NYC College of Technology
Borough of Manhattan Community College
General Physics Ⅰ: Algebra-Based PHYS 1433 Physics Ⅰ: PHY 210
General Physics Ⅱ: Algebra-Based PHYS 1434
Sunday, December 11, 2016
Find Ratio of Powers of Emitted Radiation
Two spheres are made from the same material. The radius of the second sphere is twice less than the radius of the first sphere, but the absolute temperature of the second sphere is twice greater than the absolute temperature of the first sphere. Find p₂/p₁, the ratio of the powers of emitted radiations of the second (p₂), and the first (p₁) spheres.
Saturday, December 10, 2016
Sunday, November 27, 2016
Find the Change in Entropy
A
physical body with a constant mass and a constant heat capacity has
the change of entropy ΔS₁₂
when the temperature of the body changes from the initial temperature
T₁
to the final temperature T₂.
If this body changes the temperature from the same initial
temperature T₁
to the new final temperature T₃,
find the change in entropy for this body in terms of ΔS₁₂,
T₁,
T₂,
and T₃.
Find the heat Q₄₋₂₋₁, which is added to the gas in the process 4-2-1
In
the process of taking a gas from state 1 to state 4 along the curved
path the heat leaves the system is Q₁₋₄
and the work done on the system is W₁₋₄.
When
the gas is taken along the path 4-2-1, the work done by the gas is
W₄₋₂₋₁.
Find the heat Q₄₋₂₋₁,
which is added to the gas in the process 4-2-1, in terms of Q₁₋₄,
W₁₋₄,
W₄₋₂₋₁
What fraction of the original amount of air in the pressure vessel has been added into the pressure vessel?
A pressure vessel initially is filled
with air at the temperature T₁
and the gauge pressure P₁.
Finally air in the pressure vessel has the temperature T₂
and the gauge pressure P₂.
What fraction of the original amount of air in the pressure vessel
has been added into the pressure vessel, or removed from the pressure
vessel? The pressure vessel has a constant volume.
Find the root mean square velocity of molecules with the mass m₂
A mixture of two gasses consists of
molecules with the masses m₁
and m₂.
Molecules of mass m₁
have the root mean square velocity v₁.
Find the root mean square velocity of molecules with the mass m₂
in terms of m₁,
m₂, and v₁
What Fraction of the Original Air Must Be Removed?
A tire is filled with air at the temperature T₁ to a gauge pressure of P₁. If the tire reaches a temperature T₂, what fraction of the original air must be removed if the original pressure P₁ is to be maintained?
Friday, October 28, 2016
Wednesday, October 12, 2016
Gravitational Potential Energy
#PhysicsProblem #Physics #problem #object #floor #gravitational #potential #energy #Howmuch #PotentialEnergy #AboveTheFloor #GivenData pic.twitter.com/JPMwGoTW69— Physics I (@PHY210) October 12, 2016
A 1-kg object 2 m above the floor in a regular building at the Earth has a gravitational potential energy of 3 J.
How much gravitational potential energy does the object have when it is 4 m above the floor?
Given Data:
m = 1kg
y₁ = 2m
U₁ = 3J
y₂ = 4m
U₂ = ?
Useful Physics Formulas
U = mgh
ΔU = Δ(mgh) = mgΔh
Solution
ΔU = Δ(mgh) = mgΔh = mg(y₂ - y₁)
ΔU = U₂ - U₁
U₂ = U₁ + mg(y₂ - y₁)
U₂ = 3J + 1kg · 10ᵐ/s² · (4m - 2m) = 3J + 20J = 23J
Problem's answer is 23 J.
Δ·⁰¹²³⁴⁵⁶⁷⁸⁹⁺⁻⁼⁽⁾ⁱⁿᴬᴭᴮᴯᴱᴲᴳᴴᴵᴶᴷᴸᴹᴺᴻᴼᴽᴾᴿᵀᵁᵂᵃᵄᵅᵆᵇᵉᵊᵋᵌᵍᵏᵐᵑᵒᵓᵖᵗᵘᵚᵛᵝᵞᵟᵠᵡ₀₁₂₃₄₅₆₇₈₉₊₋₌₍₎ₐₑₒₓₔₕₖₗₘₙₚₛᵢᵣᵤᵥᵦᵧᵨᵩᵪ½↉⅓⅔¼¾⅕⅖⅗⅘⅙⅚⅐⅛⅜⅝⅞⅑⅒⅟℀℁℅℆
Friday, October 7, 2016
BMCC Students, Please Repeat Your Submission for the Quiz 2!
BMCC Students, Please repeat your submission for the quiz 2! Unfortunately for technical reasons your previous submissions of the quiz 2 were not recorded.
Tuesday, October 4, 2016
Physics Problem - A Spring is Fixed Vertically to the Floor
A #spring is fixed #vertically to the floor.
— Physics I (@PHY210) October 5, 2016
A 10-kg #box is then #pressed down such that the spring is #compressed https://t.co/Z5fLcbq2LX
Sunday, October 2, 2016
The potential energy of a 10-kg mass is given by ...
The potential energy is given by the function U(x) = kx⁻¹, where k is a constant, and variable x is the position, the coordinate. (a) Derive the function of the coordinate x, which describes the force produced by this potential energy.
F(x) = - d U(x) / dx
F(x) = - d kx⁻¹ / dx = kx⁻²
F(x) = kx⁻²
(b) Let this potential energy is obtained by the body with the mass of 10kg. The constant is known: k = -3.98 × 10¹⁵ Jm.
Find the force on this body when it is located atx = 6.38 × 10⁶ m?
Find the force on this body when it is located atx = 6.38 × 10⁶ m?
F(x) = kx⁻² = -3.98 × 10¹⁵ Jm / ( 6.38 × 10⁶ m)²
The code for the Google calculator: (-3.98E15J*m) / ( 6.38E6m )^2
Google calculator's result: -97.7781272 newtons
Problem's answer: F = -97.8 N or 97.8 N towards x = 0
Saturday, October 1, 2016
Constant Power
What is the power output of an engine when a car of mass M accelerates with the constant power from rest to a final speed V over a distance d on flat, level ground?
