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July 9, Week 6 Today: Chapter 10, Elastic Potential Energy Homework - - PowerPoint PPT Presentation
July 9, Week 6 Today: Chapter 10, Elastic Potential Energy Homework - - PowerPoint PPT Presentation
July 9, Week 6 Today: Chapter 10, Elastic Potential Energy Homework #6 due Friday Office hours today, 1:00-5:00 Elastic Energy 9th July 2014 Hookes Law A simple example of a variable force is the force needed to stretch a spring. Elastic
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Hooke’s Law
Elastic Energy 9th July 2014
A simple example of a variable force is the force needed to stretch a spring.
SLIDE 4
Hooke’s Law
Elastic Energy 9th July 2014
A simple example of a variable force is the force needed to stretch a spring. Hooke’s Law
- The
force needed to stretch
- r
compress a spring increases linearly with stretching distance
SLIDE 5
Hooke’s Law
Elastic Energy 9th July 2014
A simple example of a variable force is the force needed to stretch a spring. Hooke’s Law
- The
force needed to stretch
- r
compress a spring increases linearly with stretching distance
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Hooke’s Law
Elastic Energy 9th July 2014
A simple example of a variable force is the force needed to stretch a spring. Hooke’s Law
- The
force needed to stretch
- r
compress a spring increases linearly with stretching distance
SLIDE 7
Hooke’s Law
Elastic Energy 9th July 2014
A simple example of a variable force is the force needed to stretch a spring. s Hooke’s Law
- The
force needed to stretch
- r
compress a spring increases linearly with stretching distance
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Hooke’s Law
Elastic Energy 9th July 2014
A simple example of a variable force is the force needed to stretch a spring. s Hooke’s Law
- The
force needed to stretch
- r
compress a spring increases linearly with stretching distance Fsp = ks
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Hooke’s Law
Elastic Energy 9th July 2014
A simple example of a variable force is the force needed to stretch a spring. s Hooke’s Law
- The
force needed to stretch
- r
compress a spring increases linearly with stretching distance Fsp = ks k = spring constant, Unit: N/m s = stretching distance
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Hooke’s Law
Elastic Energy 9th July 2014
A simple example of a variable force is the force needed to stretch a spring. s lo Hooke’s Law
- The
force needed to stretch
- r
compress a spring increases linearly with stretching distance Fsp = ks k = spring constant, Unit: N/m s = stretching distance
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Hooke’s Law
Elastic Energy 9th July 2014
A simple example of a variable force is the force needed to stretch a spring. s lo l Hooke’s Law
- The
force needed to stretch
- r
compress a spring increases linearly with stretching distance Fsp = ks k = spring constant, Unit: N/m s = stretching distance
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Hooke’s Law
Elastic Energy 9th July 2014
A simple example of a variable force is the force needed to stretch a spring. s lo l s = l − lo Hooke’s Law
- The
force needed to stretch
- r
compress a spring increases linearly with stretching distance Fsp = ks k = spring constant, Unit: N/m s = stretching distance
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Spring Exercise
Elastic Energy 9th July 2014
Fsp = ks A horizontal 50-N force is applied to a 100 N/m spring whose unstretched length is 0.5 m. What is the spring’s length after the force has been applied? 50 N
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Spring Exercise
Elastic Energy 9th July 2014
Fsp = ks A horizontal 50-N force is applied to a 100 N/m spring whose unstretched length is 0.5 m. What is the spring’s length after the force has been applied? 50 N (a) 0 m
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Spring Exercise
Elastic Energy 9th July 2014
Fsp = ks A horizontal 50-N force is applied to a 100 N/m spring whose unstretched length is 0.5 m. What is the spring’s length after the force has been applied? 50 N (a) 0 m (b) 0.5 m
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Spring Exercise
Elastic Energy 9th July 2014
Fsp = ks A horizontal 50-N force is applied to a 100 N/m spring whose unstretched length is 0.5 m. What is the spring’s length after the force has been applied? 50 N (a) 0 m (b) 0.5 m (c) 1 m
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Spring Exercise
Elastic Energy 9th July 2014
Fsp = ks A horizontal 50-N force is applied to a 100 N/m spring whose unstretched length is 0.5 m. What is the spring’s length after the force has been applied? 50 N (a) 0 m (b) 0.5 m (c) 1 m (d) 1.5 m
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Spring Exercise
Elastic Energy 9th July 2014
Fsp = ks A horizontal 50-N force is applied to a 100 N/m spring whose unstretched length is 0.5 m. What is the spring’s length after the force has been applied? 50 N (a) 0 m (b) 0.5 m (c) 1 m (d) 1.5 m (e) 2 m
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Spring Exercise
Elastic Energy 9th July 2014
