(a) Let x = 14.75 ± 0.09. Evaluate F = 3x½.
First the principle value of F is
P(F) = 3(14.75)½ = 11.5217 .
Next, we take the derivative of F with respect to x
dF/dx = 3 / 2x½ .
The uncertainty in F is thus
δF = δx dF/dx = 0.09 × 3 / 2(14.75)½ = 0.0352 .
Keeping one figure in the uncertainty, the result is F = 11.52 ± 0.04.
(b) Let θ = 27.5 ± 0.5°. Evaluate F = sin(θ) - cos(θ).
First the principle value of F is
P(F) = sin(27.5°) - cos(27.5°) = -0.42526 .
Next, we take the derivative of F with respect to θ
dF/dθ = cos(θ) + sin(θ) .
The uncertainty in F is thus
δF = Δθ dF/dθ = (0.5° × π/180°) {cos(27.5)° + sin(27.5°)} = 0.0118 .
Keeping one figure in the uncertainty, the result is F = -0.43 ± 0.01.
(c) Let θ = 27.5 ± 0.5°. Evaluate F = sin(θ) + cos(θ).
First the principle value of F is
P(F) = sin(27.5°) + cos(27.5°) = 1.34876.
Next, we take the derivative of F with respect to
dF/dθ = cos(θ) - sin(θ) .
The uncertainty in F is thus
δF = Δθ dF/dθ = (0.5° × π/180°) |cos(27.5°) - sin(27.5°)| = 0.00371 .
Keeping one figure in the uncertainty, the result is F = 1.349 ± 0.004.
(d) Let t = 2.35 ± 0.06 s. Evaluate F = 5t2 - 3t + 2.
First the principle value of F is
P(F) = 5(2.35)2 -3(2.35) + 2 = 22.5625 .
Next, we take the derivative of F with respect to t
dF/dt = 10t - 3 .
The uncertainty in F is thus
δF = δt dF/dt = 0.06 {10(2.35) - 3} = 1.23 .
Keeping one figure in the uncertainty, the result is F = 23 ± 1.
(e) Let = 0.754 ± 0.004 rad. Evaluate F = [tan(θ)]½.
First the principle value of F is
P(F) = [tan(0.754)]½ = 0.96907 .
Next, we take the derivative of F with respect to t
dF/dθ = ½[tan(θ)]-½ / cos2(θ) .
The uncertainty in F is thus
δF = δt dF/dt = 0.004 × ½ /{ [tan(.754)]½ cos2(.754)} = 0.00388 .
Keeping one figure in the uncertainty, the result is F = 0.969 ± 0.004.
(a)
We need to do two partial derivatives
¶ z/¶ x = ½ (1/z) (2x) = x / z , and
¶ z/¶ y = ½ (1/z) (2y) = y / z .
The uncertainty in z is thus
δz = ( δx x + δy y) / z .
(b) R = Acos(θ)
We need to do two partial derivatives
¶ R/¶ A = cos(θ) , and
¶ R/¶q = -Asin(θ) .
The uncertainty in R is thus
δR = δA cos(θ) + Δθ Asin(θ).
(c) N = N0e-λt
We need to do three partial derivatives
¶ N/¶ N0 = e-λt = N/N0 ,
¶ N/¶l = -tN0 e-λt = -tN , and
¶ N/¶ t = -λN0 e-λt = -λN .
The uncertainty in N is thus
δN = N{δN0/N0 + dl t + δt λ }.
(d) F = A/B + C/D
We need to do four partial derivatives
¶ F/¶ A = 1/B ,
¶ F/¶ B = -A/B2 ,
¶ F/¶ C = 1/D , and
¶ F/¶ D = -C/D2 .
The uncertainty in F is thus
δF = δA/B + δB A/B2 + δC/D + δD C/D2 .
(e) v = v0 + at
We need to do three partial derivatives
¶ v/¶ v0 = 1 ,
¶ v/¶ a = t , and
¶ v/¶ t = a .
The uncertainty in v is thus
δv = δv0 + δa t + δt a.
(f)
We need to do three partial derivatives
¶ t/¶l = -(1/λ2)ln(R0/R) = -t/λ ,
¶ t/¶ R0 = (1 / λR0) , and
¶ t/¶ R = - (1 / λR).
The uncertainty in t is thus
δt = t dl/λ + (δR0/R0 + δR/R)/λ .
(g) d = v0t + ½at2
We need to do three partial derivatives
¶ d/¶ v0 = t ,
¶ d/¶ a = ½t2 , and
¶ d/¶ t = v0 + at .
The uncertainty in d is thus
δd = δv0 t + ½δa t2 + δt (v0 + at) .
(h) X = Rtan2(θ)
We need to do two partial derivatives
¶ X/¶ R = tan2(θ) , and
¶ X/¶q = 2R tan(θ) / cos2(θ) .
The uncertainty in X is thus
δX = δR tan2(θ) + Δθ 2Rtan(θ) / cos2(θ) .
(i)
We need to do three partial derivatives
¶ v/¶ R = ½[Rgtan(θ)]-½ gtan(θ) = gtan(θ) / 2v ,
¶ v/¶ g = ½[Rgtan(θ)]-½ Rtan(θ) = Rtan(θ) / 2v, and
¶ v/¶q = ½[Rgtan(θ)]-½ Rg/cos2(θ) = Rg / 2vcos2(θ)
The uncertainty in v is thus
δv = {[δR g + δg R]tan(θ) + Δθ Rg/cos2(θ)} / 2v .
(j) L = mvrsin(φ)
We need to do four partial derivatives
¶ L/¶ m = vrsin(φ) = L/m ,
¶ L/¶ v = mrsin(φ) = L/v ,
¶ L/¶ r = mvsin(φ) = L/r , and
¶ L/¶f = mvrcos(φ) = L/tan(φ) .
The uncertainty in L is thus
δv = L{δm/m + δv/v + δr/r + Δθ/tan(θ)} .
Questions?mike.coombes@kwantlen.ca