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Physics 1

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Task 1: Vector components and free body
diagrams
QUESTION 1
a. π‘₯ π‘π‘œπ‘šπ‘π‘œπ‘›π‘’π‘›π‘‘
|→
𝐹𝑔π‘₯ | = 𝐹𝑔 sin 2 5
|→
𝐹𝑔π‘₯ | = (40) sin 2 5
|→
𝐹𝑔π‘₯ | = 16.9𝑁
|→
𝐹𝑔π‘₯ | = 17𝑁
Y component
|→
𝐹𝑔𝑦 | = 𝐹𝑔 cos 2 5
|→
𝐹𝑔𝑦 | = (40) cos 2 5
|→
𝐹𝑔𝑦 | = 36.252𝑁
|→
𝐹𝑔𝑦 | = 36𝑁
b. X component
→
𝑣π‘₯
= (25π‘š⁄𝑠 ) cos 7 5
→
𝑣π‘₯
= 6.47π‘š⁄𝑠
→
𝑣π‘₯
= 6.5π‘š⁄𝑠
Y component
→
𝑣𝑦
= (25π‘š⁄𝑠 ) sin 7 5
→
𝑣𝑦
= 24.148π‘š ⁄𝑠
→
𝑣𝑦
= 24π‘š⁄𝑠
c. X component
→
𝑣π‘₯
= (17π‘š⁄𝑠 ) cos 6 5
→
𝑣π‘₯
→
𝑣π‘₯
= 7.185π‘š ⁄𝑠
= 7.2π‘š⁄𝑠
Y component
→
𝑣𝑦
= (17π‘š⁄𝑠 ) sin 6 5
→
𝑣𝑦
= 15.41π‘š ⁄𝑠
→
𝑣𝑦
= 15π‘š⁄𝑠
QUESTION 2
a.
b.
Task 2: Relative velocity and projectile
motion problem solving
QUESTION 1
a. Let helicopter represent H
Let the ground represent G
Let airspeed represent A
Given:
|→
𝑣𝐻𝐴 | = 42.5π‘š ⁄𝑠[π‘Š]
|→
𝑣𝐴𝐺 | = 25π‘š ⁄𝑠[𝐸 30°π‘†]
Solving for components of
|→
𝑣𝐻𝐴 |
|→
𝑣𝐻𝐴π‘₯ | =?
|→
𝑣𝐻𝐴𝑦 | =?
Vector falls on east – west horizontal line with no vertical components. Vector only has horizontal
→
components. Therefore, horizontal component of| →
𝑣𝐻𝐴 |, | 𝑣𝐻𝐴π‘₯ | is 42.5 m/s [W] and the vertical
→
component of | →
𝑣𝐻𝐴 | | 𝑣𝐻𝐴𝑦 | is 0 m/s [S]
Solving for components of | →
𝑣𝐴𝐺 |
|→
𝑣𝐴𝐺 | = 25.0π‘š ⁄𝑠 [𝐸 30° 𝑆]
|→
𝑣𝐴𝐺π‘₯ | =?
|→
𝑣𝐴𝐺𝑦 | =?
Find the horizontal component using cosine formula
|→
𝑣𝐴𝐺π‘₯ | = π‘£π‘π‘œπ‘ πœƒ
|→
𝑣𝐴𝐺π‘₯ | = (25π‘š ⁄𝑠 ) cos 3 0°
|→
𝑣𝐴𝐺π‘₯ | = 21.65π‘š ⁄𝑠
|→
𝑣𝐴𝐺π‘₯ | = 22π‘š ⁄𝑠 [𝐸]
Find the vertical component using sine formula
|→
𝑣𝐴𝐺𝑦 | = π‘£π‘ π‘–π‘›πœƒ
|→
𝑣𝐴𝐺𝑦 | = (25π‘š ⁄𝑠 ) sin 3 0°
|→
𝑣𝐴𝐺𝑦 | = 12.5π‘š ⁄𝑠
|→
𝑣𝐴𝐺𝑦 | = 13π‘š ⁄𝑠 [𝑆]
→
Therefore, the horizontal component of | →
𝑣𝐴𝐺 |, | 𝑣𝐴𝐺π‘₯ | is 22 m/s [E] and the vertical component of
→
|→
𝑣𝐴𝐺 | | 𝑣𝐴𝐺𝑦 | is 13 m/s [S]
b. Let west and south be positive directions
Given:
|→
𝑣𝐻𝐴π‘₯ | = 42.5 π‘š ⁄𝑠 [π‘Š]
|→
𝑣𝐴𝐺π‘₯ | = 22 π‘š ⁄𝑠 [𝐸] rounded to 2 significant figures
|→
𝑣𝐴𝐺𝑦 | = 13 π‘š ⁄𝑠 [𝑆] rounded to 2 significant figures
→
Required: | →
𝑣𝐻𝐺π‘₯ | =? | 𝑣𝐻𝐺𝑦 | =?