Ignore
energy lost due to friction and air resistance.
Derive a formula for the power P in terms of variables: the mass M, the final speed V, and the distance d.
P=P(M,V,d) ?
Derive a formula for the power P in terms of variables: the mass M, the final speed V, and the distance d.
P=P(M,V,d) ?
v=v(t)
The speed is a function of time.
Pt
= ½m v(t)²
Because of the energy conservation law.
v(t)²=2tP/m=(2P/m)t
v(t)=(2P/m)½t½
x(t)=(2P/m)½
(⅔t3/2)
x(t)²=(2P/m)
(⅔)²
t³
t=v(t)²
/ (2P/m)
t³=v(t)⁶
/ (2P/m)³
x(t)²=(2P/m)
(⅔)²
t³=(2P/m)
(⅔)²
v(t)⁶
/ (2P/m)³
x(t)²=(⅔)²
v(t)⁶
/ (2P/m)
²
x(t)=(⅔)
v(t)³
/ (2P/m)
2P/m
= (⅔) v(t)³
/ x(t)
P
= ½(⅔) v(t)³m
/ x(t)
P
= ⅓ v(t)³m
/ x(t)
= ⅓ V³m
/ d
Physics Problem - Find Average Power
What is the #average #power #output of an #engine when a #car of #mass M #accelerates #uniformly (a=const) from #rest to a final #speed V... pic.twitter.com/iqz40MQpOh
— Physics I (@PHY210) October 1, 2016
Friday, September 30, 2016
Physics Problem - Work, Kinetic Energy
Problem
from Quiz 5
A
train with the mass M
accelerates uniformly from the rest to the speed V
when passing through a distance d.
What is its kinetic energy
when it passing through a distance d₁ (d₁ < d)?
What is its kinetic energy
when it passing through a distance d₁ (d₁ < d)?
Given
Data: M = 15,000
kg
Vₒ
= 0
V
= 15
m / s
d
= 150
m
d₁
= 75
m
K₁
=
?
Solution:
K(kinetic
energy) = Kₒ(kinetic
energy initial) + W(work)
= W
W
= Fx
K
= W
= Fd
= ½MV²
F
= ½MV²
/ d
K₁
=
W₁
=
Fd₁
=
½MV²
d₁
/
d
K₁
= ½(15,000
kg)(15
m/s)²
(75m)
/
(150m) = 843750
J
Google
Calculator Code:
0.5*(15000
kg)*(15
m/s)^2*(75m)
/
(150m)
Answer:
840
kJ
Thursday, September 29, 2016
System of Two Pulleys and Two Masses
A photo posted by Vasiliy S. Znamenskiy (@znamenski) on
Monday, September 12, 2016
Thursday, September 1, 2016
2 Describing Motion: Kinematics in One Dimension
For students PHYS 1441 (NYC College of Technology) E474 [54392]: pic.twitter.com/Ta5cpIU7vK
— Physics I (@PHY210) September 1, 2016
Wednesday, August 31, 2016
PDF Versions of Textbook
In general, all exams in my class are open-book exams. It means students may use paper textbooks during exams. But I don't give permission to use in exams of any electronic devices except simple calculators. Students may use PDF versions of the textbook during lectures, laboratory lessons, or at home.
Tuesday, June 28, 2016
Wednesday, June 8, 2016
Wednesday, June 1, 2016
Saturday, May 28, 2016
Saturday, May 21, 2016
Friday, May 13, 2016
What is the change in entropy of the bullet during this process?
A bullet of mass m slams into a concrete wall and melts on impact. If the temperature of the speeding bullet was T₁ and if the specific heat of bullet's material is c and its latent heat of fusion is L, what is the change in entropy of the bullet during this process? The melting point of lead is T₂.
Heating:
dS₁ = dQ₁/T
dQ₁ = cmdT
dS₁ = cmdT/T = cmd(lnT)
ΔS₁ = ∫cmd(lnT) = cm∫d(lnT) = cm(lnT₂-lnT₁) = cm ln(T₂/T₁)
ΔS₁ = cm ln(T₂/T₁)
Melting:
dS₂ = dQ₂/T₂
ΔS₂ = ΔQ₂/T₂ = Lm/T₂
ΔS = ΔS₁+ΔS₂ = cm ln(T₂/T₁)+Lm/T₂
A 16-gram lead bullet slams into a concrete wall and melts on impact. If the temperature of the speeding bullet was 25°C and if the specific heat of lead is 0.13 kJ/(kgK) and its latent heat of fusion is 23 kJ/kg, what is the change in entropy of the bullet during this process? The melting point of lead is 601K.
m=16g
T₁=25°C=25°+273.15=298.15K
T₂=601K
c=0.13 kJ/(kgK)
L=23 kJ/kg
ΔS=cm ln(T₂/T₁)+Lm/T₂
Calculation by Google calculator:
0.13kJ/(kg*K) * 16g * ln(601 / 298.15) in J/K =
1.4580763 J / K
23kJ/kg * 16g / 601K in J/K =
0.612312812 J / K
1.4580763 J / K + 0.612312812 J / K = 2.07038911 J / K
ΔS≈2.1J/K
Heating:
dS₁ = dQ₁/T
dQ₁ = cmdT
dS₁ = cmdT/T = cmd(lnT)
ΔS₁ = ∫cmd(lnT) = cm∫d(lnT) = cm(lnT₂-lnT₁) = cm ln(T₂/T₁)
ΔS₁ = cm ln(T₂/T₁)
Melting:
dS₂ = dQ₂/T₂
ΔS₂ = ΔQ₂/T₂ = Lm/T₂
ΔS = ΔS₁+ΔS₂ = cm ln(T₂/T₁)+Lm/T₂
A 16-gram lead bullet slams into a concrete wall and melts on impact. If the temperature of the speeding bullet was 25°C and if the specific heat of lead is 0.13 kJ/(kgK) and its latent heat of fusion is 23 kJ/kg, what is the change in entropy of the bullet during this process? The melting point of lead is 601K.
m=16g
T₁=25°C=25°+273.15=298.15K
T₂=601K
c=0.13 kJ/(kgK)
L=23 kJ/kg
ΔS=cm ln(T₂/T₁)+Lm/T₂
Calculation by Google calculator:
0.13kJ/(kg*K) * 16g * ln(601 / 298.15) in J/K =
1.4580763 J / K
23kJ/kg * 16g / 601K in J/K =
0.612312812 J / K
1.4580763 J / K + 0.612312812 J / K = 2.07038911 J / K
ΔS≈2.1J/K
Wednesday, May 11, 2016
What is the diameter of the top section, d?
