name: setiawan office: s13-02-09, phys. departm. phone: 6516-2988 email:...

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Name: Setiawan Office: S13-02-09, Phys. Departm. Phone: 6516-2988 Email: [email protected] Consultation: Wed. 10.00- 12.00 Tutorial 1 Where are We?????? GEM2507 Physical Questions in Everyday Life

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Page 1: Name: Setiawan Office: S13-02-09, Phys. Departm. Phone: 6516-2988 Email: physetia@nus.edu.sgphysetia@nus.edu.sg Consultation: Wed. 10.00-12.00 Tutorial

Name: SetiawanOffice: S13-02-09, Phys. Departm.Phone: 6516-2988 Email: [email protected]: Wed. 10.00-12.00

Tutorial 1

Where are We??????

GEM2507

Physical Questions in Everyday Life

Page 2: Name: Setiawan Office: S13-02-09, Phys. Departm. Phone: 6516-2988 Email: physetia@nus.edu.sgphysetia@nus.edu.sg Consultation: Wed. 10.00-12.00 Tutorial

1. What is a distance of 5 kilo parsec in lightyears?

A minute of arc, arcminute, (MOA) = 1/60 of 1o An arcsecond = 1/60 * arcminute The parsec ("parallax of one arcsecond", symbol

pc) = 30 trillion km or 3.3 light years. Defined as the distance from the sun at which two

imaginary lines—one projected from the Earth, and one projected from the sun at a right angle to a third line connecting the Earth and the sun—intersect in space at an angle of 1 arcsecond

Page 3: Name: Setiawan Office: S13-02-09, Phys. Departm. Phone: 6516-2988 Email: physetia@nus.edu.sgphysetia@nus.edu.sg Consultation: Wed. 10.00-12.00 Tutorial

Calculating the value of a parsec

A B

Page 4: Name: Setiawan Office: S13-02-09, Phys. Departm. Phone: 6516-2988 Email: physetia@nus.edu.sgphysetia@nus.edu.sg Consultation: Wed. 10.00-12.00 Tutorial

Calculating the value of a parsec

S = Sun E = Earth D = point in space 1 parsec from the Sun

1 AU = 149,597,870,700 m1 parsec ≈ 3.085 678×1016 m ≈ 3.261 564 light-years.

Page 5: Name: Setiawan Office: S13-02-09, Phys. Departm. Phone: 6516-2988 Email: physetia@nus.edu.sgphysetia@nus.edu.sg Consultation: Wed. 10.00-12.00 Tutorial

Answer for question 1

5 kiloparsec = 5 * 3261.636

= 16308.181 light years

Page 6: Name: Setiawan Office: S13-02-09, Phys. Departm. Phone: 6516-2988 Email: physetia@nus.edu.sgphysetia@nus.edu.sg Consultation: Wed. 10.00-12.00 Tutorial

Distances less than a parsec

Distances measured in fractions of a parsec usually involve objects within a single star system. So, for example:one astronomical unit (AU) - the distance

from the Sun to the Earth - is 4.85×10−6 pc.

Page 7: Name: Setiawan Office: S13-02-09, Phys. Departm. Phone: 6516-2988 Email: physetia@nus.edu.sgphysetia@nus.edu.sg Consultation: Wed. 10.00-12.00 Tutorial

Parsecs and kiloparsecs Distances measured in parsecs include distances

between nearby stars, such as those in the same spiral arm or globular cluster. For example Second Nearest star to the Earth (Proxima Centauri)

1.29 parsecs away. The center of the Milky Way is about 8 kpc from the

Earth, and the Milky Way is about 30 kpc across. Andromeda Galaxy (M31), the most distant object

visible to the naked eye, is a little under 800 kpc away from the Earth.

Page 8: Name: Setiawan Office: S13-02-09, Phys. Departm. Phone: 6516-2988 Email: physetia@nus.edu.sgphysetia@nus.edu.sg Consultation: Wed. 10.00-12.00 Tutorial

Megaparsecs and gigaparsecs

Astronomers typically measure the distances between neighboring galaxies and galaxy clusters in megaparsecs. For example:The Andromeda Galaxy is 0.77 Mpc away

from the Earth.

