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KINEMATICS IN TWO DIMENSIONS
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Page 1: Lecture 05 Kinematics in Two Dimensions

KINEMATICS IN TWO DIMENSIONS

Page 2: Lecture 05 Kinematics in Two Dimensions

�⃑�

π’™πœƒ

Recall: Polar to Rectangular𝒙=𝐬𝐜𝐨𝐬 𝜽

π’š π’š=𝐬𝐬𝐒𝐧𝜽

𝒔=βˆšπ’™β‘πŸ+π’šβ‘

𝟐

To find if and are given:

�⃑� 𝒙 π’š

𝜽=π­πšπ§βˆ’πŸ|𝐨𝐩𝐩𝐨𝐬𝐒𝐭𝐞𝐚𝐝𝐣𝐚𝐜𝐞𝐧𝐭|

Page 3: Lecture 05 Kinematics in Two Dimensions

Projectile MotionA projectile is a particle moving near the Earth’s surface under the influence of its weight only (directed downward). Projectile motion is a combination of horizontal and vertical motions.

a = gW

WW

Page 4: Lecture 05 Kinematics in Two Dimensions

Consider Projectile at an Angle:A red ball is projected at an angle q. At the same time, a yellow ball is thrown vertically upward and a green ball rolls horizontally (no friction).

A red ball is projected at an angle q. At the same time, a yellow ball is thrown vertically upward and a green ball rolls horizontally (no friction).

Note vertical and horizontal motions of balls

q

voy

vox

vo

Page 5: Lecture 05 Kinematics in Two Dimensions

Calculations for Projectile Motion (No Air Resistance)

Horizontal velocity:

Vertical velocity:

β€’ Horizontal velocity is constant (no net force along horizontal)

𝒗 𝒙=𝒗𝒐𝒙𝒗𝒐𝒙=𝒗𝒐 cos𝜽

β€’ Vertical velocity varies (net force is the gravitational force/weight)

Kinematics equations for constant acceleration

π’—π’π’š=𝒗𝒐sin 𝜽

𝒗 𝒙=βˆ† 𝒙𝒕

Page 6: Lecture 05 Kinematics in Two Dimensions

Vertical and Horizontal Motion

Simultaneously dropping a yellow ball and projecting a red ball horizontally.

Why do they strike the ground at the same

time?

Once motion has begun, the downward weight is the only force on each ball.

Once motion has begun, the downward weight is the only force on each ball.

W W

Page 7: Lecture 05 Kinematics in Two Dimensions

Consider Horizontal and Vertical Motion Separately:

Compare Displacements and Velocities

0 s0 s

1 svox 2 s 3 s

1 svy2 s

vx

vy3 s

vx

vy

Horizontal velocity doesn’t change.

Vertical velocity just like free fall.

vx

Page 8: Lecture 05 Kinematics in Two Dimensions

Calculation Range:Range is sometimes referred to the horizontal displacement for a complete projectile.

πœƒπœƒ

π‘£π‘œ

𝑣=𝑣π‘₯

𝑣=π‘£π‘œ

range,

βˆ† 𝒙=𝒗𝒐

𝟐sinπŸπœ½π’ˆ

- angle that can give maximum rangeπœ½β€²=πŸ—πŸŽπ¨βˆ’ 𝜽

Page 9: Lecture 05 Kinematics in Two Dimensions

Example 1: A ball rolls off the top of a table 1.2 m high and lands on the floor at a horizontal distance of 2.0 m. What was the velocity as it left the table?

1.2 m2.0 m

Page 10: Lecture 05 Kinematics in Two Dimensions

Given: – horizontal displacement

– vertical displacement

Find: - initial velocity

Solutions: π‘£π‘œ=𝑣π‘₯ 𝑣 π‘₯=βˆ† π‘₯𝑑

βˆ† 𝑦=π‘£π‘œπ‘¦π‘‘+12𝑔𝑑 2 𝑑=√ 2βˆ† 𝑦𝑔

π‘£π‘œ=βˆ† π‘₯

√ 2βˆ† 𝑦𝑔 π‘£π‘œ=βˆ† π‘₯√ 𝑔2βˆ† 𝑦

π‘£π‘œ=(2.0m ) √ 9.8m /s2

2 (1.2m )𝒗𝒐=πŸ’ .𝟎𝐦 /𝐬

Page 11: Lecture 05 Kinematics in Two Dimensions

Example 2:

The best leaper in the animal kingdom is the puma, which can jump to a height of 12.00 ft when leaving the ground at an angle of 45.0o. With what speed must the animal leave the ground to reach that height? How far has the puma leaped from its starting point?

Page 12: Lecture 05 Kinematics in Two Dimensions

Example 3:

Karl, who is a 2.00-m basketball player, is standing on the floor 10.0 m from the basket. If he shoots the ball at a 40.0o angle with the horizontal, at what initial speed must he throw the basketball so that it goes through the hoop without striking the backboard? The height of the basket from the ground is 3.05 m.

Page 13: Lecture 05 Kinematics in Two Dimensions

Relative velocity

Relative velocity is all about relating measurements of two different observers,

one moving with respect to the other.

Measurements of velocity depend on the reference frame (coordinate systems) of the observers.

Page 14: Lecture 05 Kinematics in Two Dimensions

Problem Solving Strategy

1. Label each object involved with a letter that reminds you of what it is (for example, E for earth).

2. Look through the problem for phrase such as β€œThe velocity of A relative to B,” and write the velocities as When a velocity is mentioned but it isn’t explicitly stated as relative to something, it’s always relative to earth.

3. Take the three velocities you’ve found and assemble them into an equation: .

4. There will be two unknown components. Solve for them with the x- and y-components of the equation developed in step 3.

Page 15: Lecture 05 Kinematics in Two Dimensions

Example 1:

The boat is heading due north as it crosses a wide river with a velocity of 10.0 km/h relative to the water. The river has a uniform velocity of 5.00 km/h due east. Determine the velocity of the boat with respect to an observer on the riverbank.

Page 16: Lecture 05 Kinematics in Two Dimensions

Example 2:

A train is traveling with a speed of 15.0 m/s relative to earth. A passenger standing at the rear of the train pitches a baseball with a speed of 15.0 m/s relative to the train off the back end, in the direction opposite the motion of the train. What is the velocity of the baseball relative to earth?