In the figure, water flows in the pipe as shown. What is the diameter of the top section, d?
d₁=5cm
v=4m/s
P=100kPa
P₂=31.5kPa
h=1.5m
d=?
vA=v₂A₂
vd₁²=v₂d²
v₂=vd₁²/d²
P+½ρv²=P₂+½ρv₂²+rgh
P+½ρv²=P₂+½ρ(vd₁²/d²)²+ρgh
P-P₂-ρgh=½ρv²d₁⁴/d⁴-½ρv²=½ρv²(d₁⁴/d⁴-1)
(P-P₂-ρgh)/(½ρv²)=d₁⁴/d⁴-1
(P-P₂-ρgh)/(½ρv²)+1=d₁⁴/d⁴
∜{(P-P₂-ρgh)/(½ρv²)+1} = d₁/d
d/d₁=∜{1/[(P-P₂-ρgh)/(½ρv²)+1]}
d = d₁ ∜{1/[(P-P₂-ρgh)/(½ρv²)+1]}
Calculation
5cm*(1/( (100kPa-31.5kPa-1000kg/m^3*9.81m/s^2*1.5m)/(1000kg/m^3*(4m/s)^2)+1 ))^(1/4)=3.4598676 cm≈3.5cm
or
d₁⁴/d⁴-1= (P-P₂-ρgh)/(½ρv²)=
=(100kPa-31.5kPa-1000kg/m^3*9.81m/s^2*1.5m)/( 1000kg/m^3*(4m/s)^2)=
=3.3615625
d₁/d=(3.3615625+1)^(1/4)= 1.44514200657
d=d₁/∙1.44514200657= 5cm /1.44514200657=3.4598676 cm≈3.5cm
⁰¹²³⁴⁵⁶⁷⁸⁹ⁱ⁺⁻⁼⁽⁾ⁿ₀₁₂₃₄₅₆₇₈₉₊₋₌₍₎ₐₑₒₓₔ∫≈Δ¼½⅓⅔⅕⅖⅗⅘⅙⅚⅛⅜⅝⅞√∛∜⨯∙ργ
d₁=5cm
v=4m/s
P=100kPa
P₂=31.5kPa
h=1.5m
d=?
vA=v₂A₂
vd₁²=v₂d²
v₂=vd₁²/d²
P+½ρv²=P₂+½ρv₂²+rgh
P+½ρv²=P₂+½ρ(vd₁²/d²)²+ρgh
P-P₂-ρgh=½ρv²d₁⁴/d⁴-½ρv²=½ρv²(d₁⁴/d⁴-1)
(P-P₂-ρgh)/(½ρv²)=d₁⁴/d⁴-1
(P-P₂-ρgh)/(½ρv²)+1=d₁⁴/d⁴
∜{(P-P₂-ρgh)/(½ρv²)+1} = d₁/d
d/d₁=∜{1/[(P-P₂-ρgh)/(½ρv²)+1]}
d = d₁ ∜{1/[(P-P₂-ρgh)/(½ρv²)+1]}
Calculation
5cm*(1/( (100kPa-31.5kPa-1000kg/m^3*9.81m/s^2*1.5m)/(1000kg/m^3*(4m/s)^2)+1 ))^(1/4)=3.4598676 cm≈3.5cm
or
d₁⁴/d⁴-1= (P-P₂-ρgh)/(½ρv²)=
=(100kPa-31.5kPa-1000kg/m^3*9.81m/s^2*1.5m)/( 1000kg/m^3*(4m/s)^2)=
=3.3615625
d₁/d=(3.3615625+1)^(1/4)= 1.44514200657
d=d₁/∙1.44514200657= 5cm /1.44514200657=3.4598676 cm≈3.5cm
⁰¹²³⁴⁵⁶⁷⁸⁹ⁱ⁺⁻⁼⁽⁾ⁿ₀₁₂₃₄₅₆₇₈₉₊₋₌₍₎ₐₑₒₓₔ∫≈Δ¼½⅓⅔⅕⅖⅗⅘⅙⅚⅛⅜⅝⅞√∛∜⨯∙ργ
Saturday, May 7, 2016
What is the possible maximum frequency of this pendulum if the distance x can be varied?
A pendulum consists of a sphere of radius R tied to a light rod so that the center of mass of the sphere is located at a distance x from the pivot point. What is the possible maximum frequency of this pendulum if the distance x can be varied?
#Physics #problem #PhysicsProblem #PhysicalProblem #pendulum #sphere #radius #light #rod #center #mass #distance #pivot #point #maximum #frequency #lightrod #centerofmass
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Friday, May 6, 2016
Hints for Quiz 15
Formulae: v= λ f; μ=m/l; v²=Fₜ/μ; P=½μω²A²v; T=1/f; ω=2πf; v²=v₀²+2ad; d=v₀t+at²; L =½mλ, m=1,2,... (fixed at both ends); L =¼λ+½mλ m=0,1,...(fixed at one end),
v= λ f (v Wave speed, λ wavelength, f frequency)
μ=m/l (μ linear density, m mass, l cord length)
v²=Fₜ/μ (v speed of transverse waves in a cord, Fₜ tension force)
P=½μω²A²v (P power transported by transverse waves in a string, cord, rope)
v²=v₀²+2ad; d=v₀t+at² (a acceleration, d displacement, t time)
Standing waves with the wavelength λ in a string with the length L: L =½mλ, m=1,2,... (strings are fixed at both ends)
L =¼λ+½mλ, m=0,1,...(strings are fixed at only one end)
1. A wire of uniform linear mass density hangs from the ceiling. It takes the time t for a pulse to travel the length of the wire. How long is the wire?
