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Alina [70]
3 years ago
11

A mass is undergoing simple harmonic motion. When its displacement is 0, it is at its equilibrium position. At that moment, its

speed is _______ and its acceleration is _______.
0, 0
max, max
0, max
max, o
Physics
1 answer:
Nostrana [21]3 years ago
4 0

Answer:

Its speed is maximum and its acceleration is zero

Explanation:

- Concerning the speed:

In a simple harmonic motion, the speed can be determined through the law of conservation of energy. In fact, we have that the total mechanical energy of the system, which is sum of elastic potential energy U and kinetic energy K, is constant:

E=U+K=\frac{1}{2}kx^2+\frac{1}{2}mv^2

where k is the spring constant, x is the displacement, m is the mass and v is the speed.

We see that when the displacement is 0, x = 0: this means that the elastic potential energy U is also 0, therefore the kinetic energy K is maximum, and so the speed v is also maximum.

- Concerning the acceleration:

According to Newton's second law, the acceleration of the system is proportional to the net force:

a=\frac{F}{m}

the net force is just the restoring force of the spring, given by Hooke's law:

F=-kx

So, the acceleration is

a=-\frac{kx}{m}

and we see that when the displacement is zero, x = 0, and so the acceleration is also zero.

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The 100-m dash can be run by the best sprinters in 10.0 s. A 66-kg sprinter accelerates uniformly for the first 45 m to reach to
irga5000 [103]

(a) 154.5 N

Let's divide the motion of the sprinter in two parts:

- In the first part, he starts with velocity u = 0 and accelerates with constant acceleration a_1 for a total time t_1 During this part of the motion, he covers a distance equal to s_1 = 45 m, until he finally reaches a velocity of v_1 = u + a_1t_1. We can use the following suvat equation:

s_1 = u t_1 + \frac{1}{2}a_1t_1^2

which reduces to

s_1 = \frac{1}{2}a_1 t_1^2 (1)

since u = 0.

- In the second part, he continues with constant speed v_1 = a_1 t_1, covering a distance of d_2 = 55 m in a time t_2. This part of the motion is a uniform motion, so we can use the equation

s_2 = v_1 t_2 = a_1 t_1 t_2 (2)

We also know that the total time is 10.0 s, so

t_1 + t_2 = 10.0 s\\t_2 = (10.0-t_1)

Therefore substituting into the 2nd equation

s_2 = a_1 t_1 (10-t_1)

From eq.(1) we find

a_1 = \frac{2s_1}{t_1^2} (3)

And substituting into (2)

s_2 = \frac{2s_1}{t_1^2}t_1 (10-t_1)=\frac{2s_1}{t_1}(10-t_1)=\frac{20 s_1}{t_1}-2s_1

Solving for t,

s_2+2s_1=\frac{20 s_1}{t_1}\\t_1 = \frac{20s_1}{s_2+2s_1}=\frac{20(45)}{55+2(45)}=6.2 s

So from (3) we find the acceleration in the first phase:

a_1 = \frac{2(45)}{(6.2)^2}=2.34 m/s^2

And so the average force exerted on the sprinter is

F=ma=(66 kg)(2.34 m/s^2)=154.5 N

b) 14.5 m/s

The speed of the sprinter remains constant during the last 55 m of motion, so we can just use the suvat equation

v_1 = u +a_1 t_1

where we have

u = 0

a_1  =2.34 m/s^2 is the acceleration

t_1 = 6.2 s is the time of the first part

Solving the equation,

v_1 = 0 +(2.34)(6.2)=14.5 m/s

3 0
3 years ago
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