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That's what I want to know.
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The physical formula and derivation formula are as follows:
The movement of the particle - the linear motion grip elimination.
Average velocity v-flat = s t (defined) 2Useful inference vt 2 v0 2=2as
Intermediate moment velocity vt 2= v flat = (v t + v o) 2
Intermediate position velocity vs 2 = [(v o2 + v t2) 2] 1 2
Displacement s = v flat t = v o t + at2 2=v t 2 t
Acceleration a=(v t - v o) t is in the positive direction of v o, a is in the same direction as v o (accelerates) a>0;If it is reversed, it will be a<0
The experimental inference is that δS=at2 δs is the difference between the displacements of adjacent succession equal time (t).
Main physical quantities and units: muzzle velocity (v o): m s plus section huaizhi velocity (a): m s2 final velocity (vt): m s
The law of conservation of energy.
The gravitational and repulsive forces of the intermolecular explicit argument (1) rr=r0, f-induced = frepulsion, f-molecular=0, e-molecule potential energy = emin (minimum).
r>r0, f repulsion, f molecular force behaves as gravitational force.
r>10r0, f induction = f repulsion 0, f molecular force 0, e molecular potential energy 0
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Let the time of each time period be t, and the initial velocity of each time period v0=at is obtained according to the formula s=v0t+1 2at 2v=at
Note: t represents the time consumed from the start of the exercise to the time period consumed) s1 = 1 2at 2
s2=(at)t+1 2at 2=3 2at 2s3=(2at)t+1 2at 2=5 2at 2sn=(nat)t+1 2at 2=(2n-1) 2at 2In summary, we get s1:s2:s3:
sn=1:3:
5:…:2n-1)(n…)
We can first find that the motion displacement of the object reaches s2s3s
ns.
The initial velocity is 0s=1 2at 2
Time taken t1=t=(1-0)t
2s=1/2a(√2t)^2
Time taken t2 = 2t - t1 = ( 2 - 1)t
3s=1/2a(√3t)^2
Time taken t3 = 3t - (t1 + t2) = (3- 2) tns = 1 2a( nt) 2
Time taken tn= nt-(t1+......t2)=(n- n-1)t, we get t1:t2:t3:....:tn=(√1-0):(2-√1):(3
2):…n-√n-1)
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It's actually quite simple.
It's just not good to fight.
and the square has a root number.
So you set the distance for 2s
V1v2V3 three speeds are the start.
The last three velocities in the middle.
v2^2-v1^2=2as
v3^2-v2^2=2as
A is equal to v2 2-v1 2=v3 2-v2 2 moved over and resolved.
I got it.
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Have you ever learned.
v^2-v0^2=2ax
Ah, it's easy to have.
Set in order. v1v2
v3v2^2-v1^2=2ax
v3^2-v2^2=2ax
Because the acceleration a is constant, and the displacement between each velocity is equal, then v2 2-v1 2=v3 2-v2 2 2 shift term is obtained 2*(v2 2)=v1 2
v3^2ps:v^2-v0^2=2ax
It is derived from v=v0+at
T = (v-v0) a is brought in x=v0t+1 2*at 2, then x=v0(v-v0) a+(1 2)*a(v-v0) 2 a2 is multiplied by 2a on both sides of the equation, simplify:
2ax=2v0*v-2v0^2+v^2-2v0*v+v0^22ax=v^2-v0^2
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Let's take an example.
According to the equations s s =v t and v=at, they have a t which is a common physical quantity, and then and and . Available:
v²=2as
It is by joining the same variables that many formulas can be deduced
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、...... at the end of the first second and the end of the second secondThe ratio of velocity at the end of the nth second v1:v2:v3......:vn=1:2:3:……n。
、...... within the first 1 second and within the first 2 secondsThe ratio of displacements in the first n seconds s1:s2:s3:......sn=1:4:9……:n2。
、...... in time t and time 2tThe ratio of the displacement at the first time n is s :s defense :s ......sn=1:3:5:……2n-1)。
Through the pre-s, pre-2s, pre-3s ......, the ratio of the time required in the first ns t1:t2:......tn=1:√2:√3……:n。
Over 1s, 2s, blind loss 3s、......The ratio of the time required for the first ns t:t:t ......tn=1: grinding the god of the stove (2 1):( 3- 2) ......n-√n-1)
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、...... at the end of the first second and the end of the second secondThe ratio of velocity at the end of the nth second v1:v2:v3......:vn=1:2:3:……Judgment Swift: n.
Derivation: v1=at, v2=a*2t, v3=a*3t....vn=a*nt
、...... within the first 1 second and within the first 2 secondsThe ratio of displacements in the first n seconds s1:s2:s3:......sn=1:4:9……:n2。
Derivation: s1=at*t 2 , s2=a(2t)*(2t) 2=2at*t s3=a(3t)*(3t) 2=9at*t 2
.sn=a(nt)*(nt)/2=n*nat*t/2
、...... in time t and time 2tThe ratio of the displacement in the first time nt is s:s :s ......sn=1:3:5:……2n-1)。Pin this flush search.
Derivation: From the knowable:
si=s1=at*t/2 , sii=s2-s1=3at*t/2, siii=s3-s2=5at*t/2...
sn=sn-sn_1=n*nat*t/2-(n-1)*(n-1)at*t/2 =(2n-1)at*t/2
The last three are all obtained by adding and subtracting the first three, which is very easy, so I won't say more.
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1. Uniform acceleration of the linear motion of the nuclear disturbance The continuous mass is equally displaced.
s1=s2=s3=sn From vo=o, we can see that s=s is proportional to t*t under the condition of equal acceleration.
Obtain t1 square t2 square t3 square tn square = 1 2 3 n conversion to obtain three billy formulas.
Two. Uniform acceleration or linear motion for continuous equal time.
v = at ti t2 t3 tn=1 2 3 n v is proportional to t In the same way, three other formulas can be obtained by s=at*t.
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The derivation of six proportions of uniform acceleration linear motion with a physical initial velocity of 0 is obtained.
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1.This ratio is only suitable for uniform acceleration linear motion with zero initial velocity.
According to s = , then within 1s, within 2s, within 3s 、......The displacements of ns are ,,ah, so the ratio is 1:4:9:....:n^2
2.、... in the 1st, 2nd, and 3rd sThe displacement ratio of the ns is 1:(4-1):
9-4):(16-9)……n^2 - n-1)^2] = 1:
2n-1)3.This one is the easiest. The instantaneous velocity at the end of n seconds is an, so the velocity ratio at the end of 1s, 2s, and 3s is 1:
2:3……There is also a scale, that is, from moment zero, the displacement ratio in equal time intervals is 1: (with 2 -1):
with 3 - with 2) :(with 4 - with 3): ....Heel n - Heel (n-1)).
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This is the formula for uniform acceleration motion with an initial velocity of 0.
For example, the acceleration is 1m s and the end velocity is 1m s and the displacement in one second = (end velocity 1 + initial velocity 0) multiplied by time 1 = displacement in 2 seconds = (end velocity 2 + 0) multiplied by 2 = 2m, and then push it down by yourself to help yourself.
The displacement in 1 second is the displacement in 2 seconds.
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It is conserved by mechanical energy.
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