Download PHYS 1112 In-Class Exam #2A Thu. March 19, 2009, 11:00am-12:15pm

Physics 1112
Spring 2009
University of Georgia
Instructor: HBSchüttler
PHYS 1112 In-Class Exam #2A
Thu. March 19, 2009, 11:00am-12:15pm
This is a closed-book, closed-notes exam. The last exam pages are sheets of formulae and
numerical data for you to consult.
The exam consists of 12 multiple-choice questions. Each question is worth one raw score
point. There will be no penalty for wrong answers. No partial credit will be given. I
recommend that you read all the questions at the start so that you can allocate your time
wisely. (Answer the easy questions first!)
You may use a scientific calculator for arithmetic only; your calculator must be non-graphing,
non-programmable, and non-algebraic. You are not allowed to share your calculator. The
use of cell phones, pagers, PDAs, or any other electronic devices (besides calculators) is
forbidden. All such gadgets must be turned off and put away; distractions caused by these
devices will not be tolerated.
• Do not open the exam until you are told to begin.
• Make sure the scantron sheet has your name and your UGA Card ID (810-...) number
filled in. Make sure you also have entered your name, UGA Card ID number and
signature on the exam cover page (this page!) below.
• At the end of the exam period you must hand in both your scantron sheet and the
exam paper cover page, signed and with your name and UGA Card ID (810-...) number
filled-in.
• Your exam will not be graded, and you will receive a score of zero, if you do not hand
in both a properly filled in scantron sheet and the exam paper cover page, properly
filled-in and signed.
• You have until the end of the class period (i.e. until 12:15pm for Period 3 Class, until
3:15pm for Period 5 Class) to finish the exam and hand in the required exam materials
described above.
By signing below, you indicate that you understand the instructions for this exam and agree
to abide by them. You also certify that you will personally uphold the university standards
of academic honesty for this exam, and will not tolerate any violations of these standards by
others. Unsigned exams will not be graded.
Name (please print):
UGACard ID (810-...) #:
Signature:
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Physics 1112
Spring 2009
University of Georgia
Instructor: HBSchüttler
Conceptual Problems
Problem 1: A beam of coherent (laser) light of wavelength λ is incident upon a diffraction
grating with line spacing d, with λ < d, as shown in the figure below. Assume |∆y| is the
distance (in cm) between the two 1st-order intensity maxima, observed on a screen at a
distance L on the other side of the grating. This distance |∆y| will
1st order maxima
Fig. 2.03
Δy
Screen
θ
L
Diff. Grating
Laser Beam
(A)
(B)
(C)
(D)
(E)
decrease if we increase L (keeping λ and d fixed);
decrease if we increase λ (keeping L and d fixed);
decrease if we increase d (keeping λ and L fixed);
increase if we decrease λ (keeping L and d fixed);
increase if we increase d (keeping λ and L fixed).
Problem 2: If two point charges Q1 and Q2 at some distance r repel each other with a
force of 160N, what force would they exert on each other if r is quadrupled (×4); and Q1
and Q2 are unchanged ? The two charges will
(A)
(B)
(C)
(D)
(E)
repel each other with a force of 40µN
attract each other with a force of 2560kN
attract each other with a force of 10N
repel each other with a force of 2560kN
repel each other with a force of 10N
Problem 3: Q in the figure below is a negative point charge. Which arrow drawn at P
~ generated by Q at P ?
could correctly represent the electric field vector E
2
Physics 1112
Spring 2009
University of Georgia
Instructor: HBSchüttler
Fig. 2.09
P
(B)
(A)
(C)
(E)
(D)
Q
(A)
(B)
(C)
(D)
(E)
Problem 4: In Experiment 1 an electron travels from point A to point B, in the electric
~ generated by/between two oppositely charged capacitor plates, as shown in the figure
field E
below. In Experiment 2 a proton travels from point A to point B, in the same electric field
between the same two charged capacitor plates. A proton has a charge +e and an electron
has a charge −e.
Fig. 2.14
------------------------E
A
B
E
+++++++++++++++++++++++++++
Assume the electron experiences a rise in electric potential, ∆V = +500V, and a loss of
potential energy, ∆U = −80aJ (where 1aJ ≡ 10−18 J), in traveling from A to B. What will
the proton experience ?