Use: μ=m/l; F=mg; v²=v₀²+2ad; d=v₀t+at²
2. A stretched string with a mass m and a length l is placed under a tension F. How much power must be supplied to the string to generate traveling waves that have a frequency f and an amplitude A?
Use: μ=m/l; v²=Fₜ/μ; P=½μω²A²v; v= λ f.
3. A string of mass m and length l can carry a wave with the power P. The amplitude of the wave is A. What is the period of oscillation if the tension applied to the string is F?
Use: μ=m/l; v²=Fₜ/μ; P=½μω²A²v; T=1/f; v= λ f.
4. A string of mass m and length l can carry a wave with the power P. When a tension of F is applied to the string it oscillates with a period T. What is the amplitude of the wave?
Use: μ=m/l; v²=Fₜ/μ; P=½μω²A²v; T=1/f.
5. In the figure, point A is below the ceiling on the distance h. Determine how much longer it will take for a pulse to travel along wire 1 than it would along wire 2. Both wires are made of the same material and have identical cross sections.
Use: μ=m/l, v²=Fₜ/μ; F=mg.
6. A guitar string with a mass m and a length l is attached to a guitar at two points separated by the distance x. What tension must the guitar string have so that its fundamental note is f?
Use L =½mλ, m=1,2,...; v= λ f; μ=m/l; v²=Fₜ/μ;
7. Two adjacent frequencies of transverse standing waves on a string held fixed at both ends are f1 and f2. What is the fundamental frequency of the transverse standing waves on this string?
Use: L =½mλ, m=1,2,...;
8. A wave of amplitude A, wavelength λ, and frequency f. What is its speed?
Use: v= λ f
⁰¹²³⁴⁵⁶⁷⁸⁹ⁱ⁺⁻⁼⁽⁾ⁿ₀₁₂₃₄₅₆₇₈₉₊₋₌₍₎ₐₑₒₓₔₕₖₗₘₙₚₛₜ∫≈Δ¼½⅓⅔⅕⅖⅗⅘⅙⅚⅛⅜⅝⅞√∛∜⨯∙ργ
v= λ f (v Wave speed, λ wavelength, f frequency)
μ=m/l (μ linear density, m mass, l cord length)
v²=Fₜ/μ (v speed of transverse waves in a cord, Fₜ tension force)
P=½μω²A²v (P power transported by transverse waves in a string, cord, rope)
v²=v₀²+2ad; d=v₀t+at² (a acceleration, d displacement, t time)
Standing waves with the wavelength λ in a string with the length L: L =½mλ, m=1,2,... (strings are fixed at both ends)
L =¼λ+½mλ, m=0,1,...(strings are fixed at only one end)
1. A wire of uniform linear mass density hangs from the ceiling. It takes the time t for a pulse to travel the length of the wire. How long is the wire?
Use: μ=m/l; F=mg; v²=v₀²+2ad; d=v₀t+at²
2. A stretched string with a mass m and a length l is placed under a tension F. How much power must be supplied to the string to generate traveling waves that have a frequency f and an amplitude A?
Use: μ=m/l; v²=Fₜ/μ; P=½μω²A²v; v= λ f.
3. A string of mass m and length l can carry a wave with the power P. The amplitude of the wave is A. What is the period of oscillation if the tension applied to the string is F?
Use: μ=m/l; v²=Fₜ/μ; P=½μω²A²v; T=1/f; v= λ f.
4. A string of mass m and length l can carry a wave with the power P. When a tension of F is applied to the string it oscillates with a period T. What is the amplitude of the wave?
Use: μ=m/l; v²=Fₜ/μ; P=½μω²A²v; T=1/f.
5. In the figure, point A is below the ceiling on the distance h. Determine how much longer it will take for a pulse to travel along wire 1 than it would along wire 2. Both wires are made of the same material and have identical cross sections.
Use: μ=m/l, v²=Fₜ/μ; F=mg.
6. A guitar string with a mass m and a length l is attached to a guitar at two points separated by the distance x. What tension must the guitar string have so that its fundamental note is f?
Use L =½mλ, m=1,2,...; v= λ f; μ=m/l; v²=Fₜ/μ;
7. Two adjacent frequencies of transverse standing waves on a string held fixed at both ends are f1 and f2. What is the fundamental frequency of the transverse standing waves on this string?
Use: L =½mλ, m=1,2,...;
8. A wave of amplitude A, wavelength λ, and frequency f. What is its speed?
Use: v= λ f
⁰¹²³⁴⁵⁶⁷⁸⁹ⁱ⁺⁻⁼⁽⁾ⁿ₀₁₂₃₄₅₆₇₈₉₊₋₌₍₎ₐₑₒₓₔₕₖₗₘₙₚₛₜ∫≈Δ¼½⅓⅔⅕⅖⅗⅘⅙⅚⅛⅜⅝⅞√∛∜⨯∙ργ
Thursday, May 5, 2016
Wednesday, May 4, 2016
What is the magnitude of the normal force N the support exerts on the object?
The 2-dimensional object of art shown in the figure is held in display at a museum by support S and rope R. Support S is on the floor and rope R is attached to the ceiling. The coefficient of static friction between the object and support S is 0.5. If the angle, θ has its maximum value such that the object remains in static equilibrium on the support, what is the magnitude of the normal force N the support exerts on the object? The object's mass is 25 kg and the distances from object's center of mass, CM, to its contact points with the support and the rope are s = 35 cm and r = 55 cm, respectively.
