# OLDHW15 - oldhomewk 15 PAPAGEORGE MATT Due 4:00 am Question...

• Notes
• 8

This preview shows pages 1–3. Sign up to view the full content.

oldhomewk 15 – PAPAGEORGE, MATT – Due: Feb 21 2008, 4:00 am 1 Question 1, chap 8, sect 5. part 1 of 1 10 points A child pushes horizontally on a box of mass m which moves with constant speed v across a horizontal floor. The coefficient of friction between the box and the floor is μ . At what rate does the child do work on the box? 1. P = μ m g v 2. P = μ m g v correct 3. P = v μ m g 4. P = m g v 5. P = μ m v 2 Explanation: Since the box moves horizontally with con- stant speed, the force exerted by the child is equal to the frictional force on the box μ m g . Thus, the power generated by the child is P = F v = μ m g v . Question 2, chap 6, sect 1. part 1 of 1 10 points A box of mass m with an initial velocity of v 0 slides down a plane, inclined at θ with respect to the horizontal. The coefficient of kinetic friction is μ . The box stops after sliding a distance x . m μ k v 0 θ How far does the box slide? 1. x = v 2 0 2 g ( μ cos θ + sin θ ) 2. x = v 2 0 g ( μ sin θ - 2 cos θ ) 3. x = v 2 0 2 g sin θ 4. x = v 2 0 g ( μ sin θ + cos θ ) 5. x = v 2 0 2 g ( μ cos θ - sin θ ) correct 6. x = v 2 0 g (sin θ - μ cos θ ) 7. x = v 2 0 2 g μ cos θ 8. x = v 2 0 2 g ( μ sin θ - cos θ ) 9. x = v 2 0 2 g (sin θ - μ cos θ ) 10. x = v 2 0 2 g ( μ sin θ + cos θ ) Explanation: Basic Concepts: Motion under constant force W = vector F · vectors P = Δ W Δ t P = d W dt = vector F · vectorv . Solution: The net force on the block parallel to the incline is F net = F m g sin θ - F f , where F f is the friction force. Thus, Newton’s equation for the block reads m a = m g sin θ - F f = m g sin θ - μ N = m g (sin θ - μ cos θ ) a = g (sin θ - μ cos θ ) , where N = m g cos θ . To find the distance the block slides down the incline, use v 2 = v 2 0 + 2 a ( x - x 0 ) ,

This preview has intentionally blurred sections. Sign up to view the full version.

oldhomewk 15 – PAPAGEORGE, MATT – Due: Feb 21 2008, 4:00 am 2 valid for a body moving with a constant accel- eration. Since x 0 = 0 and v f = 0 (the block stops), we get x = - v 2 0 2 a = - v 2 0 2 g (sin θ - μ cos θ ) = v 2 0 2 g ( μ cos θ - sin θ ) . Question 3, chap 8, sect 5. part 1 of 1 10 points Water flows over a section of Niagara Falls at a rate of 1 . 9 × 10 6 kg / s and falls 67 m. The acceleration of gravity is 9 . 8 m / s 2 . What is the power wasted by the waterfall? Correct answer: 1 . 24754 × 10 9 W (tolerance ± 1 %). Explanation: P = W t = m g h t = ρ g h = (1 . 9 × 10 6 kg / s) (9 . 8 m / s 2 ) (67 m) = 1 . 24754 × 10 9 W Question 4, chap 8, sect 5. part 1 of 4 10 points A particle of mass m moves along the x axis. Its position varies with time according to x = (5 m / s 3 ) t 3 - (7 m / s 2 ) t 2 . What is the velocity of the particle at any time t ? 1. v = (27 m / s 2 ) t 2 - (14 m / s) t 2. v = (15 m / s 2 ) t 2 - (14 m / s) t correct 3. v = (24 m / s 2 ) t 2 - (16 m / s) t 4. v = (27 m / s 2 ) t 2 - (4 m / s) t 5. v = (6 m / s 2 ) t 2 - (12 m / s) t 6. v = (24 m / s 2 ) t 2 - (8 m / s) t 7. v = (12 m / s 2 ) t 2 - (16 m / s) t 8. v = (18 m / s 2 ) t 2 - (12 m / s) t 9. v = (6 m / s 2 ) t 2 - (6 m / s) t 10. v = (24 m / s 2 ) t 2 - (18 m / s) t Explanation: The velocity of the particle is v = d x dt = d dt bracketleftbig (5 m / s 3 ) t 3 - (7 m / s 2 ) t 2 bracketrightbig = (15 m / s 2 ) t 2 - (14 m / s) t .
This is the end of the preview. Sign up to access the rest of the document.
• Spring '09
• KLEINMAN

{[ snackBarMessage ]}

### What students are saying

• As a current student on this bumpy collegiate pathway, I stumbled upon Course Hero, where I can find study resources for nearly all my courses, get online help from tutors 24/7, and even share my old projects, papers, and lecture notes with other students.

Kiran Temple University Fox School of Business ‘17, Course Hero Intern

• I cannot even describe how much Course Hero helped me this summer. It’s truly become something I can always rely on and help me. In the end, I was not only able to survive summer classes, but I was able to thrive thanks to Course Hero.

Dana University of Pennsylvania ‘17, Course Hero Intern

• The ability to access any university’s resources through Course Hero proved invaluable in my case. I was behind on Tulane coursework and actually used UCLA’s materials to help me move forward and get everything together on time.

Jill Tulane University ‘16, Course Hero Intern