(A)
(B)
(C)
(D)
(E)
∆V
∆V
∆V
∆V
∆V
= −50V and ∆U = −8aJ
= −100V and ∆U = −16aJ
= +100V and ∆U = +16aJ
= −500V and ∆U = −80aJ
= +500V and ∆U = +80aJ
Numerical Problems
Problem 5: If a diffraction grating with a line spacing of 1200nm is illuminated at normal
incidence by coherent (laser) light with a wavelength of 550nm, at what angles θ, measured
from the central (0th order) intensity maxium, will the 2nd order maxima be observed ?
(See figure in Problem 1.)
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Physics 1112
Spring 2009
(A)
(B)
(C)
(D)
(E)
University of Georgia
Instructor: HBSchüttler
±66.44o
±50.23o
±39.18o
±26.78o
±19.42o
Problem 6: What is the electric force between two point charges of −3.0mC and +4.0mC,
spaced 15m apart ? Is there attraction or repulsion between the two charges ?
(A)
(B)
(C)
(D)
(E)
82.52N,
479.5N,
779.1N,
2877.N,
5678.N,
repulsion
attraction
repulsion
attraction
repulsion
Problem 7: How far apart must two equal point charges, of +2.5mC each, be spaced so
that they repel each other with a force of 40.0N ?
(A)
(B)
(C)
(D)
(E)
1.634 m
37.48 m
337.3m
22.39km
3257.km
Problem 8: If a charge of −72µC is uniformly spread out over a single thin, square-shaped
sheet of aluminum foil, 3.0m to the side, what is the strength and the direction of the electric
field generated by that charge, very close to the surface and far from the edges of that foil?
(Hint: Think of the aluminum foil as a single, uniformly charged planar surface.)
~ pointing towards the foil
(A) 5752.0 × 103 N/C, E
~ pointing away from the foil
(B) 5752.0 × 103 N/C, E
~ pointing towards the foil
(C) 27.89 × 103 N/C, E
~ pointing away from the foil
(D) 27.89 × 103 N/C, E
~ pointing towards the foil
(E) 452.0 × 103 N/C, E
Problem 9: The total electric flux passing through the approximately spherical surface of a
real football (i.e., a soccer ball !!) is Φ = +565Nm2 /C (assuming outward directed normal
to the surface). What is the total electric charge enclosed inside the ball ?
(A) −2.00nC
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Physics 1112
Spring 2009
(B)
(C)
(D)
(E)
University of Georgia
Instructor: HBSchüttler
+3.00nC
−4.00nC
+5.00nC
−6.00nC
Problem 10: The 450µF capacitor in a defibrillator must be charged to store ±270mC in
its two plates. What charging voltage is required for this ?
(A)
(B)
(C)
(D)
(E)
600V
800V
1000V
1200V
1400V
Problem 11: How much electric field energy is stored in the defibrillator capacitor in
Problem 10 when it is fully charged ?
(A)
(B)
(C)
(D)
(E)
27J
36J
64J
81J
128J
Problem 12: If the electric field strength between the capacitor plates in Problem 4 is
228.V/m, what is the magnitude and the direction of the electron’s acceleration ~a, assuming
the electron is subject only to the electric force between the plates ?
(A)
(B)
(C)
(D)
(E)
4.00 × 1013 m/s2 , ~a
4.00 × 1013 m/s2 , ~a
9.00 × 1013 m/s2 , ~a
9.00 × 1013 m/s2 , ~a
9.00 × 1013 m/s2 , ~a
pointing
pointing
pointing
pointing
pointing
leftward
downward
rightward
leftward
downward
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Physics 1112
Spring 2009
University of Georgia
Instructor: HBSchüttler
Formula Sheet
Wave Optics, Interference, Diffraction
(1) Periodic Wave Condition:
v = λf =
λ
τ
(2) Index of Refraction for electromagnetic waves, definition:
n=
λvacuum
c
=
v
λ
with λvacuum ≡ c/f = cτ .
(3) Definition of Path Length Difference for two-source, double-slit or adjacent slits in
multi-slit/diffraction grating:
∆` ≡ `2 − `1
(4) Path Length Difference vs. Angle: ∆` is given approximately in terms of observation
angle θ measured from central axis:
∆` ∼
= d sin θ
if
dL
where L =distance from slits or sources to observation screen, d =spacing of adjacent sources,
slits or lines in double-slit, multi-slit or diffraction grating.
(5) Constructive Interference Condition (≡ intensity maxima, principal maxima, bright
fringes) for two-source, double-slit, multi-slit or diffraction grating:
∆` = mλ
or
d L);
d sin θ = mλ (if
with m = 0, ±1, ±2, ...
where m is the ”order” of the (principal) maximum.
