Unable to Understand How X2^2 Gets Canceled Out

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The discussion centers on the cancellation of x2^2 in the equation $$\frac{1}{2}kx_2^2=\frac{1}{2}mv_1^2$$ when solving for v1. Participants clarify that x2 is factored out to enhance readability and simplify calculations, allowing for a more straightforward expression of v1 as $$v_1=\sqrt{\frac{k}{m}}x_2$$. The importance of maintaining clarity in mathematical expressions is emphasized, particularly when deriving numerical solutions. Additionally, there is a critique regarding the explanation of elastic potential energy, suggesting that the reference point for potential energy should be treated as arbitrary to avoid complicating the analysis. Overall, the conversation highlights the balance between mathematical simplification and physical interpretation in problem-solving.
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Homework Statement
Unable to solve for solution.
Relevant Equations
Kinematic energy and spring energy
Am unable to understand how in the final answer the X2^2 gets canceled out without being inside the radical. It doesn’t make sense to me.

Any help explaining would be much appreciated as I am stuck.

Also am happy to provide more information if needed.
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Can you solve the equation$$\frac{1}{2}kx_2^2=\frac{1}{2}mv_1^2$$for ##v_1## in terms of the other quantities? What do you get?
 
kuruman said:
Can you solve the equation$$\frac{1}{2}kx_2^2=\frac{1}{2}mv_1^2$$for ##v_1## in terms of the other quantities? What do you get?

Yes it’s just x2 to take out the 1/2 after factoring on both sides then divide by M.

I’m more trying to understand why the x is left outside and isn’t inside the radical also. In this one here it’s left outside when usually it’s left inside.

Is there a particular reason?
 
The only reason I can think of is "simplify as much as you can to enhance readability and ease of calculation". Remember that $$\omega=\sqrt{\frac{k}{m}}$$ so that$$v_1=\sqrt{\frac{k}{m}}x_2=\omega \ x_2$$ The last result is simpler and more readable. Besides, if you want to find a number for ##v_1## and you put ##x_2^2## under the radical, you will have to square ##x_2## and then take its square root.
 
kuruman said:
The only reason I can think of is "simplify as much as you can to enhance readability and ease of calculation". Remember that $$\omega=\sqrt{\frac{k}{m}}$$ so that$$v_1=\sqrt{\frac{k}{m}}x_2=\omega \ x_2$$ The last result is simpler and more readable. Besides, if you want to find a number for ##v_1## and you put ##x_2^2## under the radical, you will have to square ##x_2## and then take its square root.
Note that ##v^2=x^2##, simplifies to ##v=\pm x##. Be careful not to simplify one of the two solutions out of existence.
 
jbriggs444 said:
Note that ##v^2=x^2##, simplifies to ##v=\pm x##. Be careful not to simplify one of the two solutions out of existence.
When a numerical answer is required, there should be enough information to select the solution that makes physical sense. The figure shows the cart moving to the right before hitting the spring therefore it is safe to conclude that the velocity is positive. That point should have been clarified in the solution.

I am bothered more by the solution's last pronouncement, "Elastic potential energy is always measured from the unstretched or uncompressed length of the spring." It unnecessarily complicates the analysis of the vertical mass-spring system and undermines the idea that the choice of the reference point of potential energy is arbitrary.
 
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