Hammer striking an anvil with a velocity of 50ft/sec

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Homework Help Overview

The problem involves a hammer striking an anvil with a specified velocity, examining two scenarios: one where the hammer remains in contact with the anvil and another where it does not. The context includes dynamics and energy considerations, particularly in relation to collisions and spring mechanics.

Discussion Character

  • Mixed

Approaches and Questions Raised

  • Participants explore the dynamics of the hammer-anvil interaction, considering both inelastic collision scenarios and the effects of spring support. Some participants question the initial conditions and the application of conservation laws, while others suggest using momentum conservation as a potential approach.

Discussion Status

The discussion is active, with participants offering various perspectives on how to approach the problem. Some have proposed using momentum conservation, while others are examining the implications of energy conservation in the context of the collision.

Contextual Notes

There are discussions regarding the assumptions made about the collision type (elastic vs. inelastic) and the implications of these assumptions on energy conservation. Additionally, participants are encouraged to work symbolically rather than numerically at this stage.

Dustinsfl
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Homework Statement


A hammer strikes an anvil with a velocity of 50ft/sec. The hammer weights 12 lb and the anvil weighs 100 lb. The anvil is supported on four springs with k = 100 lb/in. Find the motion if
(a) the hammer stays in contact with the anvil
(b) the hammer doesn't remain in contatct

Homework Equations


##1 lb = 4.45 N##
##1 m = 3.28ft##
##k_{eq} = 4k = 400\cdot 4.45\cdot 12\cdot 3.28 = 70060.8## N/m
##W = mg## so ##m_h = 12*4.45/9.8 = 5.45## kg and ##m_a = 100*4.45/9.8 = 45.41## kg
##\dot{x}(0) = 50/3.28 = 15.24## m/s

The Attempt at a Solution


(a)
$$
M\ddot{x} + k_{eq}x = 0
$$
where ##M = m_h + m_a = 50.86## kg.
$$
\ddot{x} + \omega_n^2x = 0
$$
where ##\omega_n^2 = \frac{70060.8}{50.86} = 1377.52##
Let ##x(t) = A\cos(\omega_nt) + B\sin(\omega_nt)##. Then ##\ddot{x} = -A\omega_n^2\cos(\omega_nt) - B\omega_n^2\sin(\omega_nt)##.
$$
\cos(\omega_nt)[-A\omega_n^2 + A\omega_n^2] + \sin(\omega_nt)[-B\omega_n^2 + B\omega_n^2] = 0
$$
The coefficient zero out so this can't be correct. The RHS has to be zero since there is no driving force.
 
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Leave out all the numbers and conversions for now, and just do everything symbolically. Hammer mass m moving vertically down at speed u strikes anvil of mass M supported on four springs of coefficient k. What is the speed of the anvil immediately after impact?
 
haruspex said:
Leave out all the numbers and conversions for now, and just do everything symbolically. Hammer mass m moving vertically down at speed u strikes anvil of mass M supported on four springs of coefficient k. What is the speed of the anvil immediately after impact?

I have been thinking about this. Should the initial velocity for the inelastic collision be found as
$$
m_h(50)^2 = v^2(m_h + m_a)
$$
Then v would be ##\dot{x}(0) = v##?

For part b, since the hammer comes off immediately, that would be view as a delta spike and ##\dot{x}(0) = 50## the velocity of the hammer, correct?
 
Dustinsfl said:
I have been thinking about this. Should the initial velocity for the inelastic collision be found as
$$
m_h(50)^2 = v^2(m_h + m_a)
$$
Then v would be ##\dot{x}(0) = v##?
Since it is an inelastic collision, work is not conserved. What is conserved?
 
Try instead using momentum conservation for both cases, then relate decreasing kinetic energy to increasing potential energy after contact.
 

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