Physics 1710 Chapter 8—Potential Energy
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Transcript of Physics 1710 Chapter 8—Potential Energy
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Solution:Solution:
Physics 1710Physics 1710 Chapter 8—Potential Chapter 8—Potential EnergyEnergy
Power = dW/dt = (Fdx)/dt = F dx/dtPower = dW/dt = (Fdx)/dt = F dx/dt
= F v (for F constant)= F v (for F constant)
= (20.0 N )(36 x 10= (20.0 N )(36 x 1033 m/ 3600 sec) m/ 3600 sec)
= 200. N m/s = 200. W (#4)= 200. N m/s = 200. W (#4)
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What is the minimum height What is the minimum height from which a small rolling ball from which a small rolling ball must be started from rest so that must be started from rest so that it will complete a loop-the-loop?it will complete a loop-the-loop?
RR
hh
Physics 1710Physics 1710 Chapter 8—Potential Chapter 8—Potential EnergyEnergy
ReviewReview
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What is the minimum height What is the minimum height from which a small rolling ball from which a small rolling ball must be started from rest so that must be started from rest so that it will complete a loop-the-loop?it will complete a loop-the-loop?
RR
hh
vv22/R = g/R = g
K = U - WK = U - W
½ mv ½ mv 22 + ½ ( + ½ (2/52/5 mv mv 22)= )=
mgh mgh
v v 22 = Rg = = Rg = 10/710/7 hg hg
h = 0.7 Rh = 0.7 R
h = h = 7/107/10(22.0 cm) = (22.0 cm) = 15.4 cm15.4 cmd = 2R+h = 69.4 cmd = 2R+h = 69.4 cm
vv
Physics 1710Physics 1710 Chapter 8—Potential Chapter 8—Potential EnergyEnergy
dd
Physics Works!Physics Works!
(When you include all relevant (When you include all relevant effects)effects)
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11′′ Lecture Lecture
• Potential Energy is Potential Energy is U = -U = -∫ F•d r∫ F•d r
• The sum of all energy, potential and The sum of all energy, potential and kinetic, ofkinetic, of a system is conserved, in the absence of a system is conserved, in the absence of dissipation:dissipation:
E = U + K – WE = U + K – W
• F = - F = - ∇U = negative gradient of U.∇U = negative gradient of U.
Physics 1710Physics 1710 Chapter 8—Potential Chapter 8—Potential EnergyEnergy
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Potential Energy:Potential Energy:
W = W = ∫ ∫ F•F•d d rr
U = -W = -∫ U = -W = -∫ F•F•d d rr
• Potential Energy is the negative of the work Potential Energy is the negative of the work required to put the system in the current state.required to put the system in the current state.
Physics 1710Physics 1710 Chapter 8—Potential Chapter 8—Potential EnergyEnergy
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What is the potential energy What is the potential energy of a 0.100 kg ball placed up a of a 0.100 kg ball placed up a 45 45 oo ramp 0.50 above the ramp 0.50 above the table?table?
Physics 1710Physics 1710 Chapter 8—Potential Chapter 8—Potential EnergyEnergy
FF
xx 0.50 0.50 mm
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What is the potential energy What is the potential energy of a 0.100 kg ball placed up a of a 0.100 kg ball placed up a 45 45 oo ramp 0.50 above the ramp 0.50 above the table?table?
Physics 1710Physics 1710 Chapter 8—Potential Chapter 8—Potential EnergyEnergy
FF
xx 0.50 0.50 mm
- - mgmg
U = - FU = - F‧x = - (-‧x = - (-mg)hmg)h
= mg h= mg h
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Example: Elevated Mass Example: Elevated Mass
F = -mg F = -mg • Potential Energy:Potential Energy:
UUgg = - = -∫∫00
hhFdy = Fdy = --∫∫00
hh(- mg) dy(- mg) dy
UUgg = mg∫ = mg∫00
h h dy = mgh dy = mgh
• Thus, the potential energy stored in an elevated Thus, the potential energy stored in an elevated mass is proportional to the mass is proportional to the height hheight h and the and the weightweight of the mass.of the mass.