μ=0.5; m=25kg; s=35cm; r=55cm
fₛ≤μN
fₛ=μN (maximum)
fₛ=Tsinθ
N+Tcosθ=mg
N∙s∙sin30°+fₛ∙s∙cos30°=rTcosθ
N∙s∙sin30°+μN∙s∙cos30°=r(mg-N)
N∙s∙sin30°+μN∙s∙cos30°=rmg-rN
N∙s∙sin30°+μN∙s∙cos30°+rN=rmg
N∙(s∙sin30°+μ∙s∙cos30°+r)=rmg
N∙=rmg/(s∙sin30°+μ∙s∙cos30°+r)
Calculation: 55*25*9.81/(35*sin(30degree)+0.5*35*cos(30degree)+55cm)=153.88376691
N=154 N
μ=0.5; m=25kg; s=35cm; r=55cm
fₛ≤μN
fₛ=μN (maximum)
fₛ=Tsinθ
N+Tcosθ=mg
N∙s∙sin30°+fₛ∙s∙cos30°=rTcosθ
N∙s∙sin30°+μN∙s∙cos30°=r(mg-N)
N∙s∙sin30°+μN∙s∙cos30°=rmg-rN
N∙s∙sin30°+μN∙s∙cos30°+rN=rmg
N∙(s∙sin30°+μ∙s∙cos30°+r)=rmg
N∙=rmg/(s∙sin30°+μ∙s∙cos30°+r)
Calculation: 55*25*9.81/(35*sin(30degree)+0.5*35*cos(30degree)+55cm)=153.88376691
N=154 N
What is the length of vector A-B?
Vector A points along the y-axis with length 5.0, vector B makes an angle of 55° with respect to the x-axis and has a length of 7.0. What is the length of vector A-B?
Solution:
Aₓ=0
Ay=5
Bₓ=7cos55°
By=7sin55°
(A-B)ₓ=-7cos55°
(A-B)y=5-7sin55°
|(A-B)| = √{(-7cos55°)²+(5-7sin55°)²}
Calculation in Google calculator
sqrt((7*cos(55degree))^2+(5-7*sin(55degrees))^2)=4.0815875465
|(A-B)|≈4.1
Solution:
Aₓ=0
Ay=5
Bₓ=7cos55°
By=7sin55°
(A-B)ₓ=-7cos55°
(A-B)y=5-7sin55°
|(A-B)| = √{(-7cos55°)²+(5-7sin55°)²}
Calculation in Google calculator
sqrt((7*cos(55degree))^2+(5-7*sin(55degrees))^2)=4.0815875465
|(A-B)|≈4.1
Trigonometrical Solution:
In trigonometry, the law of cosines (also known as the cosine formula or cosine rule) relates the lengths of the sides of a triangle to the cosine of one of its angles. The law of cosines states
c² = a² + b² - 2ab∙cos γ
where γ denotes the angle contained between sides of lengths a and b and opposite the side of length c.
The vector (A-B) geometrically looks as the third side of the triangle built by two vectors A and B.
|(A-B)|=√{A+B-2|A||B|cos(γ)},
where |A|=5, |B|=7, γ is the angle between vector, γ=90°-55°=35
Calculation:
sqrt(7^2+5^2-2*7*5*cos(35degree))=4.0815875465
|(A-B)|≈4.1
In trigonometry, the law of cosines (also known as the cosine formula or cosine rule) relates the lengths of the sides of a triangle to the cosine of one of its angles. The law of cosines states
c² = a² + b² - 2ab∙cos γ
where γ denotes the angle contained between sides of lengths a and b and opposite the side of length c.
The vector (A-B) geometrically looks as the third side of the triangle built by two vectors A and B.
|(A-B)|=√{A+B-2|A||B|cos(γ)},
where |A|=5, |B|=7, γ is the angle between vector, γ=90°-55°=35
Calculation:
sqrt(7^2+5^2-2*7*5*cos(35degree))=4.0815875465
|(A-B)|≈4.1
#физика #Physics #exam #экзамен #подготовка #preporation #FinalExam#examenation #ИтоговыйЭкзамен #задачи #problems #PhysicsProblem#PhysicalProblems #ЗадачиПоФизике
⁰¹²³⁴⁵⁶⁷⁸⁹ⁱ⁺⁻⁼⁽⁾ⁿ₀₁₂₃₄₅₆₇₈₉₊₋₌₍₎ₐₑₒₓₔₕₖₗₘₙₚₛₜ∫≈Δ¼½⅓⅔⅕⅖⅗⅘⅙⅚⅛⅜⅝⅞√∛∜⨯∙ργ
⁰¹²³⁴⁵⁶⁷⁸⁹ⁱ⁺⁻⁼⁽⁾ⁿ₀₁₂₃₄₅₆₇₈₉₊₋₌₍₎ₐₑₒₓₔₕₖₗₘₙₚₛₜ∫≈Δ¼½⅓⅔⅕⅖⅗⅘⅙⅚⅛⅜⅝⅞√∛∜⨯∙ργ
Monday, May 2, 2016
Sunday, May 1, 2016
An object is launched up a 30-degree slope at an angle of 20 degrees above the incline of the slope and lands a distance L= 3.12 m up the slope. What is the object's initial speed?
An object is launched up a 30-degree slope at an angle of 20 degrees above the incline of the slope and lands a distance L= 3.12 m up the slope. What is the object's initial speed?
ϴ₁=30°
ϴ₂=20°
L= 3.12 m
v₀=?
