12.07.2015 Views

Simple Nature - Light and Matter

Simple Nature - Light and Matter

Simple Nature - Light and Matter

SHOW MORE
SHOW LESS
  • No tags were found...

You also want an ePaper? Increase the reach of your titles

YUMPU automatically turns print PDFs into web optimized ePapers that Google loves.

Incorrect solution #4:(same notation as above)Incorrect solution #5:(same notation as above)A x = (5.0 km) cos 45 ◦ = 3.5 kmB x = −(12.0 km) cos 55 ◦ = −6.9 kmA y = (5.0 km) sin 45 ◦ = 3.5 kmB y = −(12.0 km) sin 55 ◦ = −9.8 kmC x = A x + B x= −3.4 kmC y = A y + B y= −6.3 km√|C| = Cx 2 + Cy2= 7.2 kmdirection = tan −1 (−6.3/ − 3.4)= 62 ◦ north of eastA x = (5.0 km) cos 45 ◦ = 3.5 kmB x = −(12.0 km) sin 55 ◦ = −9.8 kmA y = (5.0 km) sin 45 ◦ = 3.5 kmB y = −(12.0 km) cos 55 ◦ = −6.9 kmC x = A x + B x= −6.3 kmC y = A y + B y= −3.4 km√|C| = Cx 2 + Cy2= 7.2 kmdirection = tan −1 (−3.4/ − 6.3)= 28 ◦ north of east3.4.4 Calculus with vectorsy / Visualizing the accelerationvector.DifferentiationIn one dimension, we define the velocity as the derivative of theposition with respect to time, <strong>and</strong> we can think of the derivative aswhat we get when we calculate ∆x/∆t for very short time intervals.The quantity ∆x = x f − x i is calculated by subtraction. In threedimensions, x becomes r, <strong>and</strong> the ∆r vector is calculated by vectorsubtraction, ∆r = r f − r i . Vector subtraction is defined componentby component, so when we take the derivative of a vector, this meanswe end up taking the derivative component by component,v x = dxdt ,v y = dydt ,v z = dzdt208 Chapter 3 Conservation of Momentum

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!