Physics 1710Physics 1710 Chapter 8—Potential Chapter 8—Potential EnergyEnergy
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Relationship Between Relationship Between F F and and U:U:
U = -U = -∫ ∫ F•F•dd r r SoSo
U = -∫ [ FU = -∫ [ Fx x dx + Fdx + Fyy dy + F dy + Fzz dz] dz]ThenThen
FFx x =-dU/dx ; F=-dU/dx ; Fyy =-dU/dy; F =-dU/dy; Fzz =-dU/dz =-dU/dz
FF = - = -∇∇UU
F= -gradient of F= -gradient of UU
Physics 1710Physics 1710 Chapter 8—Potential Chapter 8—Potential EnergyEnergy
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The FThe Force is equal to the negative orce is equal to the negative gradient of the potential energy:gradient of the potential energy:
FF = - = -∇∇UUFFx x = -∂U/∂x = -∂U/∂x
FFyy = -∂U/∂y = -∂U/∂y
FFzz = -∂U/∂z = -∂U/∂z
Physics 1710Physics 1710 Chapter 8—Potential Chapter 8—Potential EnergyEnergy
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Example: PendulumExample: Pendulum
U = mg hU = mg hh = L(1- cos h = L(1- cos ))
U = mg L(1- cos U = mg L(1- cos ))
s= L s= L FFSS= - (1/L)dU/d = - (1/L)dU/d = - mg sin = - mg sin
Physics 1710Physics 1710 Chapter 8—Potential Chapter 8—Potential EnergyEnergy
ss
LL
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Example:Example: Ball on a slopeBall on a slope
• h = ax + byh = ax + by• U = mghU = mgh• FFxx = - = -∂U/∂x = ∂U/∂x = --∂(mgh)/∂x = -mg∂h/∂x ∂(mgh)/∂x = -mg∂h/∂x Similarly:Similarly:
FFyy = = --∂U/∂y = -mg b∂U/∂y = -mg b
• Thus, Thus, F = -F = -mgmg( ( aa i + i + b b j j ))
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Example: Mass on a SpringExample: Mass on a Spring
Potential Energy:Potential Energy:
U = ½ k x U = ½ k x 22
F =dU/dxF =dU/dxF= -½ k dxF= -½ k dx22/dx/dx
F= -k xF= -k x
• Thus, the force is equal to the negative of the gradient of Thus, the force is equal to the negative of the gradient of the potential energy.the potential energy.
Physics 1710Physics 1710 Chapter 8—Potential Chapter 8—Potential EnergyEnergy
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Force:Force:
z = arz = ar22
U = mgzU = mgz
• FFrr = - = -∂U/∂r = ∂U/∂r = --∂(mgz)/∂r = -mg∂z/∂r ∂(mgz)/∂r = -mg∂z/∂r = - 2amgr = - k r= - 2amgr = - k r
Like a mass on a spring!Like a mass on a spring!
Physics 1710Physics 1710 Chapter 8—Potential Chapter 8—Potential EnergyEnergy
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Conservation of EnergConservation of Energy:y:
• The sum of all energy in a system is The sum of all energy in a system is conserved, i.e. remains the same.conserved, i.e. remains the same.
E = U + KE = U + K
Physics 1710Physics 1710 Chapter 8—Potential Chapter 8—Potential EnergyEnergy
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Dissipative (non-conservative) Forces:Dissipative (non-conservative) Forces:
W = W = ∫ ∫ F•F•d d rr
==∫ (C v∫ (C vxx 2 2 )dx)dx
==∫ (C v∫ (C vxx 2 2 )(dx /dt) dt)(dx /dt) dt
=∫ (C v=∫ (C vxx 3 3 )dt)dt
E = U + K -WE = U + K -W
Physics 1710Physics 1710 Chapter 8—Potential Chapter 8—Potential EnergyEnergy
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Summary:Summary:
•The Potential Energy is equal to the The Potential Energy is equal to the negative of the work done on the system to negative of the work done on the system to put it in its present state.put it in its present state.
U = -U = -∫ F•d r∫ F•d r
• F = - F = - ∇U∇U• The sum of all energy, potential and The sum of all energy, potential and kinetic, of a system is conserved, in the kinetic, of a system is conserved, in the absence of dissipation.absence of dissipation.
E = U + K – WE = U + K – W
Physics 1710Physics 1710 Chapter 8—Potential Chapter 8—Potential EnergyEnergy
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Potential Energy:Potential Energy:
FF
-F-F
hh
U = U = m g hm g h
P P = = dU/dt dU/dt
= mg dh/dt= mg dh/dtmg =(100. mg =(100. kg)(9.8N/kg)kg)(9.8N/kg)
= 98.0 N= 98.0 N
dh/dt dh/dt = 10 m/10 = 10 m/10 s s
= 1 m/s= 1 m/s
P P = 98. W= 98. W
Physics 1710Physics 1710 Chapter 8—Potential Chapter 8—Potential EnergyEnergy