Solution:
To determine | →
𝑣𝐻𝐺π‘₯ |, and all given horizontal components.
→
→
|→
𝑣𝐻𝐺π‘₯ | = | 𝑣𝐻𝐴π‘₯ | + | 𝑣𝐴𝐺π‘₯ |
|→
𝑣𝐻𝐺π‘₯ | = 42.5π‘š ⁄𝑠 + (−22.65π‘š ⁄𝑠)
|→
𝑣𝐻𝐺π‘₯ | = 19.85π‘š ⁄𝑠
|→
𝑣𝐻𝐺π‘₯ | = 20π‘š ⁄𝑠 [π‘Š]
To determine | →
𝑣𝐻𝐺𝑦 |, add all given vertical components.
→
→
|→
𝑣𝐻𝐺𝑦 | = | 𝑣𝐻𝐴𝑦 | + | 𝑣𝐴𝐺𝑦 |
|→
𝑣𝐻𝐺𝑦 | = 0π‘š ⁄𝑠 + 12.5π‘š ⁄𝑠
|→
𝑣𝐻𝐺𝑦 | = 12.5π‘š ⁄𝑠
|→
𝑣𝐻𝐺𝑦 | = 13π‘š ⁄𝑠 [𝑆]
c. Solution: using Pythagorean theorem to find magnitude of resultant velocity
2
2
→
→
|→
𝑣𝐻𝐺 | = √ | 𝑣𝐻𝐺π‘₯ | + | 𝑣𝐻𝐺𝑦 |
2
2
|→
𝑣𝐻𝐺 | = √ (19.85π‘š ⁄𝑠 ) + (12.5π‘š ⁄𝑠)
|→
𝑣𝐻𝐺 | = √ 550.2725π‘š ⁄𝑠
|→
𝑣𝐻𝐺 | = 23.458π‘š ⁄𝑠
|→
𝑣𝐻𝐺 | = 23π‘š ⁄𝑠
Using tangent function to find direction
π‘‘π‘Žπ‘›πœƒ =
πœƒ = tan−1
|→
𝑣𝐻𝐺𝑦 |
|→
𝑣𝐻𝐺π‘₯ |
(12.5π‘š⁄𝑠)
(19.85π‘š⁄𝑠 )
πœƒ = 32°
Therefore, the resultant velocity of the helicopter relative to the ground is 23 m/s [π‘Š32°π‘†]
QUESTION 2
Solution: first, determine horizontal and vertical components of initial velocity to help find final velocity
which we will use to find the time of flight.
Given:
→
π‘Ž
= 9.8 π‘š⁄𝑠 2 [π‘‘π‘œπ‘€π‘›]
β–³ 𝑑𝑦 = 4.3 π‘š[π‘‘π‘œπ‘€π‘›]
→
𝑣𝑖
= 30 π‘š⁄𝑠
πœƒ = 35°
Solving for horizontal components
cos 3 5° =→𝑣𝑖π‘₯ ⁄ →
𝑣𝑖
→
𝑣𝑖π‘₯
→
𝑣𝑖π‘₯
→
𝑣𝑖π‘₯
=→
𝑣𝑖 cos 3 5°
= (30π‘š⁄𝑠 ) sin 3 5°
= 24.575π‘š⁄𝑠 [π‘Ÿπ‘–π‘”β„Žπ‘‘]
Solving for vertical components
sin 3 5° =→
𝑣𝑖𝑦 ⁄
→
𝑣𝑖𝑦
=
→
𝑣𝑖
→
𝑣𝑖
sin 3 5°
→
𝑣𝑖𝑦
= (30π‘š⁄𝑠 ) sin 3 5°
→
𝑣𝑖𝑦
= 17.208π‘š⁄𝑠 [𝑒𝑝]
a. Required: β–³ 𝑑 =?
