This experiment investigated factors that affect the period of a pendulum. It was found that the length of the string affected the period, with longer strings resulting in longer periods. Specifically, doubling the length of the string doubled the period. The mass of the pendulum did not affect the period. Finally, the angle of the pendulum swing was found to not significantly impact the period either.
Hypothesis: The 4 factors which can affect the strength of an electromagnet are the type of core used, the number of turns of wire, the magnitude of the current used and the shape of the solenoid.
Aim: To investigate the factors which affect the strength of an electromagnet.
English SBA for CSEC. *The file has been protected and has been submitted to CXC. Do not copy as the digital signature of the file cannot be removed or edited. Use as a guide only
This is a guide in maximizing your scores in your School Based Assessment. Please do not plagiarize, it will not only affect you it will also affect your school, teachers and also your parents. Remember, nothing worth having comes easy. Work hard!!!
Hypothesis: The 4 factors which can affect the strength of an electromagnet are the type of core used, the number of turns of wire, the magnitude of the current used and the shape of the solenoid.
Aim: To investigate the factors which affect the strength of an electromagnet.
English SBA for CSEC. *The file has been protected and has been submitted to CXC. Do not copy as the digital signature of the file cannot be removed or edited. Use as a guide only
This is a guide in maximizing your scores in your School Based Assessment. Please do not plagiarize, it will not only affect you it will also affect your school, teachers and also your parents. Remember, nothing worth having comes easy. Work hard!!!
Week 3 OverviewLast week, we covered multiple forces acting on.docxmelbruce90096
Week 3 Overview
Last week, we covered multiple forces acting on an object. This week we will cover motion in two dimensions, inclined planes, circular motion, and rotation.
Forces in Two Dimensions (1 of 2)
So far you have dealt with single forces acting on a body or more than two forces that act parallel to each other. But in real life situations more than one force may act on a body. How are Newton's laws applied to such cases? We will restrict the forces to two dimensions.
Since force and acceleration are vectors, Newton's law can be applied independently to the X and Y-axes of a coordinate system. For a given problem you can choose a suitable coordinate system. But once a coordinate system is chosen, we have to stick with it for that problem. The example that follows shows how to find the acceleration of a body when two forces act on it at right angles to each other.
Forces in Two Dimensions (2 of 2)
To find the resultant acceleration we draw an arrow OA of length 3 units along the X-axis and then an arrow AB of length 4 units along the Y-axis. The resultant acceleration is the arrow OB with the length of 5 units. Therefore, the acceleration is 5 m/s2 in the direction of OB. Also when you measure the angle AOB with a protractor, we find it to be 53°.
The acceleration caused by the two forces is 5 m/s2 at an angle of 53°.
Uniform Circular Motion
When an object travels in a circular path at a constant speed, its motion is referred to as uniform circular motion, and the object is accelerated towards the center of the circle. If the radius of the circular path is r, the magnitude of this acceleration is ac = v2 / r, where v is its speed and ac is called the centripetal acceleration. A centripetal force is responsible for the centripetal acceleration, which constantly pulls the object towards the center of the circular path. There cannot be any circular motion without a centripetal force.
Banking
When there is a sharp turn in the road or when a turn has to be taken at a high speed as in a racetrack, the outer part of the road or the track is raised from the inner part of the track. This is called banking. It provides additional centripetal force to a turning vehicle so that it doesn't skid.
The angle of banking is kept just right so that it provides all the centripetal force required and a motorist does not have to depend on the friction force at all.
Inclined Planes
Forces on an Inclined Plane
The inclined plane is a device that reduces the force needed to lift objects. Consider the forces acting on a block on an inclined surface. The inclined surface exerts a normal force FN on the block that is perpendicular to the incline. The force of gravity, FG, points downward. If there is no friction, the net force, Fnet, acting on the block is the resultant of FN and FG. By Newton's second law the net force must point down the incline because the block moves only along the incline and not perpendicular to it.
The vector triangle shows .
