AP Physics C Essential Calculus Examples of the calculus skills identified on the College Board AP Physics C Equation Sheet. Differentiation - Power Rule d n x = nx n−1 dx ( ) Example #1 Given the function, y = y o + v o t + 1 2 gt 2 d (y ). dt d 1 2gt 2 Find the first derivative, ( ) dy dy o d v o t = + + dt dt dt dy = 0 + v o + gt dt dy = v o + gt dt v = v o + gt ( ) dt Find the second derivative, d (v ). dt ( ) dv dv o d gt = + dt dt dt dv = 0+g dt dv =g dt a=g Example #2 d n du u = nun−1 dx dx ( ) Given v = ( 2ax = 2ax ) 1 2 1 = u 2 ; u = 2ax ; du = 2a dx 1 1 d n d ! 2 $ 1 −2 a a a ##u && = u 2a = u = = = dx dx " % 2 2x u 2ax ( ) ( ) www.PhysicsJedi.net Differentiation – Chain Rule df df du = dx du dx Example #3 Given the functions v x = at (1) and x = 1 2 dv . From the equations at (2). Find the acceleration, a = 2 dt given it is obvious the acceleration is “a”. Now write an equation for the velocity as a function of horizontal position. Solve equation (2) for time and substitute into equation (1). ! 2x $ & = 2ax v x = a ## & a " % Again find the acceleration, a = a= dv dv dx dv = = v dt dx dt dx dv 1 = 2ax dx 2 ( a= dv . Since vx is not a function of time, apply the chain rule. dt ) − 1 2 2a = a 2ax ! a $ dv v =# & 2ax = a dx " 2ax % Differentiation – Trig Functions d sinx = cos x dx ( d cos x = −sinx dx ) ( ) d tanx = sec 2 x dx The derivatives of ALL trig functions starting with “c” are negative. d (sin u) = cos u du dx dx d (cos u) = − sin u du dx dx Example Find the first derivative Let u = ωt + φ and d (A sin(ωt + φ)) dt du =ω dt d (sin u) = A d (sin(Aω + φ)) = A cos(Aω + φ)(ω) = Aω cos(Aω + φ) dt dt www.PhysicsJedi.net ( ) Differentiation – The Product Rule Always use the product rule; never the quotient rule. d (uv ) = u dv + v du dx dx dx Example Differentiate f = x x2 + 1 ( ) Express f as product; f = x x 2 + 1 ( ) Let u = x and v = x 2 + 1 − − 1 2 1 2 d (f ) = d (uv ) = u dv + v du dx dx dx dx 3 1 d (f ) = d (uv ) = x⎛⎜ − 1 ⎞⎟ x 2 + 1 − 2 (2x ) + x 2 + 1 − 2 dx dx ⎝ 2 ⎠ ( d (f ) = d (uv ) = − dx dx d (f ) = d (uv ) = − dx dx d (f ) = d (uv ) = dx dx ) x2 (x 3 2 +1 ) 1 + ) (x 2 ( 2 1 ) +1 2 (x + 1) (x + 1) (x + 1) x2 2 3 2 2 + 2 3 2 1 (x 2 3 ) +1 2 www.PhysicsJedi.net Differentiation – e d x e = ex dx ( ) d u du e = eu dx dx ( ) Example Differentiate e − kx Let u = −kx and du = −k dx d −kx du e = eu dx dx ( ) d −kx e = e −kx (− k ) dx ( ) d −kx e = −ke −kx dx ( ) Differentiation – ln d (ln x ) = 1 dx x d (ln u) = 1 du dx u dx www.PhysicsJedi.net Integration – Power Rule 1 n ∫ x dx = n + 1 x n +1 , n ≠ −1 Example #1 1 2 ∫ kx dx = 2 + 1kx 2 +1 = 1 3 kx This is an indefinite integral. 