→ . let up be positive direction
Using motion equation 5 to determine 𝑣𝑓𝑦
→
2
𝑣𝑓𝑦
→
𝑣𝑓𝑦
=
→
2
𝑣𝑖𝑦
+ 2→
π‘Ž β–³ 𝑑𝑦
= √(17.208π‘š⁄𝑠 )2 + 2(−9.8π‘š⁄𝑠)(−4.3)
→
𝑣𝑓𝑦
= √380.395264
→
𝑣𝑓𝑦
= ±19.50π‘š ⁄𝑠
Negative root chosen since the ball is travelling downward at this time. Therefore,
→ = −19.50π‘š ⁄𝑠[𝑒𝑝]
𝑣𝑓𝑦
Solving for time of flight using motion equation 1.
→
𝑣𝑓𝑦
→
=→
𝑣𝑖𝑦 +π‘Ž β–³ 𝑑
(−19.50π‘š⁄𝑠 ) = (17.208π‘š⁄𝑠 ) + (−9.8π‘š⁄𝑠 2 β–³ 𝑑 )
△𝑑=
(−36.708π‘š ⁄𝑠 )
(−9.8π‘š⁄𝑠 2 )
β–³ 𝑑 = 3.746𝑠
β–³ 𝑑 = 3.7𝑠
Therefore, the time of flight of the golf ball is 3.7s
b. Required: β–³ 𝑑π‘₯ =?
Using constant equation for velocity to find range, β–³ 𝑑π‘₯
→
𝑣𝑖π‘₯
=
β–³ 𝑑π‘₯
△𝑑
→
𝑣𝑖π‘₯
β–³ 𝑑π‘₯ =
△𝑑
β–³ 𝑑π‘₯ = (24.575π‘š⁄𝑠 )(3.746𝑠)
β–³ 𝑑π‘₯ = 92.06π‘š
β–³ 𝑑π‘₯ = 92π‘š
Therefore, the range for the golf ball is 92m.
c. Required:
→
𝑣𝑓
=?
Using Pythagorean theorem to solve for final velocity
2
2
→
→
|→
𝑣𝑓 | = √| 𝑣𝑓π‘₯ | + | 𝑣𝑓𝑦 |
2
2
|→
𝑣𝑓 | = √(24.575π‘š ⁄𝑠 ) + (19.50π‘š ⁄𝑠)
|→
𝑣𝑓 | = ±31.371π‘š ⁄𝑠
Choose a positive root since magnitude is always positive
|→
𝑣𝑓 | = 31π‘š ⁄𝑠
Using tangent function to determine direction
π‘‘π‘Žπ‘›πœƒ =
𝑣𝑓𝑦 ⁄ →
𝑣𝑓π‘₯
→
πœƒ = tan−1
(19.50π‘š⁄𝑠 )
(24.575π‘š⁄𝑠 )
πœƒ = 38°
Therefore, the velocity of the golf ball the instant before the ball impacts the ground is
31 π‘š⁄𝑠 [π‘Ÿπ‘–π‘”β„Žπ‘‘ 38° π‘‘π‘œπ‘€π‘›]
Task 3: Newton’s laws of motion and
uniform circular motion problem-solving
QUESTION 1
a.
b.
→
𝐹𝑛𝑒𝑑𝑦
=
→
𝐹𝑛
+ (−→
𝐹𝑔𝑦 )
All force is happening on x-axis, therefore
movement on the y-axis.
→
𝐹𝑛𝑒𝑑𝑦
= 0 because acceleration is 0 since there is no
0 = 𝐹𝑁 − π‘šπ‘” cos 3 0°
𝐹𝑁 = π‘šπ‘” cos 3 0°
𝐹𝑁 = (120π‘˜π‘”)(9.8π‘š⁄𝑠 2 ) cos 3 0°
𝐹𝑁 = 1018.45π‘˜π‘” [𝑒𝑝]
𝐹𝑁 = 1.0 × 103 π‘˜π‘” [𝑒𝑝]
c. Solution
→
πΉπ‘˜ = πœ‡π‘˜ 𝐹𝑁
→ (0.10)(1018.45π‘˜π‘”)
πΉπ‘˜ =
→
πΉπ‘˜ = 101.845𝑁
→
πΉπ‘˜ = 1.0
d. Solution for 𝐹𝑛𝑒𝑑π‘₯
× 102 𝑁
𝐹𝑛𝑒𝑑π‘₯ = 𝐹𝑔π‘₯ + (−πΉπ‘˜)
𝐹𝑛𝑒𝑑π‘₯ = (π‘šπ‘”) sin 3 0° − 101.845𝑁
𝐹𝑛𝑒𝑑π‘₯ = (120π‘˜π‘”)(9.8π‘š⁄𝑠 2 ) sin 3 0° − 101.845𝑁
𝐹𝑛𝑒𝑑π‘₯ = 588𝑁 − 101.845𝑁
𝐹𝑛𝑒𝑑π‘₯ = 486.155𝑁
Solving for acceleration
→
𝐹𝑛𝑒𝑑π‘₯
= π‘šπ‘Ž→π‘₯
486.155𝑁 = (120π‘˜π‘”)π‘Žπ‘₯
π‘Žπ‘₯ =
486.155𝑁
120π‘˜π‘”
π‘Žπ‘₯ = 4.05π‘š⁄𝑠 2 [π‘‘π‘œπ‘€π‘› π‘‘β„Žπ‘’ π‘Ÿπ‘Žπ‘šπ‘]
Therefore, the acceleration of the piano down the ramp along the axis parallel to the ramp is
4.05π‘š ⁄𝑠 2 [π‘‘π‘œπ‘€π‘› π‘‘β„Žπ‘’ π‘Ÿπ‘Žπ‘šπ‘]
QUESTION 2
a. Given: m=100kg, r=0.25m
Required: v=?
