An object is moving with initial velocity of 20m/s. It must slow down to a stop in .33 seconds and travel 4m. Write a solution that applies a force to the object to satisfy the expected result.?

The first thing I do not understand is why I can assume linear acceleration.
I have a basic understanding of calculus so explaining using integration is fine.

Answer 1

#F = m * 36.7 m/s^2#

You may “assume” linear acceleration because you are asked for “a solution”, not all solutions.

F = m * a d = v * t To stop in the specified distance and time. 4m = v(m/s) * 0.33s ; v = 12.12 m/s

To decelerate: #a = (v/t) ; a = ((12.12(m/s))/0.33s) = 36.7 m/s^2#

F = m * a

#F = m * 36.7 m/s^2#
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Answer 2

Applied force #F(t)=(-22.0m-233.7mt)# N

Initial velocity #u=20ms^-1#. Final velocity #v=0#, distance traveled #=4m#.
The applicable kinematic equation for a constant acceleration is #v^2-u^2=2as# #=>0^2-20^2=2axx4# #=>a=-400/8=-50ms^-2#
Let us find out for what time this retarding force is applied. Using the other kinematic equation #v=u+at# we get #0=20+(-50)t# #t=20/50=0.4s# We see that the object takes more time than given in the question to come to stop. This implies that it is not a case of constant deceleration.
Let us assume that the object of mass #m# is acted upon by a time dependent force #F(t)#. From Newton's Second law we get #F(t)=mxxa(t)# .....(1) We know that acceleration can be written as #(dv)/dt=a(t)# #=>dv=a(t)cdot dt# Using (1) and Integrating both sides we get #v(t)=int(F(t))/mcdot dt#......(2)
Suppose the force is given by the expression #F(t)=L+Kt# Where #L and K# are constants. (2) becomes #v(t)=int (L+Kt)/mcdot dt# #=>v(t)= L/m t+K/mt^2/2+C# where #C# is constant of integration. As #v(t)=u# initial velocity at #t=0# Expression becomes
#v(t)=L/mt+K/(2m)t^2+u# .....(3) We also know that velocity can be written in terms of displacement #s# as #(ds)/dt=v(t)# #=>ds=v(t)cdot dt# Integrating both sides we get #s=intv(t)cdot dt# Using (3) we get #s=int(L/mt+K/(2m)t^2+u)cdot dt# #=>s=L/mt^2/2+K/(2m)t^3/3+ut+C_1# #C_1# is constant of integration. Assuming that displacement is zero at #t=0#, we get #C_1=0# and the expression for displacement becomes #=>s=L/(2m)t^2+K/(6m)t^3+ut# ......(4)
Inserting given values in (3) and (4) we obtain #0=L/mxx0.33+K/(2m)(0.33)^2+20# .....(5) #4=L/(2m)(0.33)^2+K/(6m)(0.33)^3+20xx0.33# ......(6) To solve for #L and K#, multiply (5) with #0.33/2#, it becomes #0=L/(2m)xx(0.33)^2+K/(4m)(0.33)^3+20xx0.33/2# .....(7)
Subtracting (7) from (6) #4=K/(6m)(0.33)^3+20xx0.33-(K/(4m)(0.33)^3+20xx0.33/2)# #=>4=-K/(12m)(0.33)^3-20xx0.33/2# #K=-233.7m# Inserting this value of #K# in (5) we get #0=L/mxx0.33-(233.7m)/(2m)(0.33)^2+20# #L=-22.0m#
As such applied force #F(t)=(-22.0m-233.7mt)# N
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Answer 3

To bring the object to a stop in 0.33 seconds while traveling 4m, a force needs to be applied to decelerate it. Using the equation (v_f = v_i + at), where (v_f) is final velocity (0 m/s), (v_i) is initial velocity (20 m/s), (a) is acceleration, and (t) is time, we can calculate acceleration. Subsequently, using (s = ut + \frac{1}{2}at^2), where (s) is displacement (4 m), (u) is initial velocity, (a) is acceleration, and (t) is time, we can verify the result. The force applied would depend on the mass of the object, and (F = ma) could be used to find it.

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