v₀ cos(ϴ₁+ϴ₂) ∙t =L∙cos(ϴ₁)
v₀ sin(ϴ₁+ϴ₂) ∙t - ½gt² = L∙sin(ϴ₁)
t ={L∙cos(ϴ₁) / (v₀ cos(ϴ₁+ϴ₂))}
v₀ sin(ϴ₁+ϴ₂) ∙{L∙cos(ϴ₁) / (v₀ cos(ϴ₁+ϴ₂))} - ½g{L∙cos(ϴ₁) / (v₀ cos(ϴ₁+ϴ₂))}² = L∙sin(ϴ₁)
sin(ϴ₁+ϴ₂) ∙L∙cos(ϴ₁) / cos(ϴ₁+ϴ₂) - ½gL²∙cos²(ϴ₁) / (v₀² cos²(ϴ₁+ϴ₂)) = L∙sin(ϴ₁)
sin(ϴ₁+ϴ₂) ∙cos(ϴ₁) / cos(ϴ₁+ϴ₂) - ½gL∙cos²(ϴ₁) / (v₀² cos²(ϴ₁+ϴ₂)) = sin(ϴ₁)
½gL∙cos²(ϴ₁) / (v₀² cos²(ϴ₁+ϴ₂))=sin(ϴ₁+ϴ₂) ∙cos(ϴ₁)/cos(ϴ₁+ϴ₂)-sin(ϴ₁)
½gL∙cos²(ϴ₁) / (v₀² cos²(ϴ₁+ϴ₂))=
=(sin(ϴ₁+ϴ₂) ∙cos(ϴ₁) -cos(ϴ₁+ϴ₂)∙sin(ϴ₁))/cos(ϴ₁+ϴ₂)= sin(ϴ₂)/cos(ϴ₁+ϴ₂)
½gL∙cos²(ϴ₁) / (v₀² cos²(ϴ₁+ϴ₂))=sin(ϴ₂)/cos(ϴ₁+ϴ₂)
v₀² cos²(ϴ₁+ϴ₂) / (½gL∙cos²(ϴ₁)) = cos(ϴ₁+ϴ₂)/sin(ϴ₂)
v₀² / cos²(ϴ₁) = gL/(2sin(ϴ₂)cos(ϴ₁+ϴ₂))
v₀/cos(ϴ₁) = √{gL/(2sin(ϴ₂)cos(ϴ₁+ϴ₂))}
v₀ = cos(ϴ₁)√{gL/(2sin(ϴ₂)cos(ϴ₁+ϴ₂))}
Calculation:
cos(30deg)*sqrt(9.81m/s^2*3.12m/(2*sin(20deg)*cos(30deg+20deg)))=
=7.22549898 m/s
v₀ ≈ 7.23 m/s
°⁰¹²³⁴⁵⁶⁷⁸⁹ⁱ⁺⁻⁼⁽⁾ⁿ₀₁₂₃₄₅₆₇₈₉₊₋₌₍₎ₐₑₒₓₔₕₖₗₘₙₚₛₜ∫≈Δ¼½⅓⅔⅕⅖⅗⅘⅙⅚⅛⅜⅝⅞√∛∜⨯∙ρϴ
ϴ₁=30°
ϴ₂=20°
L= 3.12 m
v₀=?
v₀ cos(ϴ₁+ϴ₂) ∙t =L∙cos(ϴ₁)
v₀ sin(ϴ₁+ϴ₂) ∙t - ½gt² = L∙sin(ϴ₁)
t ={L∙cos(ϴ₁) / (v₀ cos(ϴ₁+ϴ₂))}
v₀ sin(ϴ₁+ϴ₂) ∙{L∙cos(ϴ₁) / (v₀ cos(ϴ₁+ϴ₂))} - ½g{L∙cos(ϴ₁) / (v₀ cos(ϴ₁+ϴ₂))}² = L∙sin(ϴ₁)
sin(ϴ₁+ϴ₂) ∙L∙cos(ϴ₁) / cos(ϴ₁+ϴ₂) - ½gL²∙cos²(ϴ₁) / (v₀² cos²(ϴ₁+ϴ₂)) = L∙sin(ϴ₁)
sin(ϴ₁+ϴ₂) ∙cos(ϴ₁) / cos(ϴ₁+ϴ₂) - ½gL∙cos²(ϴ₁) / (v₀² cos²(ϴ₁+ϴ₂)) = sin(ϴ₁)
½gL∙cos²(ϴ₁) / (v₀² cos²(ϴ₁+ϴ₂))=sin(ϴ₁+ϴ₂) ∙cos(ϴ₁)/cos(ϴ₁+ϴ₂)-sin(ϴ₁)
½gL∙cos²(ϴ₁) / (v₀² cos²(ϴ₁+ϴ₂))=
=(sin(ϴ₁+ϴ₂) ∙cos(ϴ₁) -cos(ϴ₁+ϴ₂)∙sin(ϴ₁))/cos(ϴ₁+ϴ₂)= sin(ϴ₂)/cos(ϴ₁+ϴ₂)
½gL∙cos²(ϴ₁) / (v₀² cos²(ϴ₁+ϴ₂))=sin(ϴ₂)/cos(ϴ₁+ϴ₂)
v₀² cos²(ϴ₁+ϴ₂) / (½gL∙cos²(ϴ₁)) = cos(ϴ₁+ϴ₂)/sin(ϴ₂)
v₀² / cos²(ϴ₁) = gL/(2sin(ϴ₂)cos(ϴ₁+ϴ₂))
v₀/cos(ϴ₁) = √{gL/(2sin(ϴ₂)cos(ϴ₁+ϴ₂))}
v₀ = cos(ϴ₁)√{gL/(2sin(ϴ₂)cos(ϴ₁+ϴ₂))}
Calculation:
cos(30deg)*sqrt(9.81m/s^2*3.12m/(2*sin(20deg)*cos(30deg+20deg)))=
=7.22549898 m/s
v₀ ≈ 7.23 m/s
°⁰¹²³⁴⁵⁶⁷⁸⁹ⁱ⁺⁻⁼⁽⁾ⁿ₀₁₂₃₄₅₆₇₈₉₊₋₌₍₎ₐₑₒₓₔₕₖₗₘₙₚₛₜ∫≈Δ¼½⅓⅔⅕⅖⅗⅘⅙⅚⅛⅜⅝⅞√∛∜⨯∙ρϴ
Thursday, April 28, 2016
The figure shows the position of a car (black circles) at one-second intervals. What is the acceleration at the time T = 4 s?
The figure shows the position of a car (black circles) at one-second intervals. What is the acceleration at the time T = 4 s?