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CSEC Physics Lab - Factors affecting period of a pendulum
1. Thisexperimentwascarriedoutto investigatethe factorsthataffectthe periodof a pendulum.
A pendulumisaweighthungfroma fixedpointsothatitcan swingfreely. The total energythroughout
the movementof the pendulumremainsconstant.Atitshighestpoint,ithasitsmaximumpotential
energyandno kineticenergy.Asitbeginstofall,the potential energybeginstochange intokinetic
energyuntil itreachesits lowestpointwhere the kineticenergyisata maximumandthe potential
energyisequal tozero.Whenit beginstorise againthe kineticenergybeginstochange potential energy
until itreachesitsmaximumonce againat the highestpoint.
A pendulummovesbackandfro due to gravity. Whenthe massis drawnupwardsand letgo,the
force of gravityacceleratesitbackto the original position.The momentumbuiltupbythe acceleration
of gravitycausesthe massto thenswinginthe opposite direction to aheightequal tothe original
position. Thisforce iscalledinertia:(itstendencytoresistitsstate of motion.)
It was shownthatthe lengthof the stringaffectedthe periodof a pendulum.Thiswasdisplayed
inthe resultsasthe differenttimestaken for20 oscillationswhilstchangingthe lengthof the string
variedfrom12.60 to 30.90 seconds.Meanwhile the timescalculatedforone oscillationvariedfrom0.63
to 1.54 seconds. Here the reasoningbehindthisfinding. Anobjectonapendulumwithalongstringis
furtherawayfrom the axisof the pendulum.Thismeansthatithas to covera longerdistance toreturn
to where itcame from.This isthe case since a longerradiusfromthe axisof rotationmeansa longerarc
lengthforthe bob to travel along. The formulalinkingthe lengthof the stringtothe periodof the
pendulumisseenbelow:
𝑇 = 2𝜋√𝑙
𝑔
Where ‘T’ isthe period,‘l’isthe lengthof the stringand ‘g’is the gravitational fieldstrength.
The mass of the bobdoesn’taffectthe periodof the pendulumsince the movementisdue to
gravity.Accelerationdue togravityisaconstant figure( 9.8ms-2
) and no matterhow heavythe bobis,
the pendulumwillaccelerateatthisrate and take the same amountof time tocomplete one backand
fro movement.Asshowninthe experiment,the time takenfor20 oscillationsonlyvariedfrom24.10 to
25.18 seconds.Thisvariationinthe resultsisonlytodue the randomerror and the vary reactiontimes
to measure the oscillations.The timescalculatedforone oscillationwithvaryingmassesalsohada small
range from 1.21 to 1.26 seconds.
Finallythe angle of displacementwastestedandresultsshowedthatthisfactordoesn’treally
affectthe periodof a pendulum.Timesfor20 oscillationsrecordedatdifferentanglesvariedonlyfrom
21.65 to 22.65 secondswhilstthe time calculatedforone oscillationrange from1.08 to only1.13
seconds.Whenthe angle of displacementincreases,the startingheightof the bobishigherthusitwill
accelerate overa longerperiodandgaina greatervelocity.However,thismovementisoveralonger
distance,sothe time takenforone oscillationwill notdecrease.Itwill remainconstant.
It was advisable todivide the resultsby20 to reduce randomerror due to humanreactiontime.
2. Sources of Error
Sourcesof Error:
- The time for one oscillationwasslightlyinaccurateasfrictiondue toair resistance slowsthe
pendulumdownwitheachswing.
- The time for twentyoscillationswasslightlyinaccuratedue tothe time taken(human
reactiontime) tostart and stopthe watch.
- There was uncertaintyinthe reference pointatwhichtostart and the stop the watch.
- There wasa bitof uncertaintyaboutwhichpointof swingtotime.
Precautions
- The time takenfor 20 oscillationswasdividedby20 to reduce the error due to human
reactiontime.
- All windowswere closedtoensure thatthe force of the winddidnot affectthe movement
of the pendulum.