56
Preparing for the GRE: Strategies for Success Welcome – we’ll get started soon Dial in or use your computer’s microphone and speakers. Submit questions via the Questions panel on the right. This session is being recorded. The recording will be sent to you via a follow up email. Make sure to sign up to receive information about future APS webinars at: www.aps.org/careers/guidance/webinars

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Page 1: Preparing for the GRE: Strategies for Success - APS …Preparing for the GRE: Strategies for Success Welcome – we’ll get started soon • Dial in or use your computer’s microphone

Preparing for the GRE: Strategies for Success

Welcome – we’ll get started soon • Dial in or use your computer’s microphone and

speakers. • Submit questions via the Questions panel on the right. • This session is being recorded. • The recording will be sent to you via a follow up email.

Make sure to sign up to receive information about future APS webinars at: www.aps.org/careers/guidance/webinars

Page 2: Preparing for the GRE: Strategies for Success - APS …Preparing for the GRE: Strategies for Success Welcome – we’ll get started soon • Dial in or use your computer’s microphone

Preparing for the Physics GRE: Strategies for Success

Yoni KahnMarch 7, 2017

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Physics GRE: the basics

• 100 questions, 170 minutes

• Multiple choice, 5 answers

• Standard (and less standard) undergrad physics

Classical mech: 20% E+M: 18% Optics/waves: 9% Thermo/stat mech: 10% Quantum: 12%~70% core subjects

Atomic physics: 10% Special relativity: 6% Lab methods: 6% Specialized topics: 9%

~30% “grab bag”

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Reference materials

• “Conquering the Physics GRE” - available on Amazon - review material and practice questions for each

subject area - 3 full-length practice tests - tips and tricks specific to Physics GRE

• ETS practice material - most recent (2008) at www.ets.org - previous (2001, 1996, 1992, 1986) at grephysics.net - 2001 and 2008 are most representative of current test

This is a test of outside knowledge: you will need to memorize some things!

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Tips and Tricks: Derive, don’t memorize!

ETS 2001 #3

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Tips and Tricks: Derive, don’t memorize!

Formula for period of circular orbit?

ETS 2001 #3

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Tips and Tricks: Derive, don’t memorize!

OR: uniform circular motion + Newton’s law of gravity

derive the formula you need

Formula for period of circular orbit?

ETS 2001 #3

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Tips and Tricks: Derive, don’t memorize!

Fcentripetal =mv2

R

ETS 2001 #3

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Tips and Tricks: Derive, don’t memorize!

Fgrav =GmM

R2Fcentripetal =

mv2

R

ETS 2001 #3

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Tips and Tricks: Derive, don’t memorize!

Fgrav =GmM

R2Fcentripetal =

mv2

R

Fcentripetal = Fgrav =) v =

rGM

R

ETS 2001 #3

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Tips and Tricks: Derive, don’t memorize!

Fcentripetal = Fgrav =) v =

rGM

R

T =2⇡R

v/ R3/2

ETS 2001 #3

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Tips and Tricks: Derive, don’t memorize!

Fcentripetal = Fgrav =) v =

rGM

R

T =2⇡R

v/ R3/2

Kepler’s Third Law!

ETS 2001 #3

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Tips and Tricks: Derive, don’t memorize!

Your turn!

ETS 2001 #62

Numbers from front of test book:e = 1.60⇥ 10�19 C

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Tips and Tricks: Derive, don’t memorize!

ETS 2001 #62

FB = qvB = 2evBFcentripetal =mv2

R

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Tips and Tricks: Derive, don’t memorize!

ETS 2001 #62

FB = qvB = 2evBFcentripetal =mv2

R

Fcentripetal = FB =) m =2eBR

v

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Tips and Tricks: Derive, don’t memorize!