(6) Destructive Interference Condition 1 (≡ intensity minima, dark fringes) for twosource or double-slit experiment:
∆` = m +
1
λ
2
or
d sin θ = m +
1
λ (if d L);
2
with
m+
1
1 3
= ± , ± , ...
2
2 2
(7) Destructive Interference Condition 2 (≡ intensity minima, dark fringes) for singleslit diffration with W =slit width and W L:
W sin θ = mλ
with m = ±1, ±2, ... (but m 6= 0).
(8) Destructive Interference Condition 3 for first intensity minimum of circular aperture
diffration with W =aperture diameter and W L:
W sin θ ∼
= 1.22λ (for 1st circular intensity minimum).
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Physics 1112
Spring 2009
University of Georgia
Instructor: HBSchüttler
Charge, Electric Force, Electric Field, Flux, Gauss’s Law
(1) Coulomb’s Law for force F ≡ |F~ | on two point charges Q1 and Q2 at distance r:
F =k
|Q1 ||Q2 |
r2
with k = 8.99 × 109 Nm2 /C2 .
~ in terms of electric force F~ exerted on test charge q
(2) Definition of Electric Field E
~ generated by ”other” charges):
(with E
~
~ ≡F ;
E
q
~ .
hence F~ = q E
~
~ depends
Note E-field
is independent of the test charge q used to detect the electric force F~ : E
~
only on the ”other” charges which generate E.
~ by Point Charge Q, at an observation point P with distance
(3) Electric Field E ≡ |E|
r from Q:
|Q|
E=k 2
r
~ pointing radially away from positive charge, Q > 0; or radially towards negative
with E
charge, Q < 0.
~ by Uniform Surface Charge Density σ ≡ Q/A on a single
(4) Electric Field E ≡ |E|
planar surface of area A with total charge Q, in close proximity to the surface:
E=
|σ|
|Q|
=
2o
2o A
~ ∼
~
with E
= const (uniform E−field)
~ normal to the surface, pointing away
where o ≡ 1/(4πk) = 8.85 × 10−12 C2 /Nm2 ; and E
from positively charged (Q > 0) or towards negatively charged (Q < 0) surface.
~ in Planar Capacitor: between closely spaced, parallel, planar
(5) Electric field E ≡ |E|
plates of charges Q and −Q, and opposing surface areas A, without dielectric (κ = 1):
E=
|Q|
o A
~ ∼
~
with E
= const (uniform E−field)
~ normal to the plate surfaces, pointing from positive towards negative plate.
with E
~ is being generated
(6) Superposition Principle of Electric Field: If an electric field E
~ at any observation point P is the vector
by multiple charged objects (Q1 , Q2 , ...), then E
~ 1, E
~ 2 , ... that would be generated
sum (resultant vector) of the electric field contributions E
by each of the charged objects in isolation at that point P :
~ =E
~1 + E
~ 2 + ...
E
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Physics 1112
Spring 2009
University of Georgia
Instructor: HBSchüttler
~
(7) Electric Flux Φ of constant E-field
through planar surface of area A with the surface
o
~
normal at angle θ from E, with 0 ≤ θ ≤ 180o :
Φ = EA cos θ
~
(8) Gauss’s Law, relating total electric flux Φ(S) of the E-field
through a closed surface S
(with outward-directed surface normal) to the total charge Q(S) enclosed inside S:
Φ(S) =
1
Q(S)
o
Electric Potential, Potential Energy, Capacitance, Electric Energy Storage
(1) Definition of Electric Potential V and electric potential difference ∆V (also known
as ”voltage drop”), in terms of potential energy U and potential energy difference ∆U ,
~
respectively, for a test charge q moving or being moved through E-field:
V = U/q ,
∆V = ∆U/q ;
hence U = qV ,
∆U = q∆V .
~
~
Note that V or ∆V is a property of the E-field,
depends only on the E-field,
and is
therefore independent of the test charge q.
~ = const):
(2) Electric Potential Difference in a Uniform Electric Field (E
∆V = −E ∆s cos θ
where ∆V ≡ VB − VA is the electric potential difference between points B and A; the vector
~ with
∆~s points from A to B with length ∆s ≡ |∆~s|; and θ is the angle between ∆~s and E
~ (θ < 90o ); and
0o ≤ θ ≤ 180o . Hence, ∆V < 0 when moving from A to B in direction of E
o
~ (θ > 90 ).
∆V > 0 when moving from A to B against direction of E
(3) Electric Potential for Point Charge Electric Field (with E = k|Q|/r2 ):
V =k
Q
r
where r is the distance from point charge Q to observation point.
