will leather-clad Biker Bob (mass = 100kg ;coeff. of static friction = 0.6) be safe?

b) How about Disco Stu, a 75kg man wearing a silk shirt and polyester pants (µs=0.15)?

Page 17: Centripetal Force Examples

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For Campus Learning Assistance Services at UCSB

We can start by drawing a free-body diagram of the forces on the person.

mg

Normal

friction

The vertical forces must balance out if the person wants to avoid the crocodile pit, so we can write down a formula:

mgfriction

What type of friction do we want – static or kinetic?

Wheel of Doom!

This carnival ride is a giant metal cylinder which will spin around and pin the occupants to the wall. The fun part is when the floor drops out from below and the patrons see a spike-filled pit of angry crocodiles awaiting them should they fall. As safety inspector, your problem will be to determine when it will be unsafe to ride. The given information is this: Radius of cylinder = 20m. Speed of rotation = 10 rpm.

a) Will leather-clad Biker Bob (mass = 100kg ;coeff. of static friction = 0.6) be safe?

b) How about Disco Stu, a 75kg man wearing a silk shirt and polyester pants (µs=0.15)?

Page 18: Centripetal Force Examples

Prepared by Vince Zaccone

For Campus Learning Assistance Services at UCSB

We can start by drawing a free-body diagram of the forces on the person.

mg

Normal

friction

The vertical forces must balance out if the person wants to avoid the crocodile pit, so we can write down a formula:

mgN

mgfriction

s

By putting the maximum force of static friction in our formula, we are assuming the man is just on the verge of sliding.

Wheel of Doom!

This carnival ride is a giant metal cylinder which will spin around and pin the occupants to the wall. The fun part is when the floor drops out from below and the patrons see a spike-filled pit of angry crocodiles awaiting them should they fall. As safety inspector, your problem will be to determine when it will be unsafe to ride. The given information is this: Radius of cylinder = 20m. Speed of rotation = 10 rpm.

a) Will leather-clad Biker Bob (mass = 100kg ;coeff. of static friction = 0.6) be safe?

b) How about Disco Stu, a 75kg man wearing a silk shirt and polyester pants (µs=0.15)?

Page 19: Centripetal Force Examples

Prepared by Vince Zaccone

For Campus Learning Assistance Services at UCSB

We can start by drawing a free-body diagram of the forces on the person.

mg

Normal

friction

The vertical forces must balance out if the person wants to avoid the crocodile pit, so we can write down a formula:

mgR

mv

mgN

mgfriction

2

s

s

We can replace N with the expression we found earlier.

Wheel of Doom!

This carnival ride is a giant metal cylinder which will spin around and pin the occupants to the wall. The fun part is when the floor drops out from below and the patrons see a spike-filled pit of angry crocodiles awaiting them should they fall. As safety inspector, your problem will be to determine when it will be unsafe to ride. The given information is this: Radius of cylinder = 20m. Speed of rotation = 10 rpm.

a) Will leather-clad Biker Bob (mass = 100kg ;coeff. of static friction = 0.6) be safe?

b) How about Disco Stu, a 75kg man wearing a silk shirt and polyester pants (µs=0.15)?

Page 20: Centripetal Force Examples

Prepared by Vince Zaccone

For Campus Learning Assistance Services at UCSB

We can start by drawing a free-body diagram of the forces on the person.

mg

Normal

friction

The vertical forces must balance out if the person wants to avoid the crocodile pit, so we can write down a formula:

gR

v

mgR

mv

mgN

mgfriction

2

s

2

s

s

Now that we have this formula, how do we use it?

Wheel of Doom!

This carnival ride is a giant metal cylinder which will spin around and pin the occupants to the wall. The fun part is when the floor drops out from below and the patrons see a spike-filled pit of angry crocodiles awaiting them should they fall. As safety inspector, your problem will be to determine when it will be unsafe to ride. The given information is this: Radius of cylinder = 20m. Speed of rotation = 10 rpm.

a) Will leather-clad Biker Bob (mass = 100kg ;coeff. of static friction = 0.6) be safe?

b) How about Disco Stu, a 75kg man wearing a silk shirt and polyester pants (µs=0.15)?

Page 21: Centripetal Force Examples

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For Campus Learning Assistance Services at UCSB

We can start by drawing a free-body diagram of the forces on the person.

mg

Normal

friction

The vertical forces must balance out if the person wants to avoid the crocodile pit, so we can write down a formula:

2s

2

s

2

s

s

v

gR

gR

v

mgR

mv

mgN

mgfriction

Notice that the mass canceled out, so based on the given information we should solve for µ.