Solution: using equation to determine minimum speed required to maintain the path of circular motion
v=√π‘Ÿπ‘”
𝑣 = √(0.25)(9.8π‘š⁄𝑠 2 )
𝑣 = ±1.565π‘š ⁄𝑠
Choose positive root since magnitude is always positive
𝑣 = 1.57π‘š⁄𝑠 (Rounded to 3 significant figures)
b. Given: r = 0.25m, m=0.100kg, v= 1.57m/s g= 9.8m/s^2
Required: 𝐹𝑇 =?
𝐹𝐢 = 𝐹𝑇 − 𝐹𝑔
𝑣2
π‘š ( ) = 𝐹𝑇 − π‘šπ‘”
π‘Ÿ
𝐹𝑇 =
(0.100π‘˜π‘”)(1.57π‘š⁄𝑠 2 )
+ π‘šπ‘”
0.25π‘š
𝐹𝑇 = 0.97969 + 0.98
𝐹𝑇 = 1.959𝑁
𝐹𝑇 = 2.0𝑁
Therefore, thew magnitude of the tension in the string at the bottom of the circle is 2.0N
QUESTION 3
a. Given: 𝐹𝐾 = 5.0𝑁 π‘š1 = 2.1π‘˜π‘” π‘š2 = 3.3π‘˜π‘”
Solving for acceleration using Newton’s Second Law
𝐹𝑛𝑒𝑑 = π‘šπ‘Ž
π‘Ž=
π‘Ž=
𝐹𝑛𝑒𝑑
π‘š
𝐹𝑇 − πΉπ‘˜ + π‘š2 𝑔 − 𝐹𝑇
(π‘š1 + π‘š2 )
π‘Ž=
π‘Ž=
π‘š2 𝑔 − πΉπ‘˜
(π‘š1 + π‘š2 )
32.34𝑁 − 5.0𝑁
5.4π‘˜π‘”
π‘Ž = 5.06π‘š⁄𝑠 2
To solve for 𝐹𝑇
Solve for π‘š1
𝐹𝑛𝑒𝑑1 = 𝐹𝑇 − πΉπ‘˜
π‘š1 π‘Ž = 𝐹𝑇 − πΉπ‘˜
𝐹𝑇 = (2.1π‘˜π‘”)(5.06π‘š ⁄𝑠 2 ) + 5.0𝑁
𝐹𝑇 = 15.626𝑁
𝐹𝑇 = 16𝑁
Therefore 𝐹𝑇 = 16𝑁 . For verification, solve for π‘š2 to see if 𝐹𝑇 will have same outcome has π‘š1
b. Solving for π‘š2
𝐹𝑛𝑒𝑑2 = 𝐹𝑔2 − 𝐹𝑇
π‘š2 π‘Ž = π‘š2 𝑔 − 𝐹𝑇
𝐹𝑇 = π‘š2 𝑔 − π‘š2 π‘Ž
𝐹𝑇 = (3.3π‘˜π‘”)(9.8π‘š⁄𝑠 2 ) − (3.3π‘˜π‘”)(5.06π‘š⁄𝑠 2 )
𝐹𝑇 = 32.34𝑁 − 16.698𝑁
𝐹𝑇 = 15.642𝑁
𝐹𝑇 = 16𝑁
Therefore, the magnitude of the tension in the string is 16N
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