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Page 1: Physics 81

11/20/2015

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Post

Laboratory

Discussion PHYSICS 81

EXERCISE 7: CONSERVATION OF ENERGY

AND LINEAR MOMENTUM

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RESULTS

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Law of Conservation of Mechanical Energy

Law of Conservation of Linear Momentum

EXERCISE 8: TORQUE

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𝜏 ∝ π‘™π‘’π‘›π‘”π‘‘β„Ž π‘œπ‘“ π‘šπ‘œπ‘šπ‘’π‘›π‘‘ π‘Žπ‘Ÿπ‘š

𝜏 ∝ π‘šπ‘Žπ‘ π‘  π‘œπ‘“ π‘‘β„Žπ‘’ π‘™π‘œπ‘Žπ‘‘ π‘“π‘œπ‘Ÿπ‘π‘’

Torque produced by the bar is not

included in the summation of torque

produced in Part I and II since

_______________.

The normal force from the iron stand is

not included on the forces that produce

torque because ___________________.

RESULTS

Part I

Displacement Method

𝐹𝐡 = π‘Šπ‘“π‘‘ = π‘šπ‘“π‘‘π‘”

using Archimedes’ principle

FBD Method

𝐹𝐡 = π‘Šπ‘™π‘œπ‘ π‘  = π‘Šπ‘Žπ‘–π‘Ÿ βˆ’π‘Šπ‘“π‘™π‘’π‘–π‘‘

Part II: U-tube manometer

π‘ƒπ‘€π‘Žπ‘‘π‘’π‘Ÿ = π‘ƒπ‘œπ‘–π‘™(π‘Žπ‘‘ π‘‘β„Žπ‘’ π‘–π‘›π‘‘π‘’π‘Ÿπ‘“π‘Žπ‘π‘’)

EXERCISE 9: BUOYANT FORCE AND

SPECIFIC GRAVITY

Part I:

𝐹𝐡(π‘€π‘Žπ‘‘π‘’π‘Ÿ) > 𝐹𝐡(π‘œπ‘–π‘™)

𝐹𝐡 ∝ 𝜌 𝑠𝑖𝑛𝑐𝑒 𝜌(π‘€π‘Žπ‘‘π‘’π‘Ÿ) > 𝜌(π‘œπ‘–π‘™)

FBD method

𝐹 = 𝑇 + 𝐹𝐡 βˆ’ π‘Š = 0

𝐹𝐡 = π‘Š βˆ’ 𝑇

𝐹𝐡 = π‘Šπ‘Žπ‘–π‘Ÿ βˆ’π‘Šπ‘“π‘™π‘’π‘–π‘‘

RESULTS

Part II:

π‘ƒπ‘€π‘Žπ‘‘π‘’π‘Ÿ = π‘ƒπ‘œπ‘–π‘™ π‘Žπ‘‘ π‘‘β„Žπ‘’ π‘–π‘›π‘‘π‘’π‘Ÿπ‘“π‘Žπ‘π‘’

πœŒπ‘€π‘” β„Žπ‘€ βˆ’ β„Žπ‘– = πœŒπ‘œπ‘–π‘™π‘” β„Žπ‘œπ‘–π‘™ βˆ’ β„Žπ‘–

πœŒπ‘œβ€² = πœŒπ‘œπ‘–π‘™πœŒπ‘€π‘Žπ‘‘π‘’π‘Ÿ

=(β„Žπ‘€βˆ’β„Žπ‘–)(β„Žπ‘œπ‘–π‘™βˆ’β„Žπ‘–)

𝜌 1/∝ β„Ž

RESULTS

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π·π‘’π‘Ÿπ‘–π‘£π‘’: 𝑇 = 2πœ‹ 𝑙𝑔

𝐹 = 𝐹𝑠 = βˆ’π‘˜π‘₯ = π‘šπ‘”π‘ π‘–π‘›πœƒ

since 𝑠 = π‘™πœƒ and sinΞΈ β‰ˆ πœƒ βˆ’π‘˜π‘₯ = βˆ’π‘˜π‘  = π‘šπ‘”πœƒ

π‘˜ = βˆ’π‘šπ‘”πœƒπ‘ =π‘šπ‘”πœƒπ‘™πœƒ= π‘šπ‘”π‘™

𝑇 = 2πœ‹ π‘šπ‘˜= 2πœ‹ π‘š

π‘šπ‘”/𝑙= 2πœ‹ 𝑙

𝑔

EXERCISE 10: SIMPLE HARMONIC

MOTION RESULTS

y = 3.9359x + 0.1006

RΒ² = 0.997

0

1

2

3

4

5

6

0 0.5 1 1.5

T2

length (m)

%25.2%

/03.10

/9359.3

4

44

2

2

2

22

error

smg

msg

mg

gm

Part I: Finding the

specific heat

capacity of an

unknown metal

Part II: Finding the

latent heat of

fusion of ice

EXERCISE 11: CALORIMETRY

Part I:

βˆ’π‘„π‘™π‘œπ‘ π‘  = π‘„π‘”π‘Žπ‘–π‘›

βˆ’π‘„π‘šπ‘’π‘‘π‘Žπ‘™ = 𝑄𝑐 + 𝑄𝑀 + 𝑄𝑠

Part II:

π‘„π‘™π‘œπ‘ π‘  = π‘„π‘”π‘Žπ‘–π‘›

βˆ’(𝑄𝑐+𝑄𝑀 + 𝑄𝑠) = 𝑄𝑖 (𝑇𝑖 π‘‘π‘œ 0) + 𝑄𝑝𝑐 + 𝑄𝑖 (0 π‘‘π‘œ 𝑇𝑓)

RESULTS


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