Wheel of Doom!

This carnival ride is a giant metal cylinder which will spin around and pin the occupants to the wall. The fun part is when the floor drops out from below and the patrons see a spike-filled pit of angry crocodiles awaiting them should they fall. As safety inspector, your problem will be to determine when it will be unsafe to ride. The given information is this: Radius of cylinder = 20m. Speed of rotation = 10 rpm.

a) Will leather-clad Biker Bob (mass = 100kg ;coeff. of static friction = 0.6) be safe?

b) How about Disco Stu, a 75kg man wearing a silk shirt and polyester pants (µs=0.15)?

Page 22: Centripetal Force Examples

Prepared by Vince Zaccone

For Campus Learning Assistance Services at UCSB

We can start by drawing a free-body diagram of the forces on the person.

mg

Normal

friction

The vertical forces must balance out if the person wants to avoid the crocodile pit, so we can write down a formula:

2s

2

s

2

s

s

v

gR

gR

v

mgR

mv

mgN

mgfriction

The radius and speed are given, but the speed is in rpm, so we will need to convert it to m/s.

Wheel of Doom!

This carnival ride is a giant metal cylinder which will spin around and pin the occupants to the wall. The fun part is when the floor drops out from below and the patrons see a spike-filled pit of angry crocodiles awaiting them should they fall. As safety inspector, your problem will be to determine when it will be unsafe to ride. The given information is this: Radius of cylinder = 20m. Speed of rotation = 10 rpm.

a) Will leather-clad Biker Bob (mass = 100kg ;coeff. of static friction = 0.6) be safe?

b) How about Disco Stu, a 75kg man wearing a silk shirt and polyester pants (µs=0.15)?

Page 23: Centripetal Force Examples

Prepared by Vince Zaccone

For Campus Learning Assistance Services at UCSB

We can start by drawing a free-body diagram of the forces on the person.

mg

Normal

friction

The vertical forces must balance out if the person wants to avoid the crocodile pit, so we can write down a formula:

2s

2

s

2

s

s

v

gR

gR

v

mgR

mv

mgN

mgfriction

The radius and speed are given, but the speed is in rpm, so we will need to convert it to m/s.

sm21

rev

m202

sec60

min1

min

rev10

Wheel of Doom!

This carnival ride is a giant metal cylinder which will spin around and pin the occupants to the wall. The fun part is when the floor drops out from below and the patrons see a spike-filled pit of angry crocodiles awaiting them should they fall. As safety inspector, your problem will be to determine when it will be unsafe to ride. The given information is this: Radius of cylinder = 20m. Speed of rotation = 10 rpm.

a) Will leather-clad Biker Bob (mass = 100kg ;coeff. of static friction = 0.6) be safe?

b) How about Disco Stu, a 75kg man wearing a silk shirt and polyester pants (µs=0.15)?

Page 24: Centripetal Force Examples

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For Campus Learning Assistance Services at UCSB

We can start by drawing a free-body diagram of the forces on the person.

mg

Normal

friction

The vertical forces must balance out if the person wants to avoid the crocodile pit, so we can write down a formula:

44.0

21

m208.9

v

gR

gR

v

mgR

mv

mgN

mgfriction

2

sm

sm

s

2s

2

s

2

s

s

2

Substitute the values for g, R and v

Wheel of Doom!

This carnival ride is a giant metal cylinder which will spin around and pin the occupants to the wall. The fun part is when the floor drops out from below and the patrons see a spike-filled pit of angry crocodiles awaiting them should they fall. As safety inspector, your problem will be to determine when it will be unsafe to ride. The given information is this: Radius of cylinder = 20m. Speed of rotation = 10 rpm.

a) Will leather-clad Biker Bob (mass = 100kg ;coeff. of static friction = 0.6) be safe?

b) How about Disco Stu, a 75kg man wearing a silk shirt and polyester pants (µs=0.15)?

Page 25: Centripetal Force Examples

Prepared by Vince Zaccone

For Campus Learning Assistance Services at UCSB

We can start by drawing a free-body diagram of the forces on the person.

mg

Normal

friction

The vertical forces must balance out if the person wants to avoid the crocodile pit, so we can write down a formula:

44.0

21

m208.9

v

gR

gR

v

mgR

mv

mgN

mgfriction

2

sm

sm

s

2s

2

s

2

s

s

2

So if the coefficient is 0.44 the person will be on the verge of sliding down into the pit.

