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1 PH 202-5E Fall 2005 Electrostatic Potential and Energy Lectures 5-7 Chapter 19 (Cutnell & Johnson, Physics 6 th edition)

Lectures5-7 El potential & Energy ch 19mirov/L5-7 ch 19.pdfLectures 5-7 Chapter 19 (Cutnell & Johnson, Physics 6th edition) 2 Electrostatic Potential and Energy. 3 Uniform electric

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Page 1: Lectures5-7 El potential & Energy ch 19mirov/L5-7 ch 19.pdfLectures 5-7 Chapter 19 (Cutnell & Johnson, Physics 6th edition) 2 Electrostatic Potential and Energy. 3 Uniform electric

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PH 202-5E Fall 2005

Electrostatic Potential and Energy

Lectures 5-7

Chapter 19(Cutnell & Johnson, Physics 6th edition)

Page 2: Lectures5-7 El potential & Energy ch 19mirov/L5-7 ch 19.pdfLectures 5-7 Chapter 19 (Cutnell & Johnson, Physics 6th edition) 2 Electrostatic Potential and Energy. 3 Uniform electric

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Electrostatic Potential and Energy

Page 3: Lectures5-7 El potential & Energy ch 19mirov/L5-7 ch 19.pdfLectures 5-7 Chapter 19 (Cutnell & Johnson, Physics 6th edition) 2 Electrostatic Potential and Energy. 3 Uniform electric

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Uniform electric field in the space between two charged parallel plates

Page 4: Lectures5-7 El potential & Energy ch 19mirov/L5-7 ch 19.pdfLectures 5-7 Chapter 19 (Cutnell & Johnson, Physics 6th edition) 2 Electrostatic Potential and Energy. 3 Uniform electric

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Electrostatic Potential V at a given point is the electric potential energy of a small test charge q situated at that point divided by the charge itself

Neither the potential V nor the potential energy EPE can be determined in an absolute sense, because only the differences ∆V and ∆EPE are measurable in terms of the work WAB.

Page 5: Lectures5-7 El potential & Energy ch 19mirov/L5-7 ch 19.pdfLectures 5-7 Chapter 19 (Cutnell & Johnson, Physics 6th edition) 2 Electrostatic Potential and Energy. 3 Uniform electric

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The electric potential difference created by a point chargeThe positive test charge +qoexperiences a repulsive force F due to the positive point charge +q. As a result, work is done by this force when the test charge moves from A to B. consequently, the electric potential is higher (uphill) at A and lower (downhill) at B.

WAB=kqqo/rA-kqqo/rB

VB-VA=-WAB/q=kq/rB -kq/rA

for rB=∞ kq/rB=0 ⇒VB=0

⇒VA= kq/rA or V=kq/r

The symbol V does not refer to the potential in any absolute sense. Rather,

V =kq/r stands for the amount by which the potential at a distance r from a point charge differs from te potential at an infinite distance away. In other words, V refers to a potential difference with the arbitrary assumption that the potential at infinity is zero.

Page 6: Lectures5-7 El potential & Energy ch 19mirov/L5-7 ch 19.pdfLectures 5-7 Chapter 19 (Cutnell & Johnson, Physics 6th edition) 2 Electrostatic Potential and Energy. 3 Uniform electric

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Example. The potential of a point charge for a zero reference potential at infinity

A point charge of q=4.0x10-8C creates a potential at a spot 1.2 m away.

The potential is (a) V=kq/r=

=(8.99x109)(+4.0x10-8)/1.2=+300V when the charge is positive

and (b) -300V when the charge is negative

Page 7: Lectures5-7 El potential & Energy ch 19mirov/L5-7 ch 19.pdfLectures 5-7 Chapter 19 (Cutnell & Johnson, Physics 6th edition) 2 Electrostatic Potential and Energy. 3 Uniform electric

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The acceleration of positive and negative charges

A positive charge accelerates from a region of higher electric potential toward a region of lower electric potential

A negative charge accelerates from a region of lower electric potential toward a region of higher electric potential

Page 8: Lectures5-7 El potential & Energy ch 19mirov/L5-7 ch 19.pdfLectures 5-7 Chapter 19 (Cutnell & Johnson, Physics 6th edition) 2 Electrostatic Potential and Energy. 3 Uniform electric

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The electric potential energy of a point charge q for non-uniform electric field

