Solving Equations for Particle Position & Velocity on x-Axis

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The acceleration of a particle moving along the x-axis is given by a(t) = 4cos(2t), leading to the velocity equation v(t) = 2sin(2t) + 1 after integration and applying initial conditions. The position function is derived as x(t) = -cos(2t) + t + 1, also through integration of the velocity function. To determine when the particle is at rest, the velocity equation is set to zero, resulting in t values of -π/12 and 5π/12. However, only t = 5π/12 falls within the specified range of 0 to π. Thus, the particle is at rest at t = 5π/12.
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A particle moves along the x-axis in such a way that its acceleration at time t for t>= 0 is given by a(t)=4cos(2t). At time t=0, the velocity of the particle is v(0)=1 and its position is x(0)=0.
a. Write an equation for the velocity of v(t) of the particle.
b. Write an equation for the position x(t) of the particle.
c. For what values of t, 0<=t<=pi, is the particle at rest

-------------------------------------
a = dv/dt
4*cos(2t) = dv/dt
v = Integral[4*cos(2t) dt] + C
v = 2 * sin(2t) + C
t = 0 -> v = 1.
1 = 2 * sin(2*0) + C
C = 1
v(t) = 2 * sin(2t) + 1

How would I go about x(t)?

And for c. 2sin(2t)+1=0 sin2t=-1/2
arcsin2t=(1/2)
t=-.261799?
 
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\frac{d^2x}{dt^2}=4\cos(2t)
\frac{dx}{dt}=\int 4\cos(2t)dt+c = 2sin2t+c
x=\int {2sin2t+c}dt+k
 


b. To find the position x(t) of the particle, we need to integrate the velocity function with respect to time. So, we have:
x(t) = Integral[2*sin(2t) + 1 dt] + C
x(t) = -cos(2t) + t + C
t = 0 -> x(0) = 0
0 = -cos(2*0) + 0 + C
C = 1
x(t) = -cos(2t) + t + 1

c. To find when the particle is at rest, we need to find the values of t for which the velocity is equal to 0. So, we have:
v(t) = 2*sin(2t) + 1 = 0
sin(2t) = -1/2
2t = arcsin(-1/2)
2t = -pi/6 or 5pi/6
t = -pi/12 or 5pi/12

Therefore, the particle is at rest at t = -pi/12 or 5pi/12, which are both within the given range of 0<=t<=pi.
 
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