Fsp = ks A horizontal 50-N force is applied to a 100 N/m spring whose unstretched length is 0.5 m. What is the spring’s length after the force has been applied? 50 N (a) 0 m (b) 0.5 m (c) 1 m (d) 1.5 m (e) 2 m
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Spring Exercise
Elastic Energy 9th July 2014
Fsp = ks A horizontal 50-N force is applied to a 100 N/m spring whose unstretched length is 0.5 m. What is the spring’s length after the force has been applied? 50 N l0 = 0.5 m s = 0.5 m l (c) 1 m s = 50 N 100 N/m = 0.5 m
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Spring Exercise II
Elastic Energy 9th July 2014
Fsp = ks A 5-kg mass is attached, as shown, to a 100 N/m spring whose unstretched length is 0.5 m. If the mass is pushed 0.3 m to the left, what is the magnitude and direction of the force exerted by the spring on the mass? 0.3 m
SLIDE 22
Spring Exercise II
Elastic Energy 9th July 2014
Fsp = ks A 5-kg mass is attached, as shown, to a 100 N/m spring whose unstretched length is 0.5 m. If the mass is pushed 0.3 m to the left, what is the magnitude and direction of the force exerted by the spring on the mass? 0.3 m (a) 30 N, Left
SLIDE 23
Spring Exercise II
Elastic Energy 9th July 2014
Fsp = ks A 5-kg mass is attached, as shown, to a 100 N/m spring whose unstretched length is 0.5 m. If the mass is pushed 0.3 m to the left, what is the magnitude and direction of the force exerted by the spring on the mass? 0.3 m (a) 30 N, Left (b) 30 N, Right
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Spring Exercise II
Elastic Energy 9th July 2014
Fsp = ks A 5-kg mass is attached, as shown, to a 100 N/m spring whose unstretched length is 0.5 m. If the mass is pushed 0.3 m to the left, what is the magnitude and direction of the force exerted by the spring on the mass? 0.3 m (a) 30 N, Left (b) 30 N, Right (c) 20 N, Left
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Spring Exercise II
Elastic Energy 9th July 2014
Fsp = ks A 5-kg mass is attached, as shown, to a 100 N/m spring whose unstretched length is 0.5 m. If the mass is pushed 0.3 m to the left, what is the magnitude and direction of the force exerted by the spring on the mass? 0.3 m (a) 30 N, Left (b) 30 N, Right (c) 20 N, Left (d) 20 N, Right
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Spring Exercise II
Elastic Energy 9th July 2014
Fsp = ks A 5-kg mass is attached, as shown, to a 100 N/m spring whose unstretched length is 0.5 m. If the mass is pushed 0.3 m to the left, what is the magnitude and direction of the force exerted by the spring on the mass? 0.3 m (a) 30 N, Left (b) 30 N, Right (c) 20 N, Left (d) 20 N, Right (e) 50 N, Right
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Spring Exercise II
Elastic Energy 9th July 2014
Fsp = ks A 5-kg mass is attached, as shown, to a 100 N/m spring whose unstretched length is 0.5 m. If the mass is pushed 0.3 m to the left, what is the magnitude and direction of the force exerted by the spring on the mass? 0.3 m (a) 30 N, Left (b) 30 N, Right (c) 20 N, Left (d) 20 N, Right (e) 50 N, Right
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Spring Exercise II
Elastic Energy 9th July 2014
Fsp = ks A 5-kg mass is attached, as shown, to a 100 N/m spring whose unstretched length is 0.5 m. If the mass is pushed 0.3 m to the left, what is the magnitude and direction of the force exerted by the spring on the mass? s = 0.3 m Fsp = (100 N/m) (0.3 m) (b) 30 N, Right Springs pull when stretched and push when compressed
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Work to Stretch a Spring
Elastic Energy 9th July 2014
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Work to Stretch a Spring
Elastic Energy 9th July 2014
si
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Work to Stretch a Spring
Elastic Energy 9th July 2014
si
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Work to Stretch a Spring
Elastic Energy 9th July 2014
si sf
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Work to Stretch a Spring
Elastic Energy 9th July 2014
si sf s F
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Work to Stretch a Spring
Elastic Energy 9th July 2014
si sf s F Fsp = ks
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Work to Stretch a Spring
Elastic Energy 9th July 2014
si sf s F Fsp = ks
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Work to Stretch a Spring
Elastic Energy 9th July 2014
si sf s F Fsp = ks sf si
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Work to Stretch a Spring
Elastic Energy 9th July 2014
si sf s F Fsp = ks sf si
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Work to Stretch a Spring
Elastic Energy 9th July 2014
si sf s F Fsp = ks sf si Fi Ff W = 1
2(sf)(Ff) − 1 2(si)(Fi)
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Work to Stretch a Spring
Elastic Energy 9th July 2014
si sf s F Fsp = ks sf si Fi Ff W = 1
2(sf)(Ff) − 1 2(si)(Fi)
W = 1
2(sf)(ksf) − 1 2(si)(ksi)
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Work to Stretch a Spring
Elastic Energy 9th July 2014
si sf s F Fsp = ks sf si Fi Ff W = 1
2(sf)(Ff) − 1 2(si)(Fi)
W = 1
2(sf)(ksf) − 1 2(si)(ksi)
W = 1
2ks2 f − 1 2ks2 i
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Elastic Potential Energy
Elastic Energy 9th July 2014
Elastic Potential energy - Potential energy due to a spring.
