02 potential energy(1)

16
Potential Energy ENG1081 Physics for Engineering

Upload: shaun-stanley

Post on 13-May-2017

216 views

Category:

Documents


1 download

TRANSCRIPT

Page 1: 02 Potential Energy(1)

Potential Energy

ENG1081 Physics for Engineering

Page 2: 02 Potential Energy(1)

Potential Energy, U

Consider the following scenarios:• Riding on a roller coaster• Jumping on a trampoline

2

Page 3: 02 Potential Energy(1)

Work and Potential Energy

• We find that at instances where U is max, K is at minimum (and vice versa)

• Since K = W• U = -W

When U positive, K negativeWhen U negative, K positive

3

Page 4: 02 Potential Energy(1)

Conservative and Non-Conservative Forces

This would be a good time to introduce two separate groups of Forces

Conservative Forces– Energy Transfer between Forces are Reversible

Non-Conservative Forces– Non-Reversible Transfer of Energy between Forces

4

Page 5: 02 Potential Energy(1)

Testing for A Conservative Force

If it Passes Both of these Conditions:

1. In a Closed Path, the Net Work done on a Round Trip is 0.

2. Between Points A and B, the Work done is Independent of the Path taken

5

Page 6: 02 Potential Energy(1)

Expression for U

• We consider a generalised Work equation

• And because U = -W

𝑊=∫𝑥 𝑖

𝑥𝑓

𝐹 (𝑥 )𝑑𝑥

∆𝑈=−∫𝑥 𝑖

𝑥 𝑓

𝐹 (𝑥 )𝑑𝑥

Force that Varies with x

6

Page 7: 02 Potential Energy(1)

Gravitational Potential

∆𝑈=−∫𝑥 𝑖

𝑥 𝑓

𝐹 (𝑥 )𝑑𝑥 • Consider only vertical displacement (y)

• Take upwards direction as +ve

• Fg = -mg𝑈=𝑚𝑔𝑦

The higher the Object is, the more Gravitational Potential Energy it Contains 7

Page 8: 02 Potential Energy(1)

Elastic Potential

∆𝑈=−∫𝑥 𝑖

𝑥 𝑓

𝐹 (𝑥 )𝑑𝑥 The Spring Force, Fs = -kx

𝑈=12 𝑘𝑥

2

8

Page 9: 02 Potential Energy(1)

Conservation of Energy

∆𝐾=𝑊∆𝑈=−𝑊⇒∆𝐾=−∆𝑈⇒𝐾 2−𝐾 1=−(𝑈 2−𝑈 1)

𝐾 2+𝑈 2=𝐾 1+𝑈 1

∆𝐸𝑚𝑒𝑐=∆𝐾 +∆𝑈=0

9

Page 10: 02 Potential Energy(1)

Force and Potential Energy

• We can find U from F(x)

• How to we determine F(x) from U?

∆𝑈=−∫𝑥 𝑖

𝑥 𝑓

𝐹 (𝑥 )𝑑𝑥

∆𝑈=−𝑊=−𝐹 (𝑥 )∆ 𝑥

𝐹 (𝑥 )=− 𝑑(𝑈)𝑑𝑥 Check:

Gravity

Spring

𝐹 𝑔=−𝑑 (𝑚𝑔𝑥 )𝑑𝑥

𝐹 𝑠=−𝑑 (12 𝑘𝑥

2)

𝑑𝑥

Negative of the slope of plot U versus x 10

Page 11: 02 Potential Energy(1)

Spring Curves

11

Note: In reading of these graphs, it is convenient to ignore the negative value of the Spring Force and treat it as any regular Force

Page 12: 02 Potential Energy(1)

Potential Energy Curve

x = 0

x +ve

12

Page 13: 02 Potential Energy(1)

Potential Energy Curve

Turning Point

Turning Point

13

Page 14: 02 Potential Energy(1)

Equilibrium Points

When the force acting on the object is zero, the object is said to be in a state of Equilibrium• Stable Equilibrium – located at minimums, will

return if the object is displaced slightly• Unstable Equilibrium – located at maximums,

will move away if the object is displaced slightly• Neutral Equilibrium – located at plateaus,

where the net force equals zero.

14

Page 15: 02 Potential Energy(1)

Equilibrium Points

• Stable Equilibrium at x3 and x5.

• Unstable Equilibrium at x4.

• Neutral Equilibrium at x1 and x6.

15

Page 16: 02 Potential Energy(1)

Conservation of Energy with Friction Involved

Consider a scenario where you are pushing a cart up a slope.

Work, W = K + U = Emec With Friction, W = Emec + Ethermal

In both cases, Conservation of Energy appliesWork, W = E = Emec + Ethermal

16