Solving for time when delta x=0?

  • Thread starter Thread starter atypical
  • Start date Start date
  • Tags Tags
    Delta Time
Click For Summary
The discussion centers on understanding the equation for time when the change in position (delta x) is zero. It clarifies that while delta x can be zero, the initial velocity and acceleration can still be non-zero, leading to two solutions for time: t=0 and another derived from the quadratic equation. The conversation highlights that the object can have an initial velocity that eventually decreases to zero due to acceleration acting in the opposite direction, such as gravity in vertical motion. The confusion arises from visualizing constant position versus the dynamics of motion, where the object may return to its initial position after changing direction. The formula applies to both horizontal and vertical motion as long as acceleration remains constant.
atypical
Messages
13
Reaction score
0
So my physics book says "from x(final)=x(initial)+V(initial)t+1/2at^2 observe that when x(final)=x(initial), the time is given by t=-2V(initial)/a"
Now if change in x is equal to 0, wouldn't your velocity v(initial)t from above along with your acceleration also be zero?
How is the book getting the t equation when delta x is zero?
 
Physics news on Phys.org
What if x is the height of an object thrown into the air?
 
fzero said:
What if x is the height of an object thrown into the air?

ok, so what I said is correct for horizontal movement but not necessarily true for vertical moment, correct? I still do not see how the book is getting the time formula from observing that equation.
 
atypical said:
Now if change in x is equal to 0, wouldn't your velocity v(initial)t from above along with your acceleration also be zero?
That is one solution, yes. It is the trivial solution.

How is the book getting the t equation when delta x is zero?
In general you have

\frac 1 2 at^2 + v_0t + (x_0-x_f) = 0

That is a quadratic equation in t. Quadratic equations have two solutions. In the special case x0=xf this reduces to

\frac 1 2 at^2 + v_0t = 0

Factoring out the common t on the left-hand side,

(t)(\frac 1 2 at + v_0) = 0

So the two solutions are given by t=0 and 1/2 a t +v_0 = 0.
 
Ok, that made complete sense. I am a bit rusty on my math and forgot when you factor "t" out you get two solutions. But i am having trouble visually imagining this. Say you visually imagine x position graph. If there is no change in x horizontally (when x(initial)=x(final)), you would have a constant line between your initial and final values of x in that time interval. Now, if your position remains a constant, then you can't have any slope therefore your velocity and acceleration would have to be zero. What am i overlooking?
 
atypical said:
Ok, that made complete sense. I am a bit rusty on my math and forgot when you factor "t" out you get two solutions. But i am having trouble visually imagining this. Say you visually imagine x position graph. If there is no change in x horizontally (when x(initial)=x(final)), you would have a constant line between your initial and final values of x in that time interval. Now, if your position remains a constant, then you can't have any slope therefore your velocity and acceleration would have to be zero. What am i overlooking?

The position is not a constant, while

x(t=t_i) = x(t=t_f),

for times t_i<t<t_f it's given by x(t). What is physically happening is that the acceleration a must act in the opposite direction from the initial velocity v_i. At some time t=t_*, the velocity v(t_*)=0 and after that the object is pushed back until it's at its initial position.

The formula doesn't care whether or not this is horizontal or vertical motion as long as the acceleration is constant. The case of vertical motion where a=-g is due to gravity is just the clearest real-life example.
 
The book claims the answer is that all the magnitudes are the same because "the gravitational force on the penguin is the same". I'm having trouble understanding this. I thought the buoyant force was equal to the weight of the fluid displaced. Weight depends on mass which depends on density. Therefore, due to the differing densities the buoyant force will be different in each case? Is this incorrect?

Similar threads

  • · Replies 1 ·
Replies
1
Views
2K
  • · Replies 6 ·
Replies
6
Views
1K
Replies
5
Views
869
  • · Replies 10 ·
Replies
10
Views
1K
  • · Replies 6 ·
Replies
6
Views
524
Replies
7
Views
1K
  • · Replies 3 ·
Replies
3
Views
890
Replies
29
Views
3K
  • · Replies 10 ·
Replies
10
Views
2K
  • · Replies 12 ·
Replies
12
Views
2K