rudransh verma
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jbriggs444 said:Why are you dividing by m only to end up multiplying by m?

jbriggs444 said:Why are you dividing by m only to end up multiplying by m?

Knowing what you now know, what would your working be if this were a piece of homework or an examination question?rudransh verma said:![]()
Simple , upto a= 25 m/s^2 is right. Then just add the above part. Question done! 200 marks out of 100.Steve4Physics said:Knowing what you now know, what would your working be if this were a piece of homework or an examination question?
It's not that simple for me because I am having trouble sorting out the logical sequence "up to a = 25 m/s^2" in all these posts (93 and counting). Would it be possible for you to post the entire solution, from beginning to end, in one complete post? Thank you.rudransh verma said:Simple , upto a= 25 m/s^2 is right. Then just add the above part. Question done! 200 marks out of 100.
Your working up to finding a=25m/s² did not correctly apply a stated sign-convention. Purely by chance, you ended up with the correct sign (+25m/s², assuming we are using upwards-is-positive).rudransh verma said:Simple , upto a= 25 m/s^2 is right. Then just add the above part. Question done! 200 marks out of 100.
That’s much better. 9/10 (or 10/10 on a good day)!rudransh verma said:$$v^2=u^2+2as$$
$$v=+-10m/s$$
Taking -ve sign!
Again $$v^2=u^2+2as$$
$$a=+25m/s^2$$
So, $$Friction= F net+mg$$
$$(.2*25 + (.2)10)$$
$$Friction= +7 N$$
Thank you for the detailed solution. I think that you are unclear about the meaning of the symbols in your first equation. I understand that you have taken "up" as positive and "down" as negative. I also understand that in the expression $$v^2=u^2+2as$$ you have taken ##v =-10## m/s to be the velocity of the knife just before it hits the cardboard and ##u=0## is the final velocity of the knife. That is all correct and consistent. My question is, what about ##s##? It should represent the displacement of the knife. Since the knife ends up below its initial position, the displacement must be negative, i.e. ##s=-2~##m. If I substitute, I get $$(-10~\text{m/s})^2=0^2+2a(-2\text{m})$$ $$100~(\text{m/s})^2=-4~a~(\text{m})$$ $$a=-25~\text{m/}{\text{s}}^2.$$Something isn't right because we know that the acceleration is positive.rudransh verma said:$$v^2=u^2+2as$$ $$v=+-10m/s$$ Taking -ve sign!
Again $$v^2=u^2+2as$$ $$a=+25m/s^2$$ So, $$Friction= F net+mg$$ $$(.2*25 + (.2)10)$$ $$Friction= +7 N$$
I think @rudransh verma's working (in full) iskuruman said:the displacement must be negative, i.e. ##s=-2~##m. If I substitute, I get $$(-10~\text{m/s})^2=0^2+2a(-2\text{m})$$ $$100~(\text{m/s})^2=-4~a~(\text{m})$$ $$a=-25~\text{m/}{\text{s}}^2.$$Something isn't right because we know that the acceleration is positive.
I am not sure. @rudransh verma uses ##v## on the left and ##u## on the right side of his equation without subscripts that specify what they stand for. Furthermore, he clearly identifies v = ±10 m/s. Why did you feel the need to use subscripts ##i## and ##f## in your equation which he doesn't use? My point is exactly yours: without subscripts one can get easily confused about what's what and where. I think the most efficient way to write this equation is in the form of the work-energy theorem per unit mass $$\vec a \cdot \vec s=\frac{1}{2}\left(v_{\!f}^2-v_{\!i}^2 \right)$$ which makes it independent of one's choice of axes.Steve4Physics said:I think @rudransh verma's working (in full) is
##v_f^2 = v_i^2+ 2as## we get
##0^2 = (-10)^2 + 2a(-2)##
##4a = 100##
##a = 25m/s## (positive as required)
I've assumed the standard equation ##v^2=u^2+2as## has been used correctly. Maybe I'm too trusting!kuruman said:I am not sure. @rudransh verma uses ##v## on the left and ##u## on the right side of his equation without subscripts that specify what they stand for. Furthermore, he clearly identifies v = ±10 m/s.
For disambiguation.kuruman said:Why did you feel the need to use subscripts ##i## and ##f## in your equation which he doesn't use?
I agree suffixes should be used to avoid ambiguities.kuruman said:My point is exactly yours: without subscripts one can get easily confused about what's what and where. I think the most efficient way to write this equation is in the form of the work-energy theorem per unit mass $$\vec a \cdot \vec s=\frac{1}{2}\left(v_{\!f}^2-v_{\!i}^2 \right)$$ which makes it independent of one's choice of axes.
That's a really neat trick I've not seen before.kuruman said:Actually, the question is even more easily solved when one applies the relevant equation piecewise to the overall motion from start to finish in which case ##v_i=v_f=0.## Then $$a_1s_1 +a_2s_2=0$$ ...