Page 9: Lectures5-7 El potential & Energy ch 19mirov/L5-7 ch 19.pdfLectures 5-7 Chapter 19 (Cutnell & Johnson, Physics 6th edition) 2 Electrostatic Potential and Energy. 3 Uniform electric

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Electrostatic Potential of a point charge

Page 10: Lectures5-7 El potential & Energy ch 19mirov/L5-7 ch 19.pdfLectures 5-7 Chapter 19 (Cutnell & Johnson, Physics 6th edition) 2 Electrostatic Potential and Energy. 3 Uniform electric

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One electron volt is the magnitude of the amount by which the potential energy of an electron changes when the electron moves through the potential difference of 1 volt

Page 11: Lectures5-7 El potential & Energy ch 19mirov/L5-7 ch 19.pdfLectures 5-7 Chapter 19 (Cutnell & Johnson, Physics 6th edition) 2 Electrostatic Potential and Energy. 3 Uniform electric

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Page 12: Lectures5-7 El potential & Energy ch 19mirov/L5-7 ch 19.pdfLectures 5-7 Chapter 19 (Cutnell & Johnson, Physics 6th edition) 2 Electrostatic Potential and Energy. 3 Uniform electric

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A headlight connected to a 12-V battery

Page 13: Lectures5-7 El potential & Energy ch 19mirov/L5-7 ch 19.pdfLectures 5-7 Chapter 19 (Cutnell & Johnson, Physics 6th edition) 2 Electrostatic Potential and Energy. 3 Uniform electric

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-2.3x10-18 J

-6.5x10-19 J

done by the electric force

Work to be done against the electric force = +10 eV

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Page 15: Lectures5-7 El potential & Energy ch 19mirov/L5-7 ch 19.pdfLectures 5-7 Chapter 19 (Cutnell & Johnson, Physics 6th edition) 2 Electrostatic Potential and Energy. 3 Uniform electric

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Page 16: Lectures5-7 El potential & Energy ch 19mirov/L5-7 ch 19.pdfLectures 5-7 Chapter 19 (Cutnell & Johnson, Physics 6th edition) 2 Electrostatic Potential and Energy. 3 Uniform electric

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Equipotential surface for a very large sheet with a uniform distribution of charge

Definition: Equipotential surface – a mathematical surface on which the electrostatic potential has a fixed constant value

Page 17: Lectures5-7 El potential & Energy ch 19mirov/L5-7 ch 19.pdfLectures 5-7 Chapter 19 (Cutnell & Johnson, Physics 6th edition) 2 Electrostatic Potential and Energy. 3 Uniform electric

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Equipotential surfaces for a positive point charge.The equipotentials are concentric spheres. Points at the same distance

from the central charge are at the same potential

rqqU

o

'4

1 ⋅⋅=

πε

rq

qUV

o

⋅==πε41

'

Page 18: Lectures5-7 El potential & Energy ch 19mirov/L5-7 ch 19.pdfLectures 5-7 Chapter 19 (Cutnell & Johnson, Physics 6th edition) 2 Electrostatic Potential and Energy. 3 Uniform electric

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Properties of the equipotential surfaces and some useful conclusions

but it is wrong V1=V2

0

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Energy of a system of charged conductors

Page 24: Lectures5-7 El potential & Energy ch 19mirov/L5-7 ch 19.pdfLectures 5-7 Chapter 19 (Cutnell & Johnson, Physics 6th edition) 2 Electrostatic Potential and Energy. 3 Uniform electric

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1.0 mm

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Capacitance

A large value of C implies that a large amount of charge can be stored at low voltage.

Page 28: Lectures5-7 El potential & Energy ch 19mirov/L5-7 ch 19.pdfLectures 5-7 Chapter 19 (Cutnell & Johnson, Physics 6th edition) 2 Electrostatic Potential and Energy. 3 Uniform electric

28V

QC∆

=

Page 29: Lectures5-7 El potential & Energy ch 19mirov/L5-7 ch 19.pdfLectures 5-7 Chapter 19 (Cutnell & Johnson, Physics 6th edition) 2 Electrostatic Potential and Energy. 3 Uniform electric

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Capacitance of a parallel plate capacitor

Page 30: Lectures5-7 El potential & Energy ch 19mirov/L5-7 ch 19.pdfLectures 5-7 Chapter 19 (Cutnell & Johnson, Physics 6th edition) 2 Electrostatic Potential and Energy. 3 Uniform electric

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Potential energy in capacitor

signal.

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Dielectrics

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