Page 9: Name: Setiawan Office: S13-02-09, Phys. Departm. Phone: 6516-2988 Email: physetia@nus.edu.sgphysetia@nus.edu.sg Consultation: Wed. 10.00-12.00 Tutorial

2. Would it be a good idea to measure the distance to the closest galaxy outside our own by triangulation?

No, as the parallax angle would be extremely small if it was used to measure the distance to the closest galaxy from our own galaxy. Indeed, the maximum distance measurable by triangulation is about 50 parsecs, only enough to explore our sun’s immediate neighborhood and far short of even being sufficient to map our own galaxy, the Milky Way

Page 10: Name: Setiawan Office: S13-02-09, Phys. Departm. Phone: 6516-2988 Email: physetia@nus.edu.sgphysetia@nus.edu.sg Consultation: Wed. 10.00-12.00 Tutorial

Method used to measure distances in universe

MethodDistance

(pc) ObjectTime(yr

)

Hubble's Law 109-1010 Quasars 1011

Apparent luminosity - Galaxies 108 Virgo Cluster 108

Apparent luminosity - Super Giants 106-107

Andromeda Cluster 107

Cepheid Variables - Type II 105

Andromeda Cluster 105

Cepheid Variables - Type I 101-104

Center of Milky Way 103

Parallax 100 Alpha Centauri 101

Page 11: Name: Setiawan Office: S13-02-09, Phys. Departm. Phone: 6516-2988 Email: physetia@nus.edu.sgphysetia@nus.edu.sg Consultation: Wed. 10.00-12.00 Tutorial

3. If we have a type-I Cepheid with the period of luminosity being approximately 140 hours and an apparent luminosity of 5 x 10-12 watt. What is it's distance from us in lightyears?

From Figure 1.9 in the lecture note, we get the absolute luminosity (L) for period 140 hrs = 5.04 x 105 s, L = Ls = 5 * 4 x 1026 W

= 2 x 1027 W The apparent luminosity is

24 d

LLA

2718

12

2 105.63 10 182.62

4 4 (5 10 )A

L xd x m pc

L x lightyears4.596

Page 12: Name: Setiawan Office: S13-02-09, Phys. Departm. Phone: 6516-2988 Email: physetia@nus.edu.sgphysetia@nus.edu.sg Consultation: Wed. 10.00-12.00 Tutorial

4. Joan (weighing 70kg) is running at a constant speed down a slope with an angle of 6 degrees with a speed of 10km/h. What is her acceleration? What is her momentum? (Use standard units!)

N

WWy

x

y

f

Constant speed = no acceleration

v = 10 km/h = 10/3.6 = 2.78 m/s

p = m v = 70 x 2.78 = 194.6 kg m/s

Page 13: Name: Setiawan Office: S13-02-09, Phys. Departm. Phone: 6516-2988 Email: physetia@nus.edu.sgphysetia@nus.edu.sg Consultation: Wed. 10.00-12.00 Tutorial

5. Give the value of the Hubble constant in terms of seconds only (i.e. no other units)

H0 = 7.2 x 104 m/s / Mpc

= 7.2 x 104 m/s / 3.0857x 1022m = 2.33 x 10-18 /s

Hubbles lawV = H0 * d

Page 14: Name: Setiawan Office: S13-02-09, Phys. Departm. Phone: 6516-2988 Email: physetia@nus.edu.sgphysetia@nus.edu.sg Consultation: Wed. 10.00-12.00 Tutorial

6. Galileo was one of the first to systematically try to measure the speed of light. His attempt involved two observers positioned in two towers that were about 10km apart. The idea was that the first observer opens a shutter in a lantern and then as soon as the second observer sees the light from the first lantern, opens his shutter. Galileo would then measure the time it takes from opening the first shutter to seeing the light from the second lantern arrive at the first lantern. Unfortunately for Galileo, this experiment turned out to be inconclusive. Why is that so? Would it have been sensible to choose towers that are further apart?

Question 6

Page 15: Name: Setiawan Office: S13-02-09, Phys. Departm. Phone: 6516-2988 Email: physetia@nus.edu.sgphysetia@nus.edu.sg Consultation: Wed. 10.00-12.00 Tutorial

Answer for question 6

It is not possible because the velocity of light is tremendously large. As a matter of fact, light only takes 0.000005 seconds to travel one mile In order to measure the speed of light. It is extremely important to measure the time accurately which needs a sufficiently long distance and extremely negligible reaction time of the observer

How to measure speed of light?http://www.colorado.edu/physics/2000/waves_particles/l

ightspeed_evidence.html