A chimpanzee is standing not too far from a tall cliff. He lets out a loud bark and is startled to hear an echo from the cliff 0.830 seconds later. How far away is the cliff? Take the speed of sound to be 331 m/s.

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ISBN:9781938168277
Author:William Moebs, Samuel J. Ling, Jeff Sanny
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Chapter14: Fluid Mechanics
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A chimpanzee is standing not too far from a tall cliff. He lets out a loud bark and is startled to hear an echo from the cliff 0.830 seconds later. How far away is the cliff? Take the speed of sound to be 331 m/s.

 

Area of circle: A = Tr?
Rate of flow
Q = Av
t = F(sin0)r
T = Fl, wherel= lever arm
Bernoulli's equation:
1
P+
+ pgy, = P, +
1
pv,´ + pgy,
Equilibrium:
Te = T - 273.15°C
Στ=0
9
T =
-T. +32
5
Non-equilibrium:
5
Tc =-(T, - 32)
Στ= Ια
Тетреrature:
Moment of inertial for a point mass
revolving about a center at a distance r:
ΔL L,ΔΤ
AA = y A,AT Y = 2a
AV = BVAT B = 3a
I= Mr?
Kinetic Energy:
Specific Heat:
Translational: ½ mv²
Rotational: ½ Im?
(J/kg. 'C)
mAT
Q = mc(T, –T,)
Angular speed o =v/r
Qcold
=-Qhot
Tensile strain:
EQ = 0
Latent Heat:
F
AL
L.
Y -Young's modulus
phase change: Q=±mL
Energy Transfer:
ΔΤ
P =
At
Density:
Ar
M
p =
V
(kg/m²)
Thermal conductivity:
Pressure:
(T, – T.)
P = kA
L.
F
P=
A
(Ра)
Hooke's Law:
F =-kx
P = P, + pgh
Acceleration in simple harmonic
motion:
Archimedes' principle:
k
a =
B = P fuidV fa
m
fluid8
Elastic potential energy:
РЕ, %3D
-kx²
2
Equation of flow continuity:
Av, = A,v,
Period:
Transcribed Image Text:Area of circle: A = Tr? Rate of flow Q = Av t = F(sin0)r T = Fl, wherel= lever arm Bernoulli's equation: 1 P+ + pgy, = P, + 1 pv,´ + pgy, Equilibrium: Te = T - 273.15°C Στ=0 9 T = -T. +32 5 Non-equilibrium: 5 Tc =-(T, - 32) Στ= Ια Тетреrature: Moment of inertial for a point mass revolving about a center at a distance r: ΔL L,ΔΤ AA = y A,AT Y = 2a AV = BVAT B = 3a I= Mr? Kinetic Energy: Specific Heat: Translational: ½ mv² Rotational: ½ Im? (J/kg. 'C) mAT Q = mc(T, –T,) Angular speed o =v/r Qcold =-Qhot Tensile strain: EQ = 0 Latent Heat: F AL L. Y -Young's modulus phase change: Q=±mL Energy Transfer: ΔΤ P = At Density: Ar M p = V (kg/m²) Thermal conductivity: Pressure: (T, – T.) P = kA L. F P= A (Ра) Hooke's Law: F =-kx P = P, + pgh Acceleration in simple harmonic motion: Archimedes' principle: k a = B = P fuidV fa m fluid8 Elastic potential energy: РЕ, %3D -kx² 2 Equation of flow continuity: Av, = A,v, Period:
Intensity level:
m
T = 2n,
k
B=10log
I.
Frequency:
f =
T
Intensity level difference:
Angular frequency:
k
w = 2n f
AB =10log
I,
m
PV = nRT, where R = 8.31 J/mole-K
Maximum Velocity, Acceleration:
A2n f
Ao = A(2nf}
Umax = A@ =
a max =
PV = constant,
PIV1 = P2V2
A = (27 f)
а max
Intensity:
Simple pendulum:
I= Pav
4ar?
T= 2n=
Doppler Shift:
Moving observer: f' = f(v+vo)/v
Speed sound temperature:
Moving source: f' = f(v)/ ( v-vs)
v= f2
Where vo = velocity of observer, vs is the
speed of the source, and v is the
speed of sound
T
U = (331m/s),
273K
Intensity of a wave:
power
Beat frequency fB
\f2- fil
I=
%3D
area
A
bol
Transcribed Image Text:Intensity level: m T = 2n, k B=10log I. Frequency: f = T Intensity level difference: Angular frequency: k w = 2n f AB =10log I, m PV = nRT, where R = 8.31 J/mole-K Maximum Velocity, Acceleration: A2n f Ao = A(2nf} Umax = A@ = a max = PV = constant, PIV1 = P2V2 A = (27 f) а max Intensity: Simple pendulum: I= Pav 4ar? T= 2n= Doppler Shift: Moving observer: f' = f(v+vo)/v Speed sound temperature: Moving source: f' = f(v)/ ( v-vs) v= f2 Where vo = velocity of observer, vs is the speed of the source, and v is the speed of sound T U = (331m/s), 273K Intensity of a wave: power Beat frequency fB \f2- fil I= %3D area A bol
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