ETS 2001 #62

FB = qvB = 2evBFcentripetal =mv2

R

f =v

2⇡R=) m =

eB

⇡f

Fcentripetal = FB =) m =2eBR

v given numbersmean simple

arithmetic

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Tips and Tricks: Dimensional Analysis

Three fundamental units: mass, length, time

Everything in classical mechanics can be expressed as products of powers of these! (For EM, need charge also)

Sometimes easier to work with composite units (electric and magnetic fields especially, also energy)

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Tips and Tricks: Dimensional Analysis

ETS 2001 #57

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Tips and Tricks: Dimensional Analysis

ETS 2001 #57

Forget fluid dynamics! Want something with units of force

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Tips and Tricks: Dimensional Analysis

ETS 2001 #57[⇢] = [M ][L]�3

[A] = [L]2

[v] = [L][T ]�1

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Tips and Tricks: Dimensional Analysis

ETS 2001 #57[⇢] = [M ][L]�3

[A] = [L]2

[v] = [L][T ]�1

[F ] = [M ][L][T ]�2

F = ⇢xAyvz

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Tips and Tricks: Dimensional Analysis

ETS 2001 #57[⇢] = [M ][L]�3

[A] = [L]2

[v] = [L][T ]�1

[F ] = [M ][L][T ]�2

F = ⇢xAyvz

Algebra or just staring at it: x = 1, y = 1, v = 2

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Tips and Tricks: Dimensional Analysis

ETS 2001 #57[⇢] = [M ][L]�3

[A] = [L]2

[v] = [L][T ]�1

[F ] = [M ][L][T ]�2

F = ⇢xAyvz

Algebra or just staring at it: x = 1, y = 1, v = 2

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Tips and Tricks: Dimensional Analysis

ETS 2001 #57[⇢] = [M ][L]�3

[A] = [L]2

[v] = [L][T ]�1

[F ] = [M ][L][T ]�2

F = ⇢xAyvz

Algebra or just staring at it: x = 1, y = 1, v = 2

if eqs. have no solution, need more quantities with units,

hence g

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Tips and Tricks: Dimensional Analysis

ETS 2001 #65

Your turn!

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Tips and Tricks: Dimensional Analysis

ETS 2001 #65

h⌫ kTand both have units of energy:

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Tips and Tricks: Dimensional Analysis

ETS 2001 #65

h⌫ kTand both have units of energy:C has same unit as k

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Tips and Tricks: Dimensional Analysis

ETS 2001 #65

h⌫ kTand both have units of energy:C has same unit as k

Taylor expand, or remember equipartition

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Tips & Tricks: Limiting Cases

ETS 2001 #60

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Tips & Tricks: Limiting Cases

Send parameter values to their limits

Recall Gauss’s Law: flux proportional to enclosed charge

ETS 2001 #60

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Tips & Tricks: Limiting Cases

Send parameter values to their limits

x ! R

Recall Gauss’s Law: flux proportional to enclosed charge

ETS 2001 #60

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Tips & Tricks: Limiting Cases

Send parameter values to their limits

x ! R flux should vanish

Recall Gauss’s Law: flux proportional to enclosed charge

ETS 2001 #60

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Tips & Tricks: Limiting Cases

Send parameter values to their limits

x ! R flux should vanish

x ! �R

Recall Gauss’s Law: flux proportional to enclosed charge

ETS 2001 #60

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Tips & Tricks: Limiting Cases

Send parameter values to their limits

x ! R flux should vanish

x ! �R flux should also vanish!

Recall Gauss’s Law: flux proportional to enclosed charge

ETS 2001 #60

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Tips & Tricks: Limiting Cases

Send parameter values to their limits

x ! R flux should vanish

x ! �R flux should also vanish!

x ! 0

Recall Gauss’s Law: flux proportional to enclosed charge

ETS 2001 #60

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Tips & Tricks: Limiting Cases

Send parameter values to their limits

x ! R flux should vanish

x ! �R flux should also vanish!

x ! 0 circle, expect

Recall Gauss’s Law: flux proportional to enclosed charge

ETS 2001 #60

⇡R2

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Tips & Tricks: Limiting Cases

Send parameter values to their limits

x ! R flux should vanish

x ! �R flux should also vanish!

