EXPERIMENT – Measurement Error (Bounds) The knowledge we

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EXPERIMENT – Measurement Error (Bounds)
The knowledge we have of the physical world is obtained by doing experiments and making
measurements. It is important to understand how to express such data and how to analyze and
draw meaningful conclusions from it. In doing this it is crucial to understand that all
measurements of physical quantities are subject to uncertainties. Indeed, typically more effort is
required to determine the error or uncertainty in a measurement than to perform the
measurement itself. The result of any measurement has two essential components: (1) a
numerical value (in a specified system of units) giving the best estimate possible of the quantity
measured, and (2) the degree of uncertainty associated with this estimated value. For example, a
measurement of the width of a table would yield a result as w = (95.3 +/- 0.1) cm.
Today we will discuss using a method to establish a tolerance or bound for your best estimate for
density of a block of wood. When using a ruler to measure a length, we are limited by the scale
markings on the ruler. We can locate the best estimate for length using our ruler by locating the
lower scale marking below the length and the upper scale marking above the length and using a
best estimate for the length. For example if the length of the block of wood is located between
the scale markings of 20.30 cm and 20.40 cm and we estimated the length to be seven tenths of
the distance between the two scale markings; we would have a lower bound of 20.30 cm, a best
estimate of 20.37 cm, and an upper bound of 20.40 cm for length.
Objective:
Investigation of error using bounds
Equipment:
Rectangular block of wood, triple beam balance calibrated to read mass, ruler or meter stick
Procedure:
1. Measure length of block of wood. Record in data table lower bound, best estimate, and
upper bound for length. Repeat with measurements for width and height of block of
wood.
2. Measure mass of block of wood. Record lower bound, best estimate, and upper bound for
mass.
Data Table
Lower bound
Best estimate
Upper bound
Best estimate
Upper bound
Length (cm)
Width (cm)
Height (cm)
Mass (g)
Calculations
Convert the measurements to SI units.
Lower bound
Length (m)
Width (m)
Height (m)
Mass (Kg)
Density for a block of wood is calculated by dividing the mass of the block of wood by the
volume of the block, where volume is the product of the block’s length, width, and height.
=
π‘š
π‘š
=
𝑉 π‘™π‘€β„Ž
To calculate density best estimate for the block of wood, use the values for best estimates for
mass, length, width, and height in SI units.
𝐡𝐸 =
π‘šπ΅πΈ
𝑉𝐡𝐸
=𝑙
π‘šπ΅πΈ
𝐡𝐸 𝑀𝐡𝐸 β„Žπ΅πΈ
=(
(
)(
)
)(
)
=
Use original data to determine significant figures and report final result.
𝐡𝐸 =
To calculate density upper bound for the block of wood, use the upper bound for mass and the
lower bounds for length, width, and height in SI units so as to make the fraction for density upper
bound as large as possible..
ο²π‘ˆπ΅ =
(
)(
π‘šπ‘ˆπ΅
π‘šπ‘ˆπ΅
=
=
𝑉𝐿𝐡
𝑙𝐿𝐡 𝑀𝐿𝐡 β„ŽπΏπ΅ (
)
)(
)
=
Use original data to determine significant figures and report final result.
ο²π‘ˆπ΅ =
To calculate density lower bound for the block of wood, use the lower bound for mass and the
upper bounds for length, width, and height in SI units so as to make the fraction for density as
large as possible..
𝐿𝐡 =
(
)(
π‘šπΏπ΅
π‘šπΏπ΅
=
=
π‘‰π‘ˆπ΅ π‘™π‘ˆπ΅ π‘€π‘ˆπ΅ β„Žπ‘ˆπ΅ (
)
)(
)
=
Use original data to determine significant figures and report final result
𝐿𝐡 =
We can then report that density best estimate 𝐡𝐸 is trapped between density lower bound
𝐿𝐡 and density upper bound ο²π‘ˆπ΅ . (𝐿𝐡 < 𝐡𝐸 < ο²π‘ˆπ΅ )
We can calculate the error between the density best estimate and the density upper bound as
𝑑1 = ο²π‘ˆπ΅ − 𝐡𝐸
and the error between the density best estimate and the density lower bound as 𝑑2 = 𝐡𝐸 − 𝐿𝐡 .
𝑑1 =
𝑑2 =
We can then report the density of our block of wood as  = 𝐡𝐸 βˆ“ 𝑑, where d is the larger of d1
or d2.
 =
We are then assured that our density best estimate is uncertain by no more than our error d.
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