Solution:
t=T-1s
x=v₀t+at²/2
40m=v₀∙4s+a∙(4s)²/2
13m=v₀∙1s+a∙(1s)²/2=(v₀+a∙1s/2)∙1s
v₀=13m/s-a∙1s/2
40m=(13m/s-a∙1s/2)∙4s+a∙(4s)²/2 = 52m-2s²∙a+8s²∙a = 52m+6s²∙a
6s²∙a=-12m
a=-2m/s²
⁰¹²³⁴⁵⁶⁷⁸⁹ⁱ⁺⁻⁼⁽⁾ⁿ₀₁₂₃₄₅₆₇₈₉₊₋₌₍₎ₐₑₒₓₔₕₖₗₘₙₚₛₜ∫≈Δ¼½⅓⅔⅕⅖⅗⅘⅙⅚⅛⅜⅝⅞√∛∜⨯∙
Solution:
t=T-1s
x=v₀t+at²/2
40m=v₀∙4s+a∙(4s)²/2
13m=v₀∙1s+a∙(1s)²/2=(v₀+a∙1s/2)∙1s
v₀=13m/s-a∙1s/2
40m=(13m/s-a∙1s/2)∙4s+a∙(4s)²/2 = 52m-2s²∙a+8s²∙a = 52m+6s²∙a
6s²∙a=-12m
a=-2m/s²
⁰¹²³⁴⁵⁶⁷⁸⁹ⁱ⁺⁻⁼⁽⁾ⁿ₀₁₂₃₄₅₆₇₈₉₊₋₌₍₎ₐₑₒₓₔₕₖₗₘₙₚₛₜ∫≈Δ¼½⅓⅔⅕⅖⅗⅘⅙⅚⅛⅜⅝⅞√∛∜⨯∙
The potential energy of a mass m=10kg is given by U=-3.98 × 10¹⁵Jm⋅ r⁻¹
The potential energy of a mass m=10kg is given by
U=-3.98 × 10¹⁵Jm⋅ r⁻¹ (potential energy decreases as r approaches zero). The force on this mass when it is located at r=6.38 × 10⁶ m is _________
Solution:
F = -dU/dr=
= -d( -3.98 × 10¹⁵⋅ r⁻¹)/dr=
= 3.98 × 10⁻¹⁵⋅ d(r⁻¹)/dr =
= -3.98 × 10⁻¹⁵⋅ r⁻² =
= -3.98 × 10¹⁵/ (6.38 × 10⁶)²
Calculation on the Google Calculator: -3.98E15/ (6.38E6)^2=-97.7781271804
|F|=97.8N, the direction is toward the origin (r=0).
⁰¹²³⁴⁵⁶⁷⁸⁹ⁱ⁺⁻⁼⁽⁾ⁿ₀₁₂₃₄₅₆₇₈₉₊₋₌₍₎ₐₑₒₓₔₕₖₗₘₙₚₛₜ∫≈Δ¼½⅓⅔⅕⅖⅗⅘⅙⅚⅛⅜⅝⅞
Solution:
F = -dU/dr=
= -d( -3.98 × 10¹⁵⋅ r⁻¹)/dr=
= 3.98 × 10⁻¹⁵⋅ d(r⁻¹)/dr =
= -3.98 × 10⁻¹⁵⋅ r⁻² =
= -3.98 × 10¹⁵/ (6.38 × 10⁶)²
Calculation on the Google Calculator: -3.98E15/ (6.38E6)^2=-97.7781271804
|F|=97.8N, the direction is toward the origin (r=0).
⁰¹²³⁴⁵⁶⁷⁸⁹ⁱ⁺⁻⁼⁽⁾ⁿ₀₁₂₃₄₅₆₇₈₉₊₋₌₍₎ₐₑₒₓₔₕₖₗₘₙₚₛₜ∫≈Δ¼½⅓⅔⅕⅖⅗⅘⅙⅚⅛⅜⅝⅞
A rocket, speeding along toward Alpha Centauri, has an acceleration a(t) = At².
A rocket, speeding along toward Alpha Centauri, has an acceleration
a(t) = At².
Assume that the rocket began at rest at the Earth (x = 0) at t = 0. Assuming it simply travels in a straight line from Earth to Alpha Centauri (and beyond), what is the ratio of the speed of the rocket when it has covered half the distance to the star to its speed when it has travelled half the time necessary to reach Alpha Centauri?
Solution:
T - total time necessary to reach Alpha Centauri
D - distance to the star
v - speed
v₁=v(D/2)
v₂=v(T/2)
v(t)=∫At²dt=⅓At³
x(t)=∫v(t)dt=⅓At³dt=⅓¼At⁴
D=AT⁴/12
D/2=AT⁴/24
D/2=At⁴/12; At⁴/12=AT⁴/24; t⁴=T⁴/2; t⁴/T⁴=½; t/T=∜½
v₁/v₂ = v(t)/v(T/2) = {⅓At³} / {⅓A(T/2)³}
=t³ / (T/2)³ =2³ (t/T)³ = 2³ ⨯ (∜½)³ = (2∜½)³ = (∜16⨯∜½)³ = (∜8)³=4∜2
This result is not among the proposed answers to choose from. Check again algebraic transformations.
⁰¹²³⁴⁵⁶⁷⁸⁹ⁱ⁺⁻⁼⁽⁾ⁿ₀₁₂₃₄₅₆₇₈₉₊₋₌₍₎ₐₑₒₓₔₕₖₗₘₙₚₛₜ∫≈Δ¼½⅓⅔⅕⅖⅗⅘⅙⅚⅛⅜⅝⅞√∛∜⨯∙
a(t) = At².
Assume that the rocket began at rest at the Earth (x = 0) at t = 0. Assuming it simply travels in a straight line from Earth to Alpha Centauri (and beyond), what is the ratio of the speed of the rocket when it has covered half the distance to the star to its speed when it has travelled half the time necessary to reach Alpha Centauri?
Solution:
T - total time necessary to reach Alpha Centauri
D - distance to the star
v - speed
v₁=v(D/2)
v₂=v(T/2)
v(t)=∫At²dt=⅓At³
x(t)=∫v(t)dt=⅓At³dt=⅓¼At⁴
D=AT⁴/12
D/2=AT⁴/24
D/2=At⁴/12; At⁴/12=AT⁴/24; t⁴=T⁴/2; t⁴/T⁴=½; t/T=∜½
v₁/v₂ = v(t)/v(T/2) = {⅓At³} / {⅓A(T/2)³}
=t³ / (T/2)³ =2³ (t/T)³ = 2³ ⨯ (∜½)³ = (2∜½)³ = (∜16⨯∜½)³ = (∜8)³=4∜2
This result is not among the proposed answers to choose from. Check again algebraic transformations.
⁰¹²³⁴⁵⁶⁷⁸⁹ⁱ⁺⁻⁼⁽⁾ⁿ₀₁₂₃₄₅₆₇₈₉₊₋₌₍₎ₐₑₒₓₔₕₖₗₘₙₚₛₜ∫≈Δ¼½⅓⅔⅕⅖⅗⅘⅙⅚⅛⅜⅝⅞√∛∜⨯∙
Wednesday, April 27, 2016
What is the location of the center of mass of the rod?