Get choice D, no complicated geometry!

x ! 0

Recall Gauss’s Law: flux proportional to enclosed charge

ETS 2001 #60

circle, expect ⇡R2

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Tips & Tricks: Limiting Cases

007626-54721 • ETS/ GRE Practicing to Take the Lit in English Test • RI51621 • OC 5/9/01revs 5/18/01 rkc • revs 6/29/01 rKc* • revs 7/20/01 sb • preflight 8/10/01 chw • revs 5/16/02 jjh • revs 6/12/02 jjh • preflight 6/27/02 jjh • 1stRevs…3.5.04…kaj • preflight 04/01/04 mwr • dr01 4/22/10 mc • dr01revs 5/7/10 mc • pdf 5/10/10 mc • Drft02 5/20/10 jdb • Revs Drft02 5/26/10 jdb • PDF Drft002/5/26/10 jdb • Preflight 6/2/10 jdb • dr01 5/4/11 mc • RevsDrft01 5/12/11 jdb • PDF Drft01 5/12/11 jdb • Drft02 5/23/11 jdb • PDF Drft02 5/24/11 jdb • Preflight 6/6/11 jdb

48

Unauthorized copying or reuse of any part of this page is illegal. GO ON TO THE NEXT PAGE.

-40-

58. In the figure above, block A has mass

mA = 25 kg and block B has mass mB = 10 kg.

Both blocks move with constant acceleration

a = 2 m/s2 to the right, and the coefficient of static

friction between the two blocks is s = 0.8. The

static frictional force acting between the blocks is

(A) 20 N (B) 50 N (C) 78 N (D) 196 N (E) 274 N

59. A simple pendulum of length l is suspended

from the ceiling of an elevator that is accelerating upward with constant acceleration a . For small oscillations, the period, T, of the pendulum is

(A) 2 lTg

��

(B) 2 lTg a

���

(C) 2 lTg a

���

(D) � �2 l aTg g a

���

(E) � �

2g alT

g a�

��

60. Three long, straight wires in the xz-plane, each carrying current I , cross at the origin of coordinates, as shown in the figure above. Let �̂ , �̂ , and �̂ denote the unit vectors in the x-, y-, and z-directions, respectively. The magnetic field B as a function of x, with y = 0 and z = 0, is

(A) 03ˆ

2Ix

��B �

(B) 03ˆ

2Ix

��B �

(C) � �0 ˆ1 2 22

Ix

�� �B �

(D) 0 ˆ2

Ix

��B �

(E) 0 ˆ2

Ix

��B �

Your turn!

ETS 2008 #59

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Tips & Tricks: Limiting Cases

007626-54721 • ETS/ GRE Practicing to Take the Lit in English Test • RI51621 • OC 5/9/01revs 5/18/01 rkc • revs 6/29/01 rKc* • revs 7/20/01 sb • preflight 8/10/01 chw • revs 5/16/02 jjh • revs 6/12/02 jjh • preflight 6/27/02 jjh • 1stRevs…3.5.04…kaj • preflight 04/01/04 mwr • dr01 4/22/10 mc • dr01revs 5/7/10 mc • pdf 5/10/10 mc • Drft02 5/20/10 jdb • Revs Drft02 5/26/10 jdb • PDF Drft002/5/26/10 jdb • Preflight 6/2/10 jdb • dr01 5/4/11 mc • RevsDrft01 5/12/11 jdb • PDF Drft01 5/12/11 jdb • Drft02 5/23/11 jdb • PDF Drft02 5/24/11 jdb • Preflight 6/6/11 jdb

48

Unauthorized copying or reuse of any part of this page is illegal. GO ON TO THE NEXT PAGE.

-40-

58. In the figure above, block A has mass

mA = 25 kg and block B has mass mB = 10 kg.

Both blocks move with constant acceleration

a = 2 m/s2 to the right, and the coefficient of static

friction between the two blocks is s = 0.8. The

static frictional force acting between the blocks is

(A) 20 N (B) 50 N (C) 78 N (D) 196 N (E) 274 N

59. A simple pendulum of length l is suspended

from the ceiling of an elevator that is accelerating upward with constant acceleration a . For small oscillations, the period, T, of the pendulum is

(A) 2 lTg

��

(B) 2 lTg a

���

(C) 2 lTg a

���

(D) � �2 l aTg g a

���

(E) � �

2g alT

g a�

��

60. Three long, straight wires in the xz-plane, each carrying current I , cross at the origin of coordinates, as shown in the figure above. Let �̂ , �̂ , and �̂ denote the unit vectors in the x-, y-, and z-directions, respectively. The magnetic field B as a function of x, with y = 0 and z = 0, is

(A) 03ˆ

2Ix

��B �

(B) 03ˆ

2Ix

��B �

(C) � �0 ˆ1 2 22

Ix

�� �B �

(D) 0 ˆ2

Ix

��B �

(E) 0 ˆ2

Ix

��B �

ETS 2008 #59

a ! 0

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Tips & Tricks: Limiting Cases