SLIDE 42
Elastic Potential Energy
Elastic Energy 9th July 2014
Elastic Potential energy - Potential energy due to a spring.
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Elastic Potential Energy
Elastic Energy 9th July 2014
Elastic Potential energy - Potential energy due to a spring.
SLIDE 44
Elastic Potential Energy
Elastic Energy 9th July 2014
Elastic Potential energy - Potential energy due to a spring.
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Elastic Potential Energy
Elastic Energy 9th July 2014
Elastic Potential energy - Potential energy due to a spring. si
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Elastic Potential Energy
Elastic Energy 9th July 2014
Elastic Potential energy - Potential energy due to a spring. si sf
SLIDE 47
Elastic Potential Energy
Elastic Energy 9th July 2014
Elastic Potential energy - Potential energy due to a spring. si − → Fel Fel = −ks sf
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Elastic Potential Energy
Elastic Energy 9th July 2014
Elastic Potential energy - Potential energy due to a spring. si − → Fel Fel = −ks sf Wel = − 1
2ks2 f − 1 2ks2 i
- Elastic work converted to potential energy
SLIDE 49
Elastic Potential Energy
Elastic Energy 9th July 2014
Elastic Potential energy - Potential energy due to a spring. si − → Fel Fel = −ks sf Wel = − 1
2ks2 f − 1 2ks2 i
- Elastic work converted to potential energy
Wel = −∆Uel ⇒ Uel = 1
2ks2
SLIDE 50
Conservation of Elastic Energy
Elastic Energy 9th July 2014
If a spring is the only force doing work on something, Ei = Ef
SLIDE 51
Conservation of Elastic Energy
Elastic Energy 9th July 2014
If a spring is the only force doing work on something, Ei = Ef E = K + Uel = 1 2mv2 + 1 2ks2
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Conservation of Elastic Energy
Elastic Energy 9th July 2014
If a spring is the only force doing work on something, Ei = Ef E = K + Uel = 1 2mv2 + 1 2ks2 1 2mv2
i + 1
2ks2
i = 1
2mv2
f + 1
2ks2
f
SLIDE 53
Elastic Potential Energy Exercise
Elastic Energy 9th July 2014
A 10-kg mass slides across a frictionless, horizontal floor going 5 m/s (and therefore has 125 J of kinetic energy) when it collides with the k = 500 N/m spring shown. What is the maximum compression of the spring?
SLIDE 54
Elastic Potential Energy Exercise
Elastic Energy 9th July 2014
A 10-kg mass slides across a frictionless, horizontal floor going 5 m/s (and therefore has 125 J of kinetic energy) when it collides with the k = 500 N/m spring shown. What is the maximum compression of the spring? (a) 125 J 500 N/m = 0.25 m
SLIDE 55
Elastic Potential Energy Exercise
Elastic Energy 9th July 2014
A 10-kg mass slides across a frictionless, horizontal floor going 5 m/s (and therefore has 125 J of kinetic energy) when it collides with the k = 500 N/m spring shown. What is the maximum compression of the spring? (a) 125 J 500 N/m = 0.25 m (b) 50 kg · m/s 500 N/m = 0.1 m
SLIDE 56
Elastic Potential Energy Exercise
Elastic Energy 9th July 2014
A 10-kg mass slides across a frictionless, horizontal floor going 5 m/s (and therefore has 125 J of kinetic energy) when it collides with the k = 500 N/m spring shown. What is the maximum compression of the spring? (a) 125 J 500 N/m = 0.25 m (b) 50 kg · m/s 500 N/m = 0.1 m (c) 125 J 250 N/m = 0.5 m
SLIDE 57
Elastic Potential Energy Exercise
Elastic Energy 9th July 2014
A 10-kg mass slides across a frictionless, horizontal floor going 5 m/s (and therefore has 125 J of kinetic energy) when it collides with the k = 500 N/m spring shown. What is the maximum compression of the spring? (a) 125 J 500 N/m = 0.25 m (b) 50 kg · m/s 500 N/m = 0.1 m (c) 125 J 250 N/m = 0.5 m (d)
- 125 J
250 N/m = 0.7071 m
SLIDE 58
Elastic Potential Energy Exercise
Elastic Energy 9th July 2014
A 10-kg mass slides across a frictionless, horizontal floor going 5 m/s (and therefore has 125 J of kinetic energy) when it collides with the k = 500 N/m spring shown. What is the maximum compression of the spring? (a) 125 J 500 N/m = 0.25 m (b) 50 kg · m/s 500 N/m = 0.1 m (c) 125 J 250 N/m = 0.5 m (d)
- 125 J
250 N/m = 0.7071 m (e)
- 125 J
500 N/m = 0.5 m
SLIDE 59
Elastic Potential Energy Exercise
Elastic Energy 9th July 2014
A 10-kg mass slides across a frictionless, horizontal floor going 5 m/s (and therefore has 125 J of kinetic energy) when it collides with the k = 500 N/m spring shown. What is the maximum compression of the spring? (a) 125 J 500 N/m = 0.25 m (b) 50 kg · m/s 500 N/m = 0.1 m (c) 125 J 250 N/m = 0.5 m (d)
- 125 J
250 N/m = 0.7071 m (e)
- 125 J
500 N/m = 0.5 m
SLIDE 60
Elastic Potential Energy Exercise
Elastic Energy 9th July 2014
A 10-kg mass slides across a frictionless, horizontal floor going 5 m/s (and therefore has 125 J of kinetic energy) when it collides with the k = 500 N/m spring shown. What is the maximum compression of the spring?