Wheel of Doom!

This carnival ride is a giant metal cylinder which will spin around and pin the occupants to the wall. The fun part is when the floor drops out from below and the patrons see a spike-filled pit of angry crocodiles awaiting them should they fall. As safety inspector, your problem will be to determine when it will be unsafe to ride. The given information is this: Radius of cylinder = 20m. Speed of rotation = 10 rpm.

a) Will leather-clad Biker Bob (mass = 100kg ;coeff. of static friction = 0.6) be safe?

b) How about Disco Stu, a 75kg man wearing a silk shirt and polyester pants (µs=0.15)?

Page 26: Centripetal Force Examples

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For Campus Learning Assistance Services at UCSB

Wheel of Doom!

This carnival ride is a giant metal cylinder which will spin around and pin the occupants to the wall. The fun part is when the floor drop out from below and the patrons see a spike-filled pit of angry crocodiles awaiting them should they fall. As safety inspector, your problem will be to determine when it will be unsafe to ride. The given information is this: Radius of cylinder = 20m. Speed of rotation = 10 rpm.

a) Will leather-clad Biker Bob (mass = 100kg ;coeff. of static friction = 0.6) be safe?

b) How about Disco Stu, a 75kg man wearing a silk shirt and polyester pants (µs=0.15)?

mg

Normal

friction

Biker Bob is safe (his 0.6 coefficient is larger than 0.44 , so static friction is enough to hold him in place)

Disco Stu is doomed! (his 0.15 coefficient is too small, so static friction fails to hold him in place)

Page 27: Centripetal Force Examples

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GRAVITY

Any pair of objects, anywhere in the universe, feel a mutual attraction due to gravity.

There are no exceptions – if you have mass, every other mass is attracted to you, and you are attracted to every other mass. Look around the room – everybody here is attracted to you!

Page 28: Centripetal Force Examples

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GRAVITY

Any pair of objects, anywhere in the universe, feel a mutual attraction due to gravity.

There are no exceptions – if you have mass, every other mass is attracted to you, and you are attracted to every other mass. Look around the room – everybody here is attracted to you!

Newton’s law of gravitation gives us a formula to calculate the attractive force between 2 objects:

221

gravr

mmGF

m1 and m2 are the masses, and r is the center-to-center distance between them

G is the gravitational constant – it’s tiny: G≈6.674*10-11 Nm2/kg2

m1

m2

r

F1 on 2

F2 on 1

Use this formula to find the magnitude of the gravity force.

Use a diagram or common sense to find the direction. The force will always be toward the other mass.

Page 29: Centripetal Force Examples

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Example:

Three planets are aligned as shown. The masses and distances are given in the diagram.

Find the net gravitational force on planet H (the middle one).

Planet Hollywood:

mass=6 x 1020 kg

Planet of the Apes:

mass=6 x 1024 kg

Daily Planet:

mass=3 x 1025 kg

1012 m 3 x 1012 m

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Example:

Three planets are aligned as shown. The masses and distances are given in the diagram.

Find the net gravitational force on planet H (the middle one).

Planet Hollywood:

mass=6 x 1020 kg

Planet of the Apes:

mass=6 x 1024 kg

Daily Planet:

mass=3 x 1025 kg

1012 m 3 x 1012 m

We should start by defining our coordinate system.

Let’s put the origin at planet H and say positive is to the right.

Page 31: Centripetal Force Examples

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Example:

Three planets are aligned as shown. The masses and distances are given in the diagram.

Find the net gravitational force on planet H (the middle one).

Planet Hollywood:

mass=6 x 1020 kg

Planet of the Apes:

mass=6 x 1024 kg

Daily Planet:

mass=3 x 1025 kg

1012 m 3 x 1012 m

We can also draw the forces on planet H in our diagram.

FDP on HFApes on H

Page 32: Centripetal Force Examples

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Example:

Three planets are aligned as shown. The masses and distances are given in the diagram.

Find the net gravitational force on planet H (the middle one).