007626-54721 • ETS/ GRE Practicing to Take the Lit in English Test • RI51621 • OC 5/9/01revs 5/18/01 rkc • revs 6/29/01 rKc* • revs 7/20/01 sb • preflight 8/10/01 chw • revs 5/16/02 jjh • revs 6/12/02 jjh • preflight 6/27/02 jjh • 1stRevs…3.5.04…kaj • preflight 04/01/04 mwr • dr01 4/22/10 mc • dr01revs 5/7/10 mc • pdf 5/10/10 mc • Drft02 5/20/10 jdb • Revs Drft02 5/26/10 jdb • PDF Drft002/5/26/10 jdb • Preflight 6/2/10 jdb • dr01 5/4/11 mc • RevsDrft01 5/12/11 jdb • PDF Drft01 5/12/11 jdb • Drft02 5/23/11 jdb • PDF Drft02 5/24/11 jdb • Preflight 6/6/11 jdb

48

Unauthorized copying or reuse of any part of this page is illegal. GO ON TO THE NEXT PAGE.

-40-

58. In the figure above, block A has mass

mA = 25 kg and block B has mass mB = 10 kg.

Both blocks move with constant acceleration

a = 2 m/s2 to the right, and the coefficient of static

friction between the two blocks is s = 0.8. The

static frictional force acting between the blocks is

(A) 20 N (B) 50 N (C) 78 N (D) 196 N (E) 274 N

59. A simple pendulum of length l is suspended

from the ceiling of an elevator that is accelerating upward with constant acceleration a . For small oscillations, the period, T, of the pendulum is

(A) 2 lTg

��

(B) 2 lTg a

���

(C) 2 lTg a

���

(D) � �2 l aTg g a

���

(E) � �

2g alT

g a�

��

60. Three long, straight wires in the xz-plane, each carrying current I , cross at the origin of coordinates, as shown in the figure above. Let �̂ , �̂ , and �̂ denote the unit vectors in the x-, y-, and z-directions, respectively. The magnetic field B as a function of x, with y = 0 and z = 0, is

(A) 03ˆ

2Ix

��B �

(B) 03ˆ

2Ix

��B �

(C) � �0 ˆ1 2 22

Ix

�� �B �

(D) 0 ˆ2

Ix

��B �

(E) 0 ˆ2

Ix

��B �

ETS 2008 #59

a ! 0 nothing should blow up or vanish

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Tips & Tricks: Limiting Cases

007626-54721 • ETS/ GRE Practicing to Take the Lit in English Test • RI51621 • OC 5/9/01revs 5/18/01 rkc • revs 6/29/01 rKc* • revs 7/20/01 sb • preflight 8/10/01 chw • revs 5/16/02 jjh • revs 6/12/02 jjh • preflight 6/27/02 jjh • 1stRevs…3.5.04…kaj • preflight 04/01/04 mwr • dr01 4/22/10 mc • dr01revs 5/7/10 mc • pdf 5/10/10 mc • Drft02 5/20/10 jdb • Revs Drft02 5/26/10 jdb • PDF Drft002/5/26/10 jdb • Preflight 6/2/10 jdb • dr01 5/4/11 mc • RevsDrft01 5/12/11 jdb • PDF Drft01 5/12/11 jdb • Drft02 5/23/11 jdb • PDF Drft02 5/24/11 jdb • Preflight 6/6/11 jdb

48

Unauthorized copying or reuse of any part of this page is illegal. GO ON TO THE NEXT PAGE.

-40-

58. In the figure above, block A has mass

mA = 25 kg and block B has mass mB = 10 kg.