A long, thin rod lies along the x-axis.
One end of the rod is located at x = 2.00 m and the other end of the rod is located at x = 6.00 m.
The linear mass density of the rod is given by ax³+b ,
where a = 0.100 kg/m⁴ and b = 0.200 kg/m.
What is the location of the center of mass of the rod?
xₘ={∫x(ax³+b)dx}/{∫(ax³+b)dx}={∫(ax⁴+bx)dx}/{∫(ax³+b)dx}=
=(⅕a(x₂⁵-x₁⁵)+½b(x₂²-x₁²)) / (¼a(x₂⁴-x₁⁴)+b(x₂-x₁))=
={(⅕0.1(6⁵-2⁵)+½0.2(6²-2²))}/{(¼0.1(6⁴-2⁴)+0.2(6-2))}
Calculation:
(0.1*(6^5-2^5)/5+0.2*(6^2-2^2)/2)/(0.1*(6^4-2^4)/4+0.2(6-2))
=4.81951219512
xₘ≈4.82
⁰¹²³⁴⁵⁶⁷⁸⁹ⁱ⁺⁻⁼⁽⁾ⁿ₀₁₂₃₄₅₆₇₈₉₊₋₌₍₎ₐₑₒₓₔₕₖₗₘₙₚₛₜ∫≈Δ¼½⅓⅔⅕⅖⅗⅘⅙⅚⅛⅜⅝⅞
One end of the rod is located at x = 2.00 m and the other end of the rod is located at x = 6.00 m.
The linear mass density of the rod is given by ax³+b ,
where a = 0.100 kg/m⁴ and b = 0.200 kg/m.
What is the location of the center of mass of the rod?
xₘ={∫x(ax³+b)dx}/{∫(ax³+b)dx}={∫(ax⁴+bx)dx}/{∫(ax³+b)dx}=
=(⅕a(x₂⁵-x₁⁵)+½b(x₂²-x₁²)) / (¼a(x₂⁴-x₁⁴)+b(x₂-x₁))=
={(⅕0.1(6⁵-2⁵)+½0.2(6²-2²))}/{(¼0.1(6⁴-2⁴)+0.2(6-2))}
Calculation:
(0.1*(6^5-2^5)/5+0.2*(6^2-2^2)/2)/(0.1*(6^4-2^4)/4+0.2(6-2))
=4.81951219512
xₘ≈4.82
⁰¹²³⁴⁵⁶⁷⁸⁹ⁱ⁺⁻⁼⁽⁾ⁿ₀₁₂₃₄₅₆₇₈₉₊₋₌₍₎ₐₑₒₓₔₕₖₗₘₙₚₛₜ∫≈Δ¼½⅓⅔⅕⅖⅗⅘⅙⅚⅛⅜⅝⅞
Tuesday, April 26, 2016
What is the distance of the resulting plate's center of mass from the origin?
A thin rectangular plate of uniform density σ₁ = 5.94 kg/m² has a length a = 0.740 m and a width of b = 0.330 m. The lower left hand corner is placed at the origin, (x, y) = (0, 0). A circular hole is cut in the plate of radius r = 0.064 m with center at (x, y) = (0.084 m, 0.084 m) and replaced with a circular disk with the same radius composed of another material of the same thickness with uniform density σ₂ = 1.67 kg/m². What is the distance of the resulting plate's center of mass from the origin? (in m)
xₘ=(σ₁ab a/2+πr²(σ₂-σ₁) x) / (σ₁ab a/2+πr²(σ₂-σ₁) x)
yₘ=(σ₁ab a/2+πr²(σ₂-σ₁) y) / (σ₁ab a/2+πr²(σ₂-σ₁) y)
d²=xₘ²+yₘ²
xₘ=(5.94*0.74*0.33*0.74/2 + (pi)*0.064^2*(1.67-5.94)*0.084)/(5.94*0.74*0.33+ (pi)*0.064^2*(1.67-5.94))=0.381260099
yₘ=(5.94*0.74*0.33*0.33/2 + (pi)*0.064^2*(1.67-5.94)*0.084)/(5.94*0.74*0.33+ (pi)*0.064^2*(1.67-5.94))=0.381260099=0.16818904902
d=sqrt(0.381260099^2+0.16818904902^2)=0.41670951429≈0.417 (m)
yₘ=(σ₁ab a/2+πr²(σ₂-σ₁) y) / (σ₁ab a/2+πr²(σ₂-σ₁) y)
d²=xₘ²+yₘ²
xₘ=(5.94*0.74*0.33*0.74/2 + (pi)*0.064^2*(1.67-5.94)*0.084)/(5.94*0.74*0.33+ (pi)*0.064^2*(1.67-5.94))=0.381260099
yₘ=(5.94*0.74*0.33*0.33/2 + (pi)*0.064^2*(1.67-5.94)*0.084)/(5.94*0.74*0.33+ (pi)*0.064^2*(1.67-5.94))=0.381260099=0.16818904902
d=sqrt(0.381260099^2+0.16818904902^2)=0.41670951429≈0.417 (m)
⁰¹²³⁴⁵⁶⁷⁸⁹ⁱ⁺⁻⁼⁽⁾ⁿ₀₁₂₃₄₅₆₇₈₉₊₋₌₍₎ₐₑₒₓₔₕₖₗₘₙₚₛₜ
#Physics #problem #PhysicsProblem #PhysicalProblem #problems#PhysicsProblems #PhysicalProblems
#Physics #problem #PhysicsProblem #PhysicalProblem #problems#PhysicsProblems #PhysicalProblems
Center of Mass
Find the y-coordinate of the center of mass of a 10-cm square plate whose density (in kg/m³) is ρ = 4.22⋅10⁴kg/m⁶⋅xy². The lower left-hand side of the plate is at the origin and the upper right-hand corner is at (10 cm, 10 cm). The plate is 0.30 cm thick.
(∫y⋅y²dy) / (∫y²dy) = ¾y = ¾⋅10cm = 7.5cm
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