Planet Hollywood:

mass=6 x 1020 kg

Planet of the Apes:

mass=6 x 1024 kg

Daily Planet:

mass=3 x 1025 kg

1012 m 3 x 1012 m

FDP on HFApes on H

221

gravr

mmGF

Our formula will find the forces (we supply the

direction from looking at the diagram):

Page 33: Centripetal Force Examples

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Example:

Three planets are aligned as shown. The masses and distances are given in the diagram.

Find the net gravitational force on planet H (the middle one).

Planet Hollywood:

mass=6 x 1020 kg

Planet of the Apes:

mass=6 x 1024 kg

Daily Planet:

mass=3 x 1025 kg

1012 m 3 x 1012 m

FDP on HFApes on H

221

gravr

mmGF

212

2024

kgNm11

HonApesm10

kg106kg1061067.6F

2

2

Our formula will find the forces (we supply the direction from looking at the diagram):

Page 34: Centripetal Force Examples

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Example:

Three planets are aligned as shown. The masses and distances are given in the diagram.

Find the net gravitational force on planet H (the middle one).

Planet Hollywood:

mass=6 x 1020 kg

Planet of the Apes:

mass=6 x 1024 kg

Daily Planet:

mass=3 x 1025 kg

1012 m 3 x 1012 m

Our formula will find the forces (we supply the direction from looking at the diagram):

FDP on HFApes on H

221

gravr

mmGF

N104.2m10

kg106kg1061067.6F 11

212

2024

kgNm11

HonApes 2

2

This is negative because the

force points to the left

Page 35: Centripetal Force Examples

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Example:

Three planets are aligned as shown. The masses and distances are given in the diagram.

Find the net gravitational force on planet H (the middle one).

Planet Hollywood:

mass=6 x 1020 kg

Planet of the Apes:

mass=6 x 1024 kg

Daily Planet:

mass=3 x 1025 kg

1012 m 3 x 1012 m

Our formula will find the forces (we supply the direction from looking at the diagram):

FDP on HFApes on H

221

gravr

mmGF

N104.2m10

kg106kg1061067.6F 11

212

2024

kgNm11

HonApes 2

2

This is negative because the

force points to the left

N103.1m103

kg106kg1031067.6F 11

212

2025

kgNm11

HonDP 2

2

This is positive because the

force points to the right

Page 36: Centripetal Force Examples

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Example:

Three planets are aligned as shown. The masses and distances are given in the diagram.

Find the net gravitational force on planet H (the middle one).

Planet Hollywood:

mass=6 x 1020 kg

Planet of the Apes:

mass=6 x 1024 kg

Daily Planet:

mass=3 x 1025 kg

1012 m 3 x 1012 m

Our formula will find the forces (we supply the direction from looking at the diagram):

FDP on HFApes on H

221

gravr

mmGF

N104.2m10

kg106kg1061067.6F 11

212

2024

kgNm11

HonApes 2

2

This is negative because the

force points to the left

N103.1m103

kg106kg1031067.6F 11

212

2025

kgNm11

HonDP 2

2

This is positive because the

force points to the right

Add the forces to get the net force on H:

N101.1F 11net

Net force is to the left

Page 37: Centripetal Force Examples

Prepared by Vince Zaccone

For Campus Learning Assistance Services at UCSB

2planet

planetgrav

R

mmGF

Rplanet

m

GRAVITY

One more useful detail about gravity:

The acceleration due to gravity on the surface of a planet is right there in the formula.

Here is the gravity formula, modified for the case where m is the mass of an object on the surface of a planet.

Page 38: Centripetal Force Examples

Prepared by Vince Zaccone

For Campus Learning Assistance Services at UCSB

2planet

planetgrav

R

mmGF

Rplanet

m

We already know that Fgrav is the weight of the object, and that should just be mg (if the planet is the Earth)

GRAVITY

One more useful detail about gravity:

The acceleration due to gravity on the surface of a planet is right there in the formula.

Here is the gravity formula, modified for the case where m is the mass of an object on the surface of a planet.

Page 39: Centripetal Force Examples

Prepared by Vince Zaccone

For Campus Learning Assistance Services at UCSB

GRAVITY

One more useful detail about gravity:

The acceleration due to gravity on the surface of a planet is right there in the formula.

Here is the gravity formula, modified for the case where m is the mass of an object on the surface of a planet.

2planet

planetgrav

R

mmGF

Rplanet

m

We already know that Fgrav is the weight of the object, and that should just be mg (if the planet is the Earth)

2planet

planet

R

mmGmg

This part is g