3 Problems typically require limits of integration. ∫ 3 2 kx 2 dx = 1 3 3 1 3 1 3 8 19 kx |2 = k3 − k 2 = 9k − k = k 3 3 3 3 3 Example #2 1 n ∫ u du = n + 1u 2x ∫ (x 2 ∫ (x 2 dx Let u = x 2 + 1 and du = 2xdx 3 dx = 2x ) +1 , n ≠ −1 3 ) +1 n +1 −3 +1 −2 1 1 −1 x2 + 1 = − x2 + 1 = 2 2 − 3 +1 2 2 x +1 ( ) ( ) ( ) Example #3 ∫ (x x 2 3 ) +1 dx Let u = x 2 + 1 and du = 2xdx From the equation du = xdx; need du = 2xdx; missing 2. Multiple by “1”. 2 1 2x 1 ⎛⎜ − 1 ⎞⎟ −1 dx = dx = = 3 3 2 ∫ 2 x2 + 1 2 ⎜⎝ 2 x 2 + 1 ⎟⎠ 4 x 2 + 1 2 x2 + 1 2 ∫( x ) ( ) ( ) ( ) www.PhysicsJedi.net Integration – Trig Functions ∫ sin x = − cos x ∫ cos x = sinx Integration – e ∫e x = ex u u ∫ e du = e Example #1 ∫ − 2kxe −kx 2 dx Let u = −kx 2 and du = −2kxdx ∫ − 2kxe −kx 2 dx = ∫ eudu = e −kx 2 Example #2 2 −kx 2 ∫ xe dx Let u = −kx and du = −2kxdx From the equation du = xdx; need du = -2kxdx; missing -2k. Multiple by “1”. ∫ xe −kx 2 2 2 − 2k 1 1 dx = − 2kxe−kx dx = − e −kx ∫ − 2k − 2k 2k www.PhysicsJedi.net Integration – ln 1 ∫ x dx = ln x Example #1 Integrate ∫ dv where “v” represents velocity v dv = ln v This is an indefinite integral. v ∫ Problems typically require limits of integration. ⎛ v dv = ln v |vv if = ln v f − ln v i = ln⎜⎜ f vi v ⎝ v i ln x Recall e = x ∫ vf ⎞ ⎟⎟ ⎠ du = ln u u ∫ Example #2 Integrate kdq ∫ (1 + kq) where “q” represents charge Let u = 1 + q and du = kdq kdq ∫ (1 + kq) = ∫ du = ln1 + q u Example #3 dq ∫ (k − q) Let u = 1 − q and du = −dq From the equation du = dq; need du = -dq; missing -1. Multiple by “1”. dq −1 ∫ (k − q) − 1 = −1∫ (− 1)dq = − ln k − q k−q This is an indefinite integral. Problems typically require limits of integration. qf dq qf 0 ∫ (k − q) = − ln k − q | 0 Recall e −ln x = e ln 1 x = ⎛ k − q ⎞ = − ln(k − qf ) − (− ln(k − 0 )) = −[ln(k − qf ) − ln(k )] = − ln⎜ ⎟ ⎝ k ⎠ 1 x www.PhysicsJedi.net Differential Equations B d2 f x ( ) + Cf dx 2 (x) = 0 B and C are constants Rearrange so the second derivative term has no coefficients. d2 f x ( )+Cf dx 2 B (x) = 0 Suppose the constants “B” and “C” equal 1. d2 f x ( )+f dx 2 (x) = 0 What function when differentiated twice and added to itself equals zero? () d2 f x ( ) = −sin x () dx () f x = sin x 2 OR () d2 f x ( ) = −cos x () dx () f x = cos x 2 Now let B≠1 and C ≠1 () ( ) Let f x = sin ωx and d2 f x ( ) = −ω dx 2 2 ( ) sin ωx Substitute the above equations into the general form of the differential equation. d2 f x ( )+Cf dx 2 B (x) = 0 −ω2 sin ωx + ( ) C sin ωx = 0 B ( ) Solve for ω ω2 = C B ω= C B () ! C $ ! $ & OR f x = A sin # C x & x # B & # B & " % " % Final form of the solution. f x = sin # () www.PhysicsJedi.net