Kinetic Energy WorkKinetic Energy Theorem Energy Losses due

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-Kinetic Energy -Work-Kinetic Energy Theorem -Energy Losses due to Friction -Power AP Physics C

-Kinetic Energy -Work-Kinetic Energy Theorem -Energy Losses due to Friction -Power AP Physics C Mrs. Coyle

Energy and Work • Energy is the ability to do work. • Work is

Energy and Work • Energy is the ability to do work. • Work is the energy transferred to or from a system by a force that acts on it.

Video Link: Kinetic Sculpture • http: //www. youtube. com/watch? v= Wc. R 7 U

Video Link: Kinetic Sculpture • http: //www. youtube. com/watch? v= Wc. R 7 U 2 tu. No. Y&feature=related

Energy • Symbol: E • Scalar • Units: – J, Joule – cal, calorie

Energy • Symbol: E • Scalar • Units: – J, Joule – cal, calorie – kcal, kilocalorie (Cal) – erg – e. V – pound -foot

Mechanical Energy • Potential Energy • Kinetic Energy

Mechanical Energy • Potential Energy • Kinetic Energy

Kinetic Energy, K= 1 mv 2 2 Energy of Motion Coyle, Greece, 2005

Kinetic Energy, K= 1 mv 2 2 Energy of Motion Coyle, Greece, 2005

Question • Can Kinetic Energy be Negative?

Question • Can Kinetic Energy be Negative?

Derivation of K

Derivation of K

Work-Energy Theorem W= KE W=KEf-KEi “In the case in which work is done on

Work-Energy Theorem W= KE W=KEf-KEi “In the case in which work is done on a system and the only change in the system is in its speed, the work done by the net force equals the change in kinetic energy of the system. ”

 • The Work-Kinetic Energy Theorem can be applied to nonisolated systems • A

• The Work-Kinetic Energy Theorem can be applied to nonisolated systems • A nonisolated system is one that is influenced by its environment (external forces act on the system)

Potential Energy, U: stored energy • Examples: – elastic potential energy – stored in

Potential Energy, U: stored energy • Examples: – elastic potential energy – stored in a spring – gravitational potential energy – electrical potential energy • Compared to a Reference Point (base level)

Conservation of Energy • Energy can neither be created nor destroyed. It can only

Conservation of Energy • Energy can neither be created nor destroyed. It can only change from form to form. • In a closed system energy is conserved • Conservation of Mechanical Energy U 1 + K 1 = U 2 + K 2

Energy can be transferred to and from the System by: Work Mechanical Waves Heat

Energy can be transferred to and from the System by: Work Mechanical Waves Heat transfer Matter Transfer (across the boundary of the system carrying energy with it) • Electrical Current Transmission • Electromagnetic Radiation • •

Change in Energy of the system equals total energy transferred • DEsystem = ST

Change in Energy of the system equals total energy transferred • DEsystem = ST – T is the energy transferred across the system boundary – Twork = W Theat = Q • The Work-Kinetic Energy theorem is a special case of Conservation of Energy

What happens when kinetic friction is present? When friction is present, the work done

What happens when kinetic friction is present? When friction is present, the work done by the frictional force W=f·r is transferred to heat energy.

Internal Energy • The energy associated with an object’s temperature is called its internal

Internal Energy • The energy associated with an object’s temperature is called its internal energy, Eint

Power • Energy transfer per unit time • Average power :

Power • Energy transfer per unit time • Average power :

Instantaneous Power

Instantaneous Power

Units of Power • SI unit of power: Watt 1 watt = 1 J/s

Units of Power • SI unit of power: Watt 1 watt = 1 J/s = 1 kg. m 2 / s 2 • US Customary unit: horsepower – 1 hp = 746 W

kilo Watt · hour, k. Wh • k. Wh is a units of work

kilo Watt · hour, k. Wh • k. Wh is a units of work or energy • 1 k. Wh =(1000 W)(3600 s)= =3. 6 x 106 J

Example 1 (#26) A 3 kg object has a velocity (6 i-2 j)m/s. a)

Example 1 (#26) A 3 kg object has a velocity (6 i-2 j)m/s. a) What is the kinetic energy at this time? b) Find the total work done on the object if its velocity changes to (8 i+4 j) m/s. (Note: v 2 = v·v) Ans: a)60 J, b)60 J

Pile Driver

Pile Driver

Example 2 (#27) • A 2, 100 kg pile driver is used to drive

Example 2 (#27) • A 2, 100 kg pile driver is used to drive a steel I-beam into the ground. The pile driver falls 5 m before coming into contact with the top of the beam and it drives the beam 12 cm farther into the ground before coming to rest. Using energy considerations, calculate the average force the beam exerts on the pile driver while the pile driver is brought to rest. Ans: 8. 78 x 105 upwards

Figure for Example 3

Figure for Example 3

Example 3 (#32) A 2 kg block is attached to a spring of a

Example 3 (#32) A 2 kg block is attached to a spring of a force constant 500 N/m on a horizontal table. The block is pulled 5. 00 cm to the right of equilibrium and released from rest. Find the speed of the block as it passes through equilibrium if a)the horizontal surface is frictionless and b) the coefficient of friction between block and surface is 0. 350. Ans: a)0. 791 m/s, b) 0. 531 m/s

Example 4 (#40) A 650 kg elevator starts from rest. It moves upward for

Example 4 (#40) A 650 kg elevator starts from rest. It moves upward for 3 s with a constant acceleration until it reaches its cruising speed of 1. 75 m/s. a)What is the average power of the elevator motor during this period? b)How does this power compare with the motor power when the elevator moves at its cruising speed? Ans: a)5. 91 x 103 W= 7. 92 hp b) 1. 11 x 104 W= 14. 9 hp