1 2mv2
i + 1
2ks2
i = 1
2mv2
f + 1
2ks2
f
vi = 5 m/s si = 0 vf = 0 sf =? ⇒ 125 J + 0 = 0 + 1 2(500 N/m)s2
f
(d)
- 125 J
250 N/m = 0.7071 m
SLIDE 61
General Energy Problems
Elastic Energy 9th July 2014
The most general problems (this term) involve gravity, springs, and
- ther forces all doing work.
SLIDE 62
General Energy Problems
Elastic Energy 9th July 2014
The most general problems (this term) involve gravity, springs, and
- ther forces all doing work.
SLIDE 63
General Energy Problems
Elastic Energy 9th July 2014
The most general problems (this term) involve gravity, springs, and
- ther forces all doing work.
m− → g
SLIDE 64
General Energy Problems
Elastic Energy 9th July 2014
The most general problems (this term) involve gravity, springs, and
- ther forces all doing work.
m− → g − → Fel
SLIDE 65
General Energy Problems
Elastic Energy 9th July 2014
The most general problems (this term) involve gravity, springs, and
- ther forces all doing work.
m− → g − → Fel − → Fother ANY other force doing work
SLIDE 66
General Energy Problems
Elastic Energy 9th July 2014
The most general problems (this term) involve gravity, springs, and
- ther forces all doing work.
m− → g − → Fel − → Fother ANY other force doing work Wtotal = Wg + Wel + Wother
SLIDE 67
General Energy Problems
Elastic Energy 9th July 2014
The most general problems (this term) involve gravity, springs, and
- ther forces all doing work.
m− → g − → Fel − → Fother ANY other force doing work Wtotal = Wg + Wel + Wother ∆K
SLIDE 68
General Energy Problems
Elastic Energy 9th July 2014
The most general problems (this term) involve gravity, springs, and
- ther forces all doing work.
m− → g − → Fel − → Fother ANY other force doing work Wtotal = Wg + Wel + Wother ∆K −∆Ug
SLIDE 69
General Energy Problems
Elastic Energy 9th July 2014
The most general problems (this term) involve gravity, springs, and
- ther forces all doing work.
m− → g − → Fel − → Fother ANY other force doing work Wtotal = Wg + Wel + Wother ∆K −∆Ug −∆Uel
SLIDE 70
General Energy Problems
Elastic Energy 9th July 2014
The most general problems (this term) involve gravity, springs, and
- ther forces all doing work.
m− → g − → Fel − → Fother ANY other force doing work Wtotal = Wg + Wel + Wother ∆K −∆Ug −∆Uel 1 2mv2
i + mgyi + 1
2ks2
i + Wother = 1
2mv2
f + mgyf + 1
2ks2
f
SLIDE 71
General Energy Conservation III
Elastic Energy 9th July 2014
1 2mv2
i + mgyi + 1
2ks2
i + Wother = 1
2mv2
f + mgyf + 1
2ks2
f
Example: An 80 kg man jumps onto a spring platform (k = 18000 N/m) going 9 m/s. How far does he compress the spring?
SLIDE 72
General Energy Conservation III
Elastic Energy 9th July 2014
1 2mv2
i + mgyi + 1
2ks2
i + Wother = 1
2mv2
f + mgyf + 1
2ks2
f
Example: An 80 kg man jumps onto a spring platform (k = 18000 N/m) going 9 m/s. How far does he compress the spring? Example: An 80 kg man skydives from a plane 1600 m above the
- ground. If he lands with a speed of 10 m/s (and was essentially at