~ is being gener(4) Superposition Principle of Electric Potential: If an electric field E
ated by multiple charged objects (Q1 , Q2 , ...), then its electric potential V at any observation
point P is the scalar sum (sum of numbers) of the electric potential contributions V1 , V2 ,
... that would be generated by each of the charged objects in isolation at that point P ; and
likewise for the electric potential difference ∆V ≡ VB − VA between any points A and B:
V = V1 + V2 + ...
or
∆V = ∆V1 + ∆V2 + ...
(5) Definition of Capacitance: For two oppositely charged metallic objects a and b,
with −Q stored on a and Q stored on b, their electric potential difference V ≡ Vb − Va is
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Physics 1112
Spring 2009
University of Georgia
Instructor: HBSchüttler
proportional to the charge Q. The capacitance of the two metallic objects is then defined
as:
Q
Q
C≡
,
hence
Q = CV
or
V =
V
C
(6) Voltage and Capacitance of a Planar Capacitor: For two oppositely charged,
parallel planar metallic plates, each of opposing surface area A, closely spaced with distance
d, the voltage V and capacitance C are
|V | = Ed =
|Q|d
;
κo A
C≡
|Q|
A
= κo ≡ κ Co
|V |
d
where κ is the dielectric constant of the dielectric (insulating) material between the plates
and κ = 1 for vacuum or air, and Co ≡ o A/d is the capacitance without dielectric.
(7) Electric Field Energy Storage in a Capacitor: The energy UE required to build up
a charge Q and a voltage V = Q/C in a capacitor is stored as electric field energy between
the capacitor plates and it is given by
UE =
1 2 1
Q = CV 2
2C
2
Mechanics Memories: Velocity, Acceleration, Force, Energy, Power
(1) Velocity
~v =
∆~r
∆t
if constant; else ~v = lim
∆~r
∆t→0 ∆t
~a =
∆~v
∆t
if constant; else ~a = lim
(2) Acceleration
∆~v
∆t→0 ∆t
(3) Constant-Acceleration Motion: for ∆~r ≡ ~rf − ~ri and ∆~v ≡ ~vf − ~vi
∆~r =
1
(~vi + ~vf ) t ;
2
∆~r = ~vi t +
1
~a t2 ;
2
∆~v = ~a t .
(4) Newton’s 2nd Law:
m~a = F~
(5) Kinetic Knergy:
1
K = m v2
2
(6) Energy Conservation Law for ∆K ≡ Kf − Ki and ∆U ≡ Uf − Ui :
Ki + Ui = Kf + Uf
or
∆K + ∆U = 0
(7) Mechanical Power: P =rate of work done by force F~ on an object moving at speed
~v , with ~v pointing at an angle θ from F~ and 0o ≤ θ ≤ 180o :
P = F v cos θ
9
Physics 1112
Spring 2009
University of Georgia
Instructor: HBSchüttler
Algebra and Trigonometry
2
az + bz + c = 0
sin θ =
opp
,
hyp
⇒
cos θ =
z=
adj
,
hyp
−b ±
√
b2 − 4ac
2a
tan θ =
opp
sin θ
=
adj
cos θ
sin2 θ + cos2 θ = 1
For very small angles θ (with |θ| 90o ):
sin θ ∼
= tan θ ∼
= θ (in radians)
Numerical Data
Acceleration of gravity (on Earth):
Speed of light in vacuum:
Coulomb’s constant:
Electron mass:
Proton mass:
c = 3.00 × 108 m/s
k = 8.99 × 109 Nm2 /C2
Permittivity of vacuum:
Elementary charge:
g = 9.81m/s2
o ≡ 1/(4πk) = 8.85 × 10−12 C2 /Nm2
e = 1.60 × 10−19 C
me = 9.11 × 10−31 kg
mp = 1.67 × 10−27 kg
Other numerical inputs will be provided with each problem statement.
SI numerical prefixes:
y = yocto =10−24 , z = zepto =10−21 , a = atto =10−18 , f = femto =10−15 , p = pico =10−12 ,
n = nano =10−9 , µ= micro =10−6 , m = milli =10−3 , c = centi =10−2 , d = deci =10−1 ,
da = deca =10+1 , h = hecto =10+2 , k = kilo =10+3 , M = Mega =10+6 , G = Giga =10+9 ,
T = Tera =10+12 , P = Peta =10+15 , E = Exa =10+18 , Z = Zetta =10+21 , Y = Yotta =10+24 .
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