Both blocks move with constant acceleration

a = 2 m/s2 to the right, and the coefficient of static

friction between the two blocks is s = 0.8. The

static frictional force acting between the blocks is

(A) 20 N (B) 50 N (C) 78 N (D) 196 N (E) 274 N

59. A simple pendulum of length l is suspended

from the ceiling of an elevator that is accelerating upward with constant acceleration a . For small oscillations, the period, T, of the pendulum is

(A) 2 lTg

��

(B) 2 lTg a

���

(C) 2 lTg a

���

(D) � �2 l aTg g a

���

(E) � �

2g alT

g a�

��

60. Three long, straight wires in the xz-plane, each carrying current I , cross at the origin of coordinates, as shown in the figure above. Let �̂ , �̂ , and �̂ denote the unit vectors in the x-, y-, and z-directions, respectively. The magnetic field B as a function of x, with y = 0 and z = 0, is

(A) 03ˆ

2Ix

��B �

(B) 03ˆ

2Ix

��B �

(C) � �0 ˆ1 2 22

Ix

�� �B �

(D) 0 ˆ2

Ix

��B �

(E) 0 ˆ2

Ix

��B �

ETS 2008 #59

a = �g

a ! 0 nothing should blow up or vanish

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Tips & Tricks: Limiting Cases

007626-54721 • ETS/ GRE Practicing to Take the Lit in English Test • RI51621 • OC 5/9/01revs 5/18/01 rkc • revs 6/29/01 rKc* • revs 7/20/01 sb • preflight 8/10/01 chw • revs 5/16/02 jjh • revs 6/12/02 jjh • preflight 6/27/02 jjh • 1stRevs…3.5.04…kaj • preflight 04/01/04 mwr • dr01 4/22/10 mc • dr01revs 5/7/10 mc • pdf 5/10/10 mc • Drft02 5/20/10 jdb • Revs Drft02 5/26/10 jdb • PDF Drft002/5/26/10 jdb • Preflight 6/2/10 jdb • dr01 5/4/11 mc • RevsDrft01 5/12/11 jdb • PDF Drft01 5/12/11 jdb • Drft02 5/23/11 jdb • PDF Drft02 5/24/11 jdb • Preflight 6/6/11 jdb

48

Unauthorized copying or reuse of any part of this page is illegal. GO ON TO THE NEXT PAGE.

-40-

58. In the figure above, block A has mass

mA = 25 kg and block B has mass mB = 10 kg.

Both blocks move with constant acceleration

a = 2 m/s2 to the right, and the coefficient of static

friction between the two blocks is s = 0.8. The

static frictional force acting between the blocks is

(A) 20 N (B) 50 N (C) 78 N (D) 196 N (E) 274 N

59. A simple pendulum of length l is suspended

from the ceiling of an elevator that is accelerating upward with constant acceleration a . For small oscillations, the period, T, of the pendulum is

(A) 2 lTg

��

(B) 2 lTg a

���

(C) 2 lTg a

���

(D) � �2 l aTg g a

���

(E) � �

2g alT

g a�

��

60. Three long, straight wires in the xz-plane, each carrying current I , cross at the origin of coordinates, as shown in the figure above. Let �̂ , �̂ , and �̂ denote the unit vectors in the x-, y-, and z-directions, respectively. The magnetic field B as a function of x, with y = 0 and z = 0, is

(A) 03ˆ

2Ix

��B �

(B) 03ˆ

2Ix

��B �

(C) � �0 ˆ1 2 22

Ix

�� �B �

(D) 0 ˆ2

Ix

��B �

(E) 0 ˆ2

Ix

��B �

ETS 2008 #59

Equivalence Principle: pendulum is “weightless”a = �g

a ! 0 nothing should blow up or vanish

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Tips & Tricks: Numbers and Estimation

The only 5 numbers you need to memorize for the GRE:

• 13.6 eV - hydrogen atom binding energy • 511 keV - mass of the electron (units of c2) • 1.22 - coefficient in Rayleigh criterion • 2.7 K - temperature of cosmic microwave background • 3 x 10-3 m K - Wien’s law coefficient

Everything else should be given on formula sheet or in the exam questions themselves

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15

10. Which of the following properties of the hydrogen atom can be predicted mostaccurately from the simple Bohr model?

(A) Energy differences between states(B) Angular momentum of the ground state(C) Degeneracy of states(D) Transition probabilities(E) Selection rules for transitions

11. The ratio of the nuclear radius to the atomic radius of an element near the middle ofthe periodic table is most nearly

(A) 10 2− (B) 10 5− (C) 10 8− (D) 10 11− (E) 10 14−

12. The total energy necessary to remove all three electrons from a lithium atom is mostnearly

(A) 2 MeV (B) 2 KeV (C) 200 eV (D) 20 eV (E) 2 eV

FluorescentScreen

ThinCopperFoil

ElectronBeam

13. In order to observe a ring diffraction pattern on the screen shown above, which ofthe following conditions must be met?

(A) The electron beam must be polarized.(B) The electron beam must be approximately monoenergetic.(C) The copper foil must be a single crystal specimen.(D) The copper foil must be of uniform thickness.(E) The electron beam must strike the foil at normal incidence.

(from ETS supplemental material)

Tips & Tricks: Numbers and Estimation

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15

10. Which of the following properties of the hydrogen atom can be predicted mostaccurately from the simple Bohr model?

(A) Energy differences between states(B) Angular momentum of the ground state(C) Degeneracy of states(D) Transition probabilities(E) Selection rules for transitions

11. The ratio of the nuclear radius to the atomic radius of an element near the middle ofthe periodic table is most nearly

(A) 10 2− (B) 10 5− (C) 10 8− (D) 10 11− (E) 10 14−

12. The total energy necessary to remove all three electrons from a lithium atom is mostnearly

(A) 2 MeV (B) 2 KeV (C) 200 eV (D) 20 eV (E) 2 eV

FluorescentScreen

ThinCopperFoil

ElectronBeam

13. In order to observe a ring diffraction pattern on the screen shown above, which ofthe following conditions must be met?

(A) The electron beam must be polarized.(B) The electron beam must be approximately monoenergetic.(C) The copper foil must be a single crystal specimen.(D) The copper foil must be of uniform thickness.(E) The electron beam must strike the foil at normal incidence.

(from ETS supplemental material)

convert energy to length with ~c ⇡ 200 MeV · fm = 200 eV · nm

Tips & Tricks: Numbers and Estimation

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15

10. Which of the following properties of the hydrogen atom can be predicted mostaccurately from the simple Bohr model?

(A) Energy differences between states(B) Angular momentum of the ground state(C) Degeneracy of states(D) Transition probabilities(E) Selection rules for transitions

11. The ratio of the nuclear radius to the atomic radius of an element near the middle ofthe periodic table is most nearly

(A) 10 2− (B) 10 5− (C) 10 8− (D) 10 11− (E) 10 14−

12. The total energy necessary to remove all three electrons from a lithium atom is mostnearly

(A) 2 MeV (B) 2 KeV (C) 200 eV (D) 20 eV (E) 2 eV

FluorescentScreen

ThinCopperFoil

ElectronBeam

13. In order to observe a ring diffraction pattern on the screen shown above, which ofthe following conditions must be met?

(A) The electron beam must be polarized.(B) The electron beam must be approximately monoenergetic.(C) The copper foil must be a single crystal specimen.(D) The copper foil must be of uniform thickness.(E) The electron beam must strike the foil at normal incidence.

(from ETS supplemental material)

Nuclear scale?

Atomic scale?

convert energy to length with ~c ⇡ 200 MeV · fm = 200 eV · nm

Tips & Tricks: Numbers and Estimation

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15

10. Which of the following properties of the hydrogen atom can be predicted mostaccurately from the simple Bohr model?

(A) Energy differences between states(B) Angular momentum of the ground state(C) Degeneracy of states(D) Transition probabilities(E) Selection rules for transitions

11. The ratio of the nuclear radius to the atomic radius of an element near the middle ofthe periodic table is most nearly

(A) 10 2− (B) 10 5− (C) 10 8− (D) 10 11− (E) 10 14−

12. The total energy necessary to remove all three electrons from a lithium atom is mostnearly

(A) 2 MeV (B) 2 KeV (C) 200 eV (D) 20 eV (E) 2 eV

FluorescentScreen

ThinCopperFoil

ElectronBeam

13. In order to observe a ring diffraction pattern on the screen shown above, which ofthe following conditions must be met?

(A) The electron beam must be polarized.(B) The electron beam must be approximately monoenergetic.(C) The copper foil must be a single crystal specimen.(D) The copper foil must be of uniform thickness.(E) The electron beam must strike the foil at normal incidence.

(from ETS supplemental material)

Nuclear scale? • proton has mass of about 1 GeV • “size” close to femtometer (10-15 m) • Z = 50, probably 10-100 fm

Atomic scale?

convert energy to length with ~c ⇡ 200 MeV · fm = 200 eV · nm

Tips & Tricks: Numbers and Estimation

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15

10. Which of the following properties of the hydrogen atom can be predicted mostaccurately from the simple Bohr model?

(A) Energy differences between states(B) Angular momentum of the ground state(C) Degeneracy of states(D) Transition probabilities(E) Selection rules for transitions

11. The ratio of the nuclear radius to the atomic radius of an element near the middle ofthe periodic table is most nearly

(A) 10 2− (B) 10 5− (C) 10 8− (D) 10 11− (E) 10 14−

12. The total energy necessary to remove all three electrons from a lithium atom is mostnearly

(A) 2 MeV (B) 2 KeV (C) 200 eV (D) 20 eV (E) 2 eV

FluorescentScreen

ThinCopperFoil

ElectronBeam

13. In order to observe a ring diffraction pattern on the screen shown above, which ofthe following conditions must be met?

(A) The electron beam must be polarized.(B) The electron beam must be approximately monoenergetic.(C) The copper foil must be a single crystal specimen.(D) The copper foil must be of uniform thickness.(E) The electron beam must strike the foil at normal incidence.

(from ETS supplemental material)

Nuclear scale? • proton has mass of about 1 GeV • “size” close to femtometer (10-15 m) • Z = 50, probably 10-100 fm

Atomic scale?• 13.6 eV binding energy for hydrogen • Bohr radius is 10-10 m • maybe 10-9 m for Z = 50

convert energy to length with ~c ⇡ 200 MeV · fm = 200 eV · nm

Tips & Tricks: Numbers and Estimation

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15

10. Which of the following properties of the hydrogen atom can be predicted mostaccurately from the simple Bohr model?

(A) Energy differences between states(B) Angular momentum of the ground state(C) Degeneracy of states(D) Transition probabilities(E) Selection rules for transitions

11. The ratio of the nuclear radius to the atomic radius of an element near the middle ofthe periodic table is most nearly

(A) 10 2− (B) 10 5− (C) 10 8− (D) 10 11− (E) 10 14−

12. The total energy necessary to remove all three electrons from a lithium atom is mostnearly

(A) 2 MeV (B) 2 KeV (C) 200 eV (D) 20 eV (E) 2 eV

FluorescentScreen

ThinCopperFoil

ElectronBeam

13. In order to observe a ring diffraction pattern on the screen shown above, which ofthe following conditions must be met?

(A) The electron beam must be polarized.(B) The electron beam must be approximately monoenergetic.(C) The copper foil must be a single crystal specimen.(D) The copper foil must be of uniform thickness.(E) The electron beam must strike the foil at normal incidence.

(from ETS supplemental material)

Nuclear scale? • proton has mass of about 1 GeV • “size” close to femtometer (10-15 m) • Z = 50, probably 10-100 fm

Atomic scale?• 13.6 eV binding energy for hydrogen • Bohr radius is 10-10 m • maybe 10-9 m for Z = 50

convert energy to length with

Ratio is closest to 10-5

~c ⇡ 200 MeV · fm = 200 eV · nm

Tips & Tricks: Numbers and Estimation

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Tips & Tricks: Numbers and Estimation

Your turn!

ETS 2001 #13

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Tips & Tricks: Numbers and Estimation

ETS 2001 #13

Small angle approx: sin ✓ ⇡ ✓

D sin ✓ = 1.22�

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Tips & Tricks: Numbers and Estimation

ETS 2001 #13

Small angle approx: sin ✓ ⇡ ✓

D ⇡ 1.22�

✓⇡ 2.5 cm

D sin ✓ = 1.22�

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Tips & Tricks - Answer Types

Easier:

Different units

Order of magnitude

“Which power of 3?”

Different limiting cases

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Tips & Tricks - Answer Types

Harder:

Same units, different numbers Random numbers

Work problem slowly, don’t get distracted by answer choices!

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Tips & Tricks - Fermi problems

“How many piano tuners are there in New York City?” “How many photons hit the Earth every day?”

Solving problems like these require quick-and-dirty estimates paired with good physical intuition -

good practice for the GRE!

See “Conquering” Ch. 9 sec. 6 for a worked example, or V. Weisskopf, “Modern Physics from an Elementary

Point of View”http://cds.cern.ch/record/274976/files/CERN-70-08.pdf?version=1

(or XKCD’s “What If” series)

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Wrapping up

Please feel free to email with further questions! [email protected]

Best of luck studying!