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

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A hammer strikes an anvil at 50 ft/sec, with the hammer weighing 12 lb and the anvil 100 lb, supported by four springs with a stiffness of 100 lb/in. For case (a), if the hammer remains in contact, the motion can be modeled using the equation of motion for a damped harmonic oscillator, leading to the calculation of the natural frequency and subsequent motion equations. In case (b), where the hammer does not stay in contact, momentum conservation principles apply, as the collision is inelastic, meaning kinetic energy is not conserved. The initial velocity for the anvil post-impact can be derived from momentum conservation, while the system's energy transitions from kinetic to potential energy after the impact. The discussion emphasizes the importance of using momentum conservation